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The incorporation of glottal source-vocal tract interaction effects to improve the naturalness of synthetic speech

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Title:
The incorporation of glottal source-vocal tract interaction effects to improve the naturalness of synthetic speech
Creator:
Wong, Chun-Fan, 1961- ( Dissertant )
Childers, Donald G. ( Thesis advisor )
Arroyo, Amauri A. ( Reviewer )
Principe, Jose C. ( Reviewer )
Couch, Leon W. ( Reviewer )
Rothman, Howard B. ( Reviewer )
Phillips, Winfred M. ( Degree grantor )
Lockhart, Madelyn M. ( Degree grantor )
Place of Publication:
Gainesville, Fla.
Publisher:
University of Florida
Publication Date:
Copyright Date:
1991
Language:
English
Physical Description:
vi, 130 leaves : ill. ; 28 cm.

Subjects

Subjects / Keywords:
Bandwidth ( jstor )
Eggs ( jstor )
Glottal consonants ( jstor )
Glottis ( jstor )
Modeling ( jstor )
Signals ( jstor )
Spoken communication ( jstor )
Vocal cords ( jstor )
Vowels ( jstor )
Waveforms ( jstor )
Dissertations, Academic -- Electrical Engineering -- UF
Electrical Engineering thesis Ph. D
Formants (Speech) -- Computer simulation ( lcsh )
Glottis -- Mathematical models ( lcsh )
Speech processing systems ( lcsh )
Speech synthesis ( lcsh )
Vocal cords -- Mathematical models ( lcsh )
Genre:
bibliography ( marcgt )
theses ( marcgt )
non-fiction ( marcgt )

Notes

Abstract:
In the conventional speech production model, voiced sounds are generated by exciting the vocal tract filter with a train of quasi-periodic glottal pulses. The glottal source and the vocal tract are assumed to be linearly separable. A fixed stylized glottal pulse shape is adopted as the source for all voided sounds. Speech synthesized with this approach can be highly intelligible, but often does not sound natural. It is believed that glottal source-vocal tract interaction, or simple source-tract interaction, is important for synthesizing natural sounding speech. The glottal source and the vocal tract interact with each other, and different glottal pulse shapes should be used for different voiced sounds. A number of source-tract interaction effects have been identified. The interaction causes the volume-velocity signal to be skewed to the right with respect to the glottal area. A ripple in the volume-velocity waveform may appear, which is thought to be caused primarily by the vocal tract first-formant frequency. The ripple is a result of glottal damping during the glottal open interval. To incorporate the source-tract interaction effects into the conventional speech production model, a variable glottal pulse model was proposed. The glottal pulse shape is defined by a few parameters, and represents the smoothed glottal volume-velocity signal. The ripple effect was approximated by increasing the first formant bandwidth of the closed-phase vocal tract filter during the glottal open interval. An analysis/synthesis system was implemented to test the performance of the proposed model. Automatic glottal inverse filtering was used to obtain the glottal volume-velocity waveform and the closed-phase vocal tract filter. A least squared error fit was performed on the glottal volume-velocity waveform to obtain the glottal source parameters. Speech synthesized with source-tract interaction sounds more natural than speech synthesized without source-tract interaction. Hence, source-tract interaction should be used to generate natural sounding speech.
Thesis:
Thesis (Ph. D.)--University of Florida, 1991.
Bibliography:
Includes bibliographical references (leaves 124-129).
General Note:
Typescript.
General Note:
Vita.
Statement of Responsibility:
by Chun-Fan Wong.

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University of Florida
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University of Florida
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Copyright [name of dissertation author]. Permission granted to the University of Florida to digitize, archive and distribute this item for non-profit research and educational purposes. Any reuse of this item in excess of fair use or other copyright exemptions requires permission of the copyright holder.
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25034730 ( OCLC )
AHZ5393 ( NOTIS )

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THE INCORPORATION OF GLOTTAL SOURCE-VOCAL TRACT INTERACTION
EFFECTS TO IMPROVE THE NATURALNESS OF SYNTHETIC SPEECH









BY

CHUN-FAN WONG


A DISSERTATION PRESENTED TO THE GRADUATE SCHOOL
OF THE UNIVERSITY OF FLORIDA IN PARTIAL FULFILLMENT
OF THE REQUIREMENTS FOR THE DEGREE OF
DOCTOR OF PHILOSOPHY

UNIVERSITY OF FLORIDA


1991












ACKNOWLEDGMENTS


I would like to thank my advisor and committee

chairman, Dr. Donald G. Childers, for giving me the

opportunity to do research in the Mind-Machine Interaction

Research Center, for his invaluable guidance and assistance,

and for bearing with me during the course of my research. I

am also thankful for his giving me some financial

assistance.

I am also grateful to Dr. Leon W. Couch, II, for his

discussion of my research subject, and for taking the time

to serve on my committee.

I would also like to thank Dr. A. Antonio Arroyo, Dr.

Jose C. Principe, and Dr. Howard B. Rothman for their

invaluable time and interest in serving on my supervisory

committee.












TABLE OF CONTENTS



page

ACKNOWLEDGMENTS ...................................... ii

ABSTRACT ...............................................

CHAPTERS

1 INTRODUCTION ................ ..................... 1

The Structure of Speech ......................... 2
The Conventional Speech Production Model ........ 4
Speech Analysis/Synthesis ....................... 4
Introduction to Source-Tract Interaction ........ 12

2 SOURCE-TRACT INTERACTION ........................ 18

Introduction .................................... 18
Speech Production Models ....................... 18
Effects of Source-Tract Interaction ............. 24
Literature Review ............................... 34
Glottal Impedance .............................. 34
Simulation Experiments ........................ 36
Theoretical Studies ............................ 40
Summary of All Source-Tract Interaction Effects 54

3 INCORPORATION OF SOURCE-TRACT INTERACTION ....... 56

Introduction .................................... 56
Modeling Source-Tract Interaction ............... 56
Source-Tract Interaction Incorporation .......... 59
Measurement of Model Parameters ................. 59
Electroglottograph (EGG) ........................ 61
Glottal Inverse Filtering ....................... 63
Literature Review ............................. 67
Automatic Glottal Inverse Filtering .......... 73






Source Models ................................... 76

4 IMPLEMENTATION AND RESULTS ...................... 82

Introduction .................................... 82
Experimental Data Base .......................... 82
Implementation of Proposed Speech Production
Model ........................................ 84
Correction of Distorted Speech Signals .......... 89
Inverse Filtering Results ...................... 104
Modeling of Glottal Flow Waveform ............... 107

5 DISCUSSION ...................................... 115

Summary ......................................... 115
Future Research Directions ..................... 116
Further Work .................................... 118

APPENDIX ............................................. 120

REFERENCES ........................................... 124

BIOGRAPHICAL SKETCH .................................. 130













Abstract of Dissertation Presented to the Graduate School
of the University of Florida in Partial Fulfillment of the
Requirements for the Degree of Doctor of Philosophy

THE INCORPORATION OF GLOTTAL SOURCE-VOCAL TRACT INTERACTION
EFFECTS TO IMPROVE THE NATURALNESS OF SYNTHETIC SPEECH

By

Chun-Fan Wong

May, 1991


Chairman: Dr. D.G. Childers
Major Department: Electrical Engineering


In the conventional speech production model, voiced

sounds are generated by exciting the vocal tract filter with

a train of quasi-periodic glottal pulses. The glottal

source and the vocal tract are assumed to be linearly

separable. A fixed stylized glottal pulse shape is adopted

as the source for all voiced sounds. Speech synthesized

with this approach can be highly intelligible, but often

does not sound natural.

It is believed that glottal source-vocal tract

interaction, or simply source-tract interaction, is

important for synthesizing natural sounding speech. The

glottal source and the vocal tract interact with each other,

and different glottal pulse shapes should be used for

different voiced sounds.







A number of source-tract interaction effects have been

identified. The interaction causes the volume-velocity

signal to be skewed to the right with respect to the glottal

area. A ripple in the volume-velocity waveform may appear,

which is thought to be caused primarily by the vocal tract

first-formant frequency. The ripple is a result of glottal

damping during the glottal open interval.

To incorporate the source-tract interaction effects

into the conventional speech production model, a variable

glottal pulse model was proposed. The glottal pulse shape

is defined by a few parameters, and represents the smoothed

glottal volume-velocity signal. The ripple effect was

approximated by increasing the first-formant bandwidth of

the closed-phase vocal tract filter during the glottal open

interval.

An analysis/synthesis system was implemented to test

the performance of the proposed model. Automatic glottal

inverse filtering was used to obtain the glottal

volume-velocity waveform and the closed-phase vocal tract

filter. A least squared error fit was performed on the

glottal volume-velocity waveform to obtain the glottal

source parameters. Speech synthesized with source-tract

interaction sounds more natural than speech synthesized

without source-tract interaction. Hence, source-tract

interaction should be used to generate natural sounding

speech.















CHAPTER 1
INTRODUCTION


The most natural way to communicate between human

beings is speech communication, and it is a very efficient

process. With the rapid advancement of computer technology,

speech communication between human and machine is also

becoming feasible. This has the advantage of freeing our

hands and eyes to do other important tasks. Also, a higher

input rate than typing can be achieved.

Digital techniques and computer technology have opened

vast possibilities for machine assistance to humans. Not

the least of these is an immense potential for storage of

and rapid access to voluminous amounts of information.

Automatic voice readout of computer-stored data allows the

machine to meet the individual on human terms. Using voice

response, the machine can provide sophisticated information

in a form easily assimilated by the human user. Moreover,

this information can be accessed and transported to the

human user over ubiquitous telephone circuits.

Typical uses of computer voice output are automatic

information services, computer-based instruction, reading

machines for the blind, spoken status reports from aircraft

and space-vehicle systems.








At present, the intelligibility of synthetic speech

attainable from the conventional linear speech production

model is quite high, but naturalness still needs to be

improved. The research objective of this dissertation is to

improve the naturalness of the synthetic speech, using a

more accurate model of speech production that includes

source-tract interaction.


The Structure of Speech

(Rabiner and Schafer, 1978)


Speech signals are composed of a sequence of sounds.

These sounds and the transitions between them serve as a

symbolic representation of information. The arrangement of

these sounds (symbols) is governed by the rules of language.

The study of these rules and their implications in human

communication is the domain of linguistics, and the study

and classification of the sounds of speech are called

phonetics.

Speech sounds can be classified into 3 distinct

classes according to their mode of excitation. Voiced

sounds are produced by forcing air through the glottis with

the tension of the vocal folds adjusted so that they vibrate

as a relaxation oscillation, thereby producing

quasi-periodic pulses of air that excite the vocal tract.

Unvoiced sounds are generated by forming a constriction at

some point in the vocal tract (usually toward the mouth),

and forcing air through the constriction at a high enough








velocity to produce turbulence. This creates a

broad-spectrum noise source to excite the vocal tract.

Plosive sounds result from making a complete closure (again,

usually toward the front of the vocal tract), building up

pressure behind the closure, and abruptly releasing it.

Most languages, including English, can be described in

terms of a set of distinctive sounds, or phonemes. In

particular, for American English, there are about 42

phonemes including vowels, diphthongs, semivowels and

consonants. Each of the phonemes can be classified as

either a continuant, or a noncontinuant sound. Continuant

sounds are produced by a fixed (non-time-varying) vocal

tract configuration excited by the appropriate source. The

class of continuant sounds includes the vowels, the

fricatives (both unvoiced and voiced), and the nasals. The

remaining sounds are produced by a changing vocal tract

configuration. These are therefore classed as

noncontinuants.

Vowels are produced by exciting a fixed vocal tract

with quasi-periodic pulses of air caused by vibration of the

vocal folds. If the nasal tract is effectively coupled to

the vocal tract during the production of a vowel, the vowel

becomes nasalized. Each vowel sound can be characterized by

the vocal tract configuration that is used in its

production. An alternative representation is in terms of

the resonance frequencies of the vocal tract (formants).








The Conventional Speech Production Model


A linear model of speech production was developed by

Fant in the late 1950's (Fant, 1960). Its discrete-time

version is shown in Figure 1-1. The speech signal is

modeled as the output of a linear quasi-time-invariant

filter excited by quasi-periodic pulses for voiced sounds,

or by random noise for unvoiced sounds. Acoustic theory

shows that the transmission characteristics of the vocal

tract is well approximated by a cascade of uncoupled

resonators and antiresonators whose bandwidths and center

frequencies may be independently controlled.


Speech Analysis/Synthesis


Efforts in speech analysis and synthesis frequently

aim at the efficient encoding and transmission of speech

information. Another important motivation is to acquire

basic understanding of speech communication. Speech

synthesis systems also play a fundamental role in learning

about the process of human speech production.

Speech synthesis is the process of producing an

acoustic signal by controlling the model for speech

production with an appropriate set of parameters. If the

model is sufficiently accurate and the parameters are

accurately determined, the resulting output of the model is

in some cases indistinguishable from natural speech.



















PITCH PERIOD


VOCAL TRACT
PARAMETERS


VOICED/
UNVOICED
SWITCH


Figure 1-1. General discrete-time model of speech
production. (From Rabiner and Schafer, 1978)








Most synthesizers use speech bandwidths between 3 kHz

(for telephone applications) and 5 kHz (for higher quality).

The perception of some consonants is slightly impaired if

frequencies between 3 and 5 kHz are omitted. Frequencies

above 5 kHz are perhaps useful to improve the speech clarity

and naturalness, but do little to aid speech understanding.

Current speech synthesizers represent trade-offs among the

conflicting demands of maximizing speech quality while

minimizing memory space, algorithmic complexity, and

computation speed.

Speech analysis is simply the process of estimating

the (time-varying) parameters of the model for speech

production from a speech signal that is assumed to be the

output of that model. Continuous speech is usually analyzed

by performing these operations on short segments of speech

which are selected at equally-spaced time intervals,

typically 10-20 msec apart.

Spectral analysis of speech came of age, so to speak,

with the development of the Sound Spectrograph. This device

provides a convenient means for permanently displaying the

short-time spectrum of a sizeable duration of signal. In

this device, a short speech utterance repeatedly modulates a

variable frequency oscillator. The modulated signal is

input to a bandpass filter. The average energy in the

output of the bandpass filter at a given time and frequency

is a crude measure of the time-dependent Fourier transform.

This energy is recorded by an ingenious electromechanical









system on teledeltos paper. The result, called a

spectrogram, is a two-dimensional representation of the

time-dependent spectrum in which the vertical dimension on

the paper represents frequency and the horizontal dimension

represents time. The spectrum magnitude is represented by

the darkness of the marking on the paper. If the bandpass

filter has a wide bandwidth (300 Hz) the spectrogram

displays good temporal resolution and poor frequency

resolution. On the other hand, if the bandpass filter has a

narrow bandwidth (45 Hz), the spectrogram has good frequency

resolution and poor time resolution.

With the advance of the digital computer, more

sophisticated digital signal processing techniques have been

developed to analyze the speech signal. One of the most

powerful speech analysis techniques is the method of linear

predictive analysis. This method has become the predominant

technique for estimating the basic speech parameters, e.g.,

pitch, formants, spectra, vocal tract area functions, and

for representing speech for low bit rate transmission or

storage. Simplicity of the model and the efficient

non-iterative algorithm for determination of the model

parameters are the main reasons for its use in many speech

applications. The disadvantage is its excessive sensitivity

to the details of the fine structure of the approximated

speech spectrum. The fine structure reflects the effect of

excitation, the effects of shape, length and position of the








time window and the effect of noise disturbances in the

signal.

The basic idea behind linear predictive analysis is

that a speech sample can be approximated as a linear

combination of past speech samples. By minimizing the sum

of the squared differences (over a finite interval) between

the actual speech samples and the linearly predicted ones, a

unique set of predictor coefficients can be determined.

(The predictor coefficients are the weighting coefficients

used in the linear combination.)

Speech synthesis falls into three broad categories:

1. LPC Synthesis (Markel and Gray, 1976)

Linear prediction synthesis is based on a mathematical

model of the speech signal. The basic assumption is that

speech samples can be predicted from a linear weighting of

past speech values, that is, the speech waveform can be

modeled as the output of an all-pole digital filter, which

is excited by an impulse train for voiced speech or a random

noise sequence for unvoiced speech. The actual voiced

excitation waveform resembles a half-rectified sine wave,

but its spectral shaping is included with the filter

response. The glottal shaping is accounted for by the

inclusion of two poles in the system (since the glottal

excitation has an approximate -12 dB roll-off). The filter

is usually represented by 10-12 coefficients and is updated

every 10-30 ms frame. In addition, two parameters

representing the filter excitation are updated every frame:








an amplitude factor and pitch period. The time-varying

prediction coefficients can be obtained by solving a set of

matrix equations which minimizes the mean square error

between the original speech waveform and the synthesized

waveform.

The LPC envelope matches the high-amplitude portions

of the spectrum, at the expense of a poorer model between

formants. So it is only an approximation for unvoiced and

nasal sounds which contain both poles and zeros. The

procedure often underestimates bandwidths.

Its main advantage is that there is a very efficient

algorithm for finding the linear prediction coefficients.

The disadvantage inherent in the LPC method is that an

all-pole model is used to model the speech spectrum. It is

not clear how the bandwidth of a root is related to the

actual formant bandwidth, because the bandwidth of the root

is sensitive to the frame duration, frame position, and

method of analysis. Also there is no direct correspondence

between LP coefficients and physiology of speech production.

2. Formant Synthesis

The formant synthesizer is based on an acoustic model

of speech production. It can be designed and realized in

the forms of analog circuit, digital hardware or computer

program.

The transfer function of the vocal tract is simulated

using a number of formant resonators. In the cascade

connection the relative amplitudes of formant peaks for









vowels come out just right without the need for individual

amplitude controls for each formant. But a parallel formant

configuration is still needed for the generation of

fricatives and plosive bursts. So a hybrid cascade/parallel

formant synthesizer is the best choice. Nasal murmurs and

vowel nasalization are approximated by the insertion of an

additional resonator and anti-resonator into the cascade

vocal tract model.

Formant synthesizers have an advantage over LPC

systems in that bandwidths can be more easily manipulated,

and zeros can be directly introduced into the filter

simulating the vocal tract (Klatt, 1980). Formant

synthesizers are capable of providing speech of good

quality, provided good input data are available. Estimation

of parameters, such as the formant frequencies, formant

bandwidths, pitch etc. can be measured directly from the

speech signal. Locating the poles and zeros automatically

in natural speech is, however, a difficult task.

3. Articulatory Synthesis

Articulatory synthesizers are based on a physiological

model of speech production. They attempt to model

faithfully the mechanical motions of the articulators and

the resulting distributions of volume velocity and sound

pressure in the lungs, larynx, and vocal and nasal tracts.

The anatomical structures that shape the vocal tract

impose constraints on the area functions, and knowledge of








these constraints enable us to simplify our specification of

the shape of the vocal tract.

In effect, the X-ray studies indicate that during the

articulation of vowels the dimensions of the vocal tract

along the length of the tongue are controlled primarily by

the position of the tongue constriction and by the degree of

tongue constriction. A minimum set of parameters may be the

position of the tongue constriction, the size of the

constriction formed by the tongue, and the dimensions in the

vicinity of the mouth opening.

Input to this type of speech synthesizer is in terms

of symbols designating target configurations of the vocal

tract. Then a synthesis program interprets these as

discrete sets of data for an articulatory model, and

generates a sequence of changing area function. The

formants are then calculated and used to control a speech

synthesizer.

Articulatory models of the vocal tract can provide

very natural structural representations of the underlying

anatomy and physiology of the vocal tract which give rise to

the speech signal. Many effects of coarticulation, vowel

reduction, and place allophones are produced automatically,

without the need for special rules. The articulatory model

is very useful for phonetic studies. The disadvantages are

that knowledge about the articulator positions is not easily

available for continuous speech, and the computation is more

complex than for other synthesis methods.








Introduction to Source-Tract Interaction


In the conventional speech production model, the

source and the vocal tract system are considered to be

independent of each other (i.e., varying vocal tract

configuration will not have any effect on the source), which

is true when the glottis is closed, or almost closed. But

when the glottis is open, loading of the vocal tract system

on the source occurs. It has been shown that the loading of

the vocal tract can have appreciable effects on the glottal

pulse shape (Ishizaka and Flanagan, 1972). This is called

glottal source vocal tract interaction or simply

source-tract interaction. It is believed that the

intelligibility of synthetic speech depends on the ability

to reproduce dynamic (transient) sounds such as stops,

whereas the naturalness of voice is mainly determined by the

true reproduction of voiced segments (Childers et al.,

1985). Source-tract interaction has been conjectured to be

important for synthesizing high quality, natural sounding

speech. Speech synthesized with source-tract interaction

sounds more natural than speech generated without such

interaction (Allen and Strong, 1985; Childers et al., 1983).

The acoustics of speech production is based on the

concept of a source and a filter function. In current

models, the source of voiced sounds is represented by a

quasiperiodic succession of pulses of air emitted through

the glottis, as the vocal folds open and close, and the








supraglottal vocal tract acts as a filter that shapes the

spectrum of the glottal flow to produce different sounds.

The filter function is assumed to be linear and short-time

invariant. When the glottis is closed, the vocal tract

filter is typically thought to be best represented by an all

pole model of order 10 to 14 (Ananth et al., 1985). The

phonetic message in speech is mainly conveyed by the

transfer function of the filter representing the vocal tract

system. For example, silent articulation with an external

throat vibrator can produce intelligible speech. Not much

work has been done on the description of the voice source

with reference to speaker specifics and to contextual

factors. Speech synthesis has gained a fair quality on the

basis of conventional idealizations, such as a -12 dB/oct

average spectrum slope and uniform shape. Source and filter

are assumed to be linearly separable.

The shape and periodicity of the vocal fold wave can

vary considerably. The extent to which variability in

period and shape affect speech naturalness and quality is an

important research question. In many existing electrical

synthesizers, the properties of the vocal fold source are

approximated only in a gross form. It is customary to

specify the vocal pitch as a smooth, continuous function and

to use a fixed glottal wave shape whose amplitude spectrum

falls at about -12 dB/octave. In many synthesizers the

source is produced by repeated impulse excitation of a

fixed, spectral-shaping network. An impulse train filtered








by a 2-pole low-pass filter has about the right average

spectrum, but the phase of this waveform is wrong. Primary

excitation of the vocal tract filter occurs at a time

corresponding to the instant the folds open, rather than at

closure. Furthermore, the spectrum envelope is perfectly

regular (i.e. monotonically decreasing at 12 dB per octave),

which contrasts with evidence indicating the presence of

zeros in the spectra of normal voicing waveforms. Such lack

of fidelity in duplicating actual glottal characteristics

undoubtedly detracts from speech naturalness and the ability

to simulate a given voice.

It has been shown that the glottal pulse waveform can

have important effects on the quality of synthetic speech

(the voice produced). Rosenberg (1971) studied the effect

on naturalness of the variation of glottal pulse shape. He

used simulated waveforms with pulse shapes differing in the

number and location of slope discontinuities. His result

indicated that simulated excitations with pulse shapes with

a single slope discontinuity at closure were preferred.

Holmes (1973) has pursued this area and shown that under

certain listening conditions, the use of glottal pulses

derived from speech significantly improves the naturalness

over fixed glottal models. Wong and Markel (1978) have

recently shown that retaining the phase characteristics of a

typical glottal pulse can improve LPC synthesis quality.

To study the glottal source, glottall) inverse

filtering is used. Glottal inverse filtering is a technique








by which the flow past the time varying glottal constriction

is estimated by a filtering operation on the acoustic signal

in human speech. The filtering operation removes the

effects of the vocal tract resonances to reveal the

underlying voice source signal. Almost all techniques for

inverse filtering the speech signal to obtain the glottal

volume-velocity are based on the linear model. The source

is assumed to be a periodic waveform generator which outputs

pulses of volume-velocity. The volume-velocity is input to

a linear, time invariant vocal tract filter. The transfer

function of the vocal tract filter is determined by the

supraglottal articulators. The output of this filter is

then passed through a second filter that models the

radiation at the lips, and is finally output as speech. The

vocal tract filter for vowel sounds is usually modeled as an

all-pole filter; this can be theoretically justified on the

basis of acoustic tube modeling of the vocal tract. The

inverse of the vocal tract filter therefore contains only

zeros or anti-resonances. If the radiated speech wave is

passed through this inverse vocal tract filter, the output

will be the differentiated glottal volume-velocity. A

simple integration of this signal will yield the glottal

volume-velocity. Inverse filtering studies on different

vowels have revealed two important phenomena:

(a) Skewing

High speed and stroboscopic motion pictures of the

glottis during normal voice have generally yielded a rather








symmetrical, triangular waveform for the projected glottal

area (Rothenberg, 1981a). On the other hand, measurements

of the glottal flow waveform by inverse filtering the sound

pressure or the flow at the mouth have often shown a

markedly unsymmetrical waveform, with a slowly-rising

glottal opening phase and a sharply terminating glottal

closing phase (for example, see Miller, 1959; Holmes, 1962;

and Rothenberg, 1973). This dissymmetry of the glottal flow

waveform can be an important determinant of voice quality in

that it increases the high frequency energy of the waveform,

as compared to the projected area waveform, and hence

affects the levels of the formants. It also concentrates

the energy in the glottal closed phase, during which the

vocal tract is most efficient (Fant, 1979a). The degree of

skewness differs for different vowels, and it has been shown

that the first formant load is the most important in

determining the degree of skewing (Ananthapadmanabha and

Fant, 1982).

(b) Ripple

Ripples are sometimes observed in the open phase of

the glottal flow waveforms. It is generally realized that

there can be appreciable first formant energy absorbed by

the glottis during the open phase of the glottal cycle, when

the glottal impedance is finite (Rothenberg, 1981a). This

is called truncation, which means the termination of formant

oscillations by excessive damping within the glottal open

period (Fant and Ananthapadmanabha, 1982). Glottal damping








causes a truncation of formant amplitudes and changes the

formant frequencies and increases their bandwidths during

the glottal open interval. This effect is especially

apparent for high frequency Fl sounds. The vowel /a/

typically has a truncated speech waveform. Its equivalent

effect is to cause oscillations on the glottal flow

waveform. The main perceptual effect of truncation is a

reduction of the loudness level of the formant (Fant and

Liljencrants, 1979). The first formant load has been found

to be the most important in determining the degree of this

effect.

Other source-tract interaction effects have also been

identified by computer simulations, theoretical studies and

inverse filtering experiments.















CHAPTER 2
SOURCE-TRACT INTERACTION



Introduction


In this chapter, we first describe the different types

of speech production models and derive the conventional

speech production model. Then we explain what source-tract

interaction is and what its effects are. A literature

review of source-tract interaction, which includes

theoretical and simulation studies, is given next. Finally,

a summary of all the source-tract interaction effects known

is given.


Speech Production Models


The conventional source-filter model of speech

production includes many inherent limitations and

assumptions which may not be always true. Source filter

theory of voice production is the theory of its

approximations. Time-varying and nonlinear functions

introduce difficulties which obscure an insight in

essentials unless we resort to simplified and approximate

transformations. To completely understand what effects they

have on the resultant synthesized speech, we shall describe

how the conventional speech production model is derived.








(a) Physical Model

The physical model in Figure 2-1 attempts to

simulate the actual physical processes involved in human

speech generation. The physically most correct approach

would be to regard the lung pressure and its associated

muscular back-up as the source and derive the output from a

set of differential equations representing the state of flow

and pressure in the combined subglottal, glottal, and

supraglottal systems in extremely short successive intervals

of time (Fant, 1981). This is actually the principle of the

Ishizaka-Flanagan (1972) model which has become most

influential in speech research. The parameters used are

physiological and include the lung pressure, the vocal tract

area function, etc. The two-mass model for the vocal folds

is shown here, but other relevant models can be used as

well.

The vocal system may be represented in terms of

incremental contiguous sections of a lossy cylindrical pipe.

The shape of the vocal tract may deviate markedly from that

of a straight acoustic tube. For frequencies corresponding

to wavelengths that are long compared to the dimensions of

the vocal tract (less than about 4000 Hz), it is reasonable

to assume plane wave propagation along the axis of the tube.

It is difficult to synthesize any speech signal from

this model, and can probably only be done by digital

simulation using a computer. Extensive computation will be

required, and so it is not practical.










MUSCLE FORCE


LUNGS TRACHEA """..
L BUNG RONCHI VOCAL TRACT
BRONCHI VC
VOCAL
FOLDS

Figure 2-1. Physical model of speech production.
Flanagan et al., 1975)


NASAL TRACT


NOSTRIL
N Un








MOUTH



(From


NOSTRIL

Un



1 DZn


t t
A1--------------------------- A,


LUNGS TRACHEA VOCAL
BRONCHI FOLDS

Figure 2-2. Electrical
et al., 1975)


VOCAL TRACT


equivalent circuit. (From Flanagan


MOUTH








(b) Electrical Equivalent

Sound pressure and volume velocity for plane wave

propagation in a uniform tube satisfy the same wave equation

as do voltage and current on a uniform transmission line

(Flanagan, 1972). Hence, sound pressure and volume velocity

can be considered to be analogous to the voltage and

current, respectively, in an electrical line. The uniform

transmission line can be represented by an equivalent

T-network, and an equivalent electrical circuit (Figure 2-2)

can be established for the vocal system. This has an

additional advantage of being able to use the network

theory, but it is still too complex.



(c) Simplified Electrical Equivalent

The effects of the subglottal and vocal tract systems

for voiced sounds are to introduce resonances, called

formants, in the frequency domain, which have to be

accurately represented in order to have high quality,

natural sounding speech. Hence, limiting ourselves to the

nonnasalized voiced sounds only, a simplified electrical

equivalent circuit (Figure 2-3) can be obtained using

parallel resonant circuits as loads, with the parameters

chosen so as to represent the formants and to approximate

the impedances of the subglottal and the vocal tract

systems. The cascade arrangement of resonators is shown to

yield vowel sounds having formants of proper amplitude when

information specifying the formant frequencies only is










*- Vsi-* Vsn"-


Figure 2-3. Simplified electrical equivalent circuit for
voiced sounds.







A-A


voiced
sounds


impulse
train


Figure 2-4. Source-filter model for voice production.








known. The effect of the radiation has been incorporated

into the formant loads. The time-varying, nonlinear glottal

impedance may be calculated from the measured or modeled

glottal area function, and simulation experiments can be run

to see how the glottal flow varies with different vocal

tract loads.



(d) The Conventional Source-Filter Model

The time-varying and nonlinear glottal impedance still

makes the solution difficult to obtain. To simplify even

further, the subglottal system is completely ignored,

because the pressure drop across the bronchi and trachea is

small, and the subglottal pressure is maintained sensibly

constant over the duration of several pitch periods by the

low-impedance lung reservoir. Also, since the glottal

impedance is generally very large when compared to the vocal

tract input impedance, because of the relatively small

opening of the glottis which separates the subglottal and

supraglottal regions, the effects of the vocal tract loading

on the glottal source are ignored also. This is similar to

having an ideal current source. Here, the glottal source

for the supraglottal region is generally defined as the

volume velocity of air flow passing the vocal folds. The

supraglottal vocal tract acts as a filter that shapes the

spectrum of the glottal flow to produce different sounds.

That is, the source does not depend on the vocal tract

shape. This gives the voiced part of the linear








source-filter model of speech production. The model for

voiced sound production is shown in Figure 2-4.

As we look for more precise models of the voice

source, whether this be for higher quality synthesis of

speech or singing, or for the study of unusual or

pathological voice qualities, the effects of the vocal tract

load on the glottal flow cannot be neglected (Rothenberg,

1981b), i.e., the glottal source and the vocal tract

interact with each other. This is called source-tract

interaction.

In recent years the demand for greater naturalness in

speech synthesis has developed a renewed interest in studies

of the voice source and source-filter interactions. This

demand which is paralleled by a general descriptive need in

acoustic phonetics, e.g., with respect to speech prosody and

individual voice qualities and speaking habits, is revealed

when we attempt to synthesize female speech by rule. Voice

pathology and theory of singing are related topics, where

the need for improved voice source models are apparent

(Fant, 1981).


Effects of Source-Tract Interaction


The major effects of source-tract interaction are

described below:








a) Skewing

The glottal flow waveforms obtained from inverse

filtering are usually skewed to the right when compared with

the glottal area functions (Figure 2-5). This effect has

been studied by Rothenberg (1981a). Using a triangular

shape for the glottal conductance, he was able to get

volume-velocity skewing by loading the conductance with the

inertance of the subglottal and supraglottal tracts. Due to

inertia effects the glottal flow generally builds up more

slowly than implied by the glottal area function but

terminates more steeply to meet the requirement of zero flow

after closure. If the lowest supraglottal resonance (the

first formant Fl) is higher than the voice fundamental

frequency FO, as is usually the case, the supraglottal

loading will be inertive at frequencies between FO and Fl,

which most strongly influence the overall waveshape of the

glottal pulse. The same applies for the lowest subglottal

formant. Hence, a pure inertance can be used as the load

for finding the glottal pulse shape. Since different vowels

will have different inertances for the vocal tract system,

the degree of skewing will be different for different

vowels. Skewing can be an important determinant of voice

quality because it varies the high frequency energy of the

waveform, and thus affects the levels of the formant

frequencies.

For female voices, the fundamental frequency (FO) is

higher and the ratio of Fl/FO is smaller than that for male











GLOTTAL
AREA


GLOTTAL
AIR FLOW







) TIME


FLOW LAG DUE FLOW FORCED TO ZERO
TO INERTIA
TO INERTIA BY THE GLOTTAL CLOSURE


Figure 2-5. Glottal flow skewed to the right.


RIPPLE


Figure 2-6. Ripple superimposed on glottal flow waveform.








voices, so the female glottal flow waveforms tend to be more

symmetrical, as have been seen in the measurements of the

glottal flow waveforms (Monsen and Engebretson, 1977).

Acoustic interaction can cause the glottal source

waveform to vary widely as a function of vowel value and FO,

since the first formant must be high compared to FO in order

for the supraglottal loading to be inertive at an

appreciable number of glottal harmonics, and because the

magnitude of the impedance below Fl varies as a function of

vowel value.



b) Ripple

The glottal flow waveforms obtained from inverse

filtering may have some superimposed ripples (Figure 2-6),

especially when the steady state is reached. One aspect of

formant ripple in the glottal pulse is the increasing rate

of decay of Fl-oscillation during glottal opening, which may

cause a smaller or greater degree of "truncation" of the

oscillation preventing the carry-over of oscillatory energy

to the next period (Fant, 1982a). This has been studied

extensively by Fant (Ananthapadmanabha and Fant, 1982; Fant

and Ananthapadmanabha, 1982; Fant, 1982a; Fant, 1982b) and

can be explained as follows. In the glottal open state, the

sub- and supraglottal parts of the vocal tract are

acoustically coupled through the time variable and nonlinear

glottal impedance, whereas when the glottis is closed the

sub- and supraglottal systems execute approximately free and








separate oscillations. Resonance frequencies and especially

bandwidths may differ in the two states. The glottal open

period can be regarded as a phase of acoustical energy

charging, followed by a discharge at glottal closure.

During the glottal closed conditions, the formants prevail

with a constant bandwidth, i.e., a constant rate of decay,

followed by a relatively faster decay of amplitude during

the next glottal open interval, when the glottal impedance

becomes finite. Thus, glottal damping can cause a

truncation of formant amplitudes during the interval of

glottal opening. The glottal waveform of the vowel /a/ is

typical of truncation. This reflects the higher sensitivity

to glottal damping of open back vowels, such as /a/,

compared to vowels with a wide pharynx cavity. The high

glottal damping is also a general characteristic of vowels

produced with incomplete glottal closure as in a breathy

voice (Fant and Ananthapadmanabha, 1982).

With truncation, the wave shape of glottal pulses may

display irregularities due to superimposed formant ripple.

The presence of such a ripple is one consequence of glottal

damping. It is convenient to use the differentiated glottal

flow to represent the source, thereby including the

frequency characteristics of radiation transfer. The

perturbations of glottal flow induced by formant ripple

become more apparent after differentiation. In the initial

positive part of the differentiated glottal flow, there is

often seen a double peak. The double peak in the








differentiated flow does not correspond to a constant

frequency F1 ripple, because of the time-varying, nonlinear

glottal impedance. In addition to truncation there occurs a

spectral broadening due to Fl-modulation within the glottal

open period. The Fl-ripple starts at a higher frequency and

ends at a lower frequency. The spectrum displays sharp

zeros of appreciable magnitude, the first located above Fl.

Considering truncation phenomena alone-without Fl-modulation

a zero would have been found at Fl. Recently, Fant et al.

(1985b) have shown that the double peak glottal flow

derivative has a spectral correlate of a broad maximum at,

or somewhat lower than, 2 Fl intersected by a sharp zero.

The intraglottal variations in the system function are only

approximately definable by time varying frequencies and

bandwidths of vocal resonances.

Effective bandwidth due to truncation increases with

the open quotient of the glottal cycle and with FO at

constant open quotient (Fant, 1981) and is highly specific

to vowel formant and phonatory mode. Boves and Cranen

(1983) have tried to estimate the changes in the formant

parameters when the glottis opens, using the covariance

linear prediction (LP) analysis. However, LP analysis over

the open phase always failed, so they compared formant

parameters obtained from the closed glottal interval with

corresponding measures obtained from a complete period.

Their results showed that generally the bandwidths obtained








from a complete cycle exceeded those from the closed glottal

interval.

The main perceptual effect of truncation is a

reduction of the loudness level of the formant. According

to Fant and Liljencrants (1979) the truncated envelope

produces a loudness equal to that of an untruncated

exponential which has the same initial amplitude and the

same mean (not r.m.s.) amplitude within the complete glottal

cycle. The spectral 3 dB-bandwidth of the truncated signal

is much larger than this effective bandwidth. Perceptual

matching experiments on truncated periodic Fl responses with

untruncated responses suggested that subjects tend to match

for an equal loudness level of Fl which implies equal mean

value of the envelope.

The first formant is quoted to be the most susceptible

to interaction effects. Examination of the first formant

could indicate the presence of any non-uniform damping.

This would identify the presence of source-tract

interaction. Its effects on the quality is not clear, but

it has been known that the first formant is very important

for vowel quality.

Other source-tract interaction effects have also been

identified (Nord et al., 1984), such as the nonlinear

superposition, where the superposition of the ripples may

affect the glottal flow derivative at the instant of closing

discontinuity and, thus, a change in the excitation level.








c) Linear Superposition

Superposition, which requires a lower degree of

glottal damping, is in a sense the opposite of truncation.

Superposition results from the carry over of formant energy

from one fundamental period to the next. Superposition

provides a maximally positive net effect when a formant

coincides with a harmonic, and a maximally negative effect

when the corresponding resonant peak is located halfway

between two harmonics. In addition, superposition of

formant ripple within the glottal open period may change the

source excitation waveform and spectrum. This is a

nonlinear source-filter interaction.



d) Nonlinear Superposition

Under conditions of small supraglottal damping and

high FO, the Fl ripple may prevail in the latter part of the

glottal opening interval, just before closure, thus

affecting the strength of the main excitation. The ripple

components may affect the phase of the signal (residue),

thus causing either an increase or a decrease in the slope

at closure. This will be referred to as a nonlinear

superposition. It is concluded that formant amplitude

changes at varying FO are a function of both linear

superposition and changes in the scale factor and spectrum

of the glottal source.

Informal experimentation with an electrical analog

version of an interactive voice source model (Rothenberg,








1981b) has shown that as the ratio Fi/FO gets smaller than

about three, the value of this ratio is increasingly

significant in determining voice quality. When Fl/FO is

near integral values, energy from previous glottal cycles

tends to cause a decrease in supraglottal pressure as the

glottis is closing (in addition to any component caused by

the low frequency vocal tract inertance). This decrease in

pressure raises the transglottal pressure and causes a

sharper drop in flow at closure. Likewise, values of Fl/FO

that fall about halfway between integral values tend to

decrease transglottal pressure during glottal closure and

cause a less sharp drop in flow at the instant of complete

closure. Thus, if the ratio Fl/FO is low, the high

frequency energy generated by the glottal closure is

determined by both the vocal tract inertance at low

frequencies and the value of Fl. Fant and Ananthapadmanabha

(1982) estimated that the condition for increased excitation

force would be satisfied by Fl = [n + 1/4]-FO, whereas Fl =

[n 1/4]-FO would have the opposite effect.

The interaction between Fl and FO should be

differentiated from the interaction predicted by the linear

superposition. In linear superposition, a formant is

maximally strengthened when it is an exact multiple of the

fundamental frequency, while the value of Fl/FO for maximum

transglottal pressure during the glottal closure may not be

an exact integer. Of more significance is the fact that

linear superposition predicts that the coincidence of Fl and








a multiple of FO will strengthen only Fl and not the higher

order formants. For nonlinear superposition the ratio of Fl

to FO can have a significant effect on all formants.

Rothenberg (1987) has studied the case of soprano

voice when Fl/FO approximately equals to one. He showed

that a phonation with Fl close to FO minimized air

consumption.

A typical feature found in most simulations is that

because of superposition interaction, one glottal pulse

differs somewhat in shape, peak amplitude, and even in

duration from neighboring pulses even at constant FO and

other phonatory conditions held constant. The period by

period perturbations of glottal flow waveshape probably add

to the naturalness element in normal speech as opposed to

the regularity stereotype of conventional speech

synthesizers. Pathologically extreme perturbations such as

vocal fry affect both periodicity and the gross shape of

glottal flow pulses including mechanical interaction.

Source-filter interaction theory may prove to be especially

important for the analysis of the voice excitation mechanism

at higher fundamental frequencies as in female and

children's voices.

Glottal air flow as well as vocal fold vibratory

patterns may be affected by changes in subglottal pressure

and supraglottal articulations. It is not inconceivable

that the glottal flow pattern may influence the mechanical

motion of the folds and thus of the glottal area function.








One would expect a small shortening of the closure time as a

response to a negative supraglottal pressure peak preceding

the termination of the glottal pulse.


Literature Review


A number of authors have investigated the problem of

source-tract interaction and have tried to elucidate the

effect of the vocal tract on the waveform of glottal volume

flow by means of theoretical analysis or simulation based on

models of speech production.


Glottal Impedance


The glottis is a narrow constriction formed between

two vibrating vocal folds. The excess air pressure in the

lungs causes air to flow through the trachea and the

glottis. This pulsating air flow not only causes acoustic

excitation of vocal cavity resonances but is also

responsible for sustaining vocal fold vibration.

Van den Berg et al. (1957) proposed an empirical

formula for predicting the steady (dc) flow based on

extensive experiments on static larynx models with uniform

glottis. His formula for the pressure drop is

U2 2 U
AP=kP-+ 12 D123
2A A

where p is the density of air, p is the coefficient of

viscosity, U is the volume velocity flow, AP is the excess

subglottal pressure, and A is the glottal area, D is the









glottal depth, and 1 is the length of the glottis. The

constant k = (kI k2) is determined empirically. The

constants kI and k2 are the so-called entry drop and exit

recovery coefficients. The form of the above equation is

guided by aerodynamic theories. The first term is called

the kinetic resistance drop and the second term is called

the viscous drop. According to van den Berg, ki = 1.375,

and k2 = 0.5. Thus, the volume velocity of air flow, U, can

be calculated for given glottal dimensions and pressure.

Recent investigations suggest a revision of the value for

k2, which is much smaller, of the order of 0.01 0.05.

The above discussion is restricted to the glottal flow

through a uniform glottis. Experiments on nonuniform

glottal shapes strongly indicate the dependence of glottal

resistance on the shape of the glottis. We can, to a first

order approximation, estimate the glottal resistance of a

nonuniform glottis to be the same as that of the glottal

resistance of a uniform glottis of width corresponding to

the minimum width of the nonuniform glottis, but with the

viscous drop term omitted. Thus A in the equation

corresponds to the minimum area of the glottis. Owing to

the flow dependent resistance, the glottal damping is larger

at low voice efforts than at high voice efforts.

During phonation the glottal area changes continually.

For small dimensions of the glottis, incompressibility is a

valid assumption. With the air mass in the glottis, the

glottal impedance now incorporates an additional term









corresponding to the glottal inertance. Assuming a constant

glottal depth D the glottal inertance is

D
Lg= P -

Since Lg changes in time with A, the pressure drop across Lg

is


APL = Lg + Udg
dt dt

The effect of glottal inertance is rather small.

For typical values of vocal subglottal pressure, the

viscous term approximately equals the kinetic term when the

glottal areas are just a fraction (< 1/5) of the maximum

area. In other words, over most of the open cycle of the

vocal folds the glottal resistance is determined by the

kinetic term.

The Lg/Rg time constant is small compared with the

fundamental period, so the glottal volume flow may be

considered as a series of consecutively established steady

states.


Simulation Experiments


Ishizaka and Flanagan (1972) proposed their two-mass

model of the vocal folds and succeeded in explaining the

glottal source-vocal tract interaction in terms of

physiological and acoustic parameters of the vocal folds and

vocal tract.








Guerin et al. (1976) developed a glottal source model,

which is shown in Figure 2-7, to generate a volume velocity

signal that includes the interaction with the vocal

cavities. The model is loaded by an equivalent circuit for

the driving point impedance of the vocal tract. This

circuit is controlled dynamically by the first two formant

frequencies. The synthesis of this circuit was based on the

results they have obtained from a computer simulation of a

lossy vocal tract transmission-line model. Rv and Rk are

the viscous and kinetic components of the glottal

resistance, Lg is the glottal inertance and the area

generating box represents the mechanical one (or two) mass

model. They calculated the volume velocity function U(t) of

different vowels by a computer simulation of the circuit,

using the same glottal area function 'A(t). Compared with

A(t), the glottal flow has additional fluctuations at

frequencies near the first formant frequency of the

considered vowel. A "coupling index" was defined as a

measure of the degree of source-tract interaction which was

found to be important for all the first formant range.

In the work of Ananthapadmanabha and Fant (1982), the

acoustic modeling of voice production started by assuming a

specific glottal area function within a fundamental period

and a specific lung pressure. Recent modeling efforts have

incorporated more realistic circuits to simulate the

impedances of the subglottal and supraglottal tracts,

leading to rather complex time-varying relationships between



























P, A(t) F1 V c





L2
U (t)
F2








kj1(t) Rv= k L k3 ck4
A2(t) At) A3(t) A((t)


F2 (t)

Fl(t): first formant; F2(t): second formant.



Figure 2-7. Glottal source model loaded by an equivalent
circuit of the vocal tract input impedance. (From Guerin
et al., 1976)








area and glottal flow. The glottal area function in general

depends on phonetic context, phonatory mode, voice

intensity, pitch etc. The flow and pressure states in other

parts of the system were then calculated by techniques

similar to those of Ishizaka and Flanagan (1972) leading to

numerical determinations of the glottal flow, the output

flow at the lips, and the sound pressure at a distance from

the speaker's mouth.

Speech synthesized with source-tract interaction

sounds more natural than speech generated without such

interaction (Childers et al., 1983; Childers and Wu, 1990).

This was confirmed by employing a glottal area function

which controls the time varying glottal impedance in an

equivalent circuit of the vocal system. The output of this

circuit is a time-varying glottal volume velocity function

which includes the effect of source-tract interaction.

Glottal air flow as well as vocal folds vibratory

patterns may be affected by changes in subglottal pressure

and supraglottal articulations. Guerin (1985) has studied

the effect of source-tract interaction of different vowels

on the fundamental frequency of the vocal folds oscillation,

using a two-mass model of the vocal folds loaded by an

equivalent circuit of the vocal tract input impedance. His

results showed that FO increased slightly with Fl which was

contrary to the measurements of intrinsic fundamental

frequency made on natural speech. Hence, the intrinsic

value of the fundamental frequency of different vowels is








not determined by the acoustic coupling, but by other more

important effects which largely compensate for the effects

of the acoustic coupling.

Cheng and Guerin (1987) have studied the strategy for

controlling the male and female glottal sources, based on

the research on source-tract interaction. Physiological

parameters make the control easier but need heavy

calculations, while acoustic parameters lead to simpler

calculations, but do not allow an accurate control of the

individual characteristics. So they used mixed

physiological acoustic parameters in order to use the

advantages of the two kinds of parameters. The three

independent parameters adopted were lung pressure,

vocal-fold tension and first supraglottal formant which led

to the three dependent parameters of fundamental frequency,

asymmetry quotient and open quotient.


Theoretical Studies


Detailed physical-acoustic models of the subglottal

systems have been proposed that can generate patterns of

pressure and air flow that seem quite realistic (Ishizaka

and Flanagan, 1972). However, such detailed models often do

not make clear which aspects of the interaction between the

glottal source and vocal tract are most active in

determining the quality of the voice. In order to

understand the way in which voice quality is affected by the

source-tract interaction it is desirable to formulate a








model or models that break down this interaction into its

more important and less important components.

The studies will be restricted to acoustic interaction

and not include the effect that the supraglottal pressure

variations might have on the motion of the vocal folds.



(a) Rothenberg's Studies

Rothenberg (1981b) described an interactive model for

the voice source which includes the acoustic interaction

between the glottal source and the subglottal and

supraglottal acoustic systems. He concentrated on the

development of a model which is valid for the more open

vocalic sounds that comprise most of speech and singing. In

such sounds the dissipativee) supraglottal flow resistance

is small compared to the glottal flow resistance and the

frequency of the first formant is appreciably greater than

the voice fundamental frequency. His studies of the glottal

flow have indicated that for such unconstricted vocal tract

configurations the influence of the vocal tract acoustics on

the glottal flow waveform stems primarily from two factors.

The first is the subglottal and supraglottal pressure

variations caused by the inertive components of the

subglottal and supraglottal vocal tract impedances at the

voice fundamental frequency FO and its lower harmonics, and

the second is the supraglottal pressure oscillations at the

lowest vocal tract resonance. The subglottal pressure

oscillations at the lowest subglottal resonance may also be









significant at the higher ranges of fundamental frequency

used in singing and some types of speech, but this factor

has not been included explicitly in his model.

When the ratio of the first formant frequency Fl to FO

is high, say more than about three, the formant energy

carried over between glottal cycles is small enough so that

the inertive loading tends to be the more significant

factor, tilting the glottal flow pulse to the right, and

causing the sharp slope discontinuity at the instant of

glottal closure which generates most of the higher frequency

energy in voiced speech.

For the purpose of this simplified discussion, the

glottal constriction can be thought of as a purely

dissipative flow resistance which is inversely proportional

to the glottal area. The glottal area waveform is

represented by a roughly triangular pulse. This pulse is

similar in shape to many recordings of projected glottal

area (the area of the opening that would be seen from

directly above or below the glottis) that have been made

using photoglottographic techniques. In addition, the

acoustic impedance of the supraglottal and subglottal

systems can be approximated by an inertive reactance at FO

and those glottal harmonics falling below Fl (for the

supraglottal system) and below the lowest subglottal

acoustic resonance (for the subglottal system). The

justification for this simplified representation is that the

supraglottal acoustic impedance as seen by the glottis is








inertive for frequencies more than a few percent less than

Fl, and the subglottal acoustic impedance as seen by the

glottis also tends to be inertive for frequencies between

the highest respiratory tissue resonance, which is of the

order-of-magnitude of 10 Hz in adults, and the lowest

acoustic resonance, which is roughly 300 to 400 Hz in

adults.

Since the subglottal and supraglottal air masses can

be considered to be more inertive (mass-like) than compliant

(compressible) under his assumptions, if the vocal folds

open after being closed a long time, there will be a delay

or lag in the build-up of air flow relative to the increase

in area, as the lung pressure acts to overcome the inertia

of the combined air mass. (The inertance of the air mass in

the glottis acts differently because it is time-varying and

will be neglected in this simplified discussion.) If we

assume a linear-system viewpoint, the opening phase of the

glottal air flow, until about 3/4 of the glottal area pulse

has passed, shows a time lag, or shift to the right, due to

the time constant Lt/Rg, where Lt is the tract inertance at

FO and its lowest harmonics and Rg is the (time-varying)

glottal resistance. This time constant also causes an

appreciable rounding or smoothing of the top of the air flow

pulse, since the time constant is near its largest value at

that time due to the low value of Rg.

However, the linear system analogy breaks down during

the final 1/4 of the glottal pulse, since the closing vocal








folds force the glottal resistance to be infinite at the

closure (assuming perfect closure), and thereby force the

flow to zero in a relatively short time. During that time

interval (the last 1/4 or so of the glottal pulse) the

tracheal pressure can be found to have a significant

increase due to the inertance of the subglottal flow, and

the pharyngeal pressure a significant decrease due to the

inertance of the supraglottal flow. Thus, the transglottal

pressure during this interval is much higher than during the

rest of the glottal pulse, and acts to support the glottal

air flow until the actual instant of glottal closure is

approached.

Figure 2-8 shows the solution of the nonlinear

differential equation that results when the glottis is

represented by a time-varying resistance and the subglottal

and supraglottal acoustic systems by a single constant

inertance (Rothenberg, 1981a). The subglottal pressure will

be considered to be constant and the glottal inertance will

be considered to be zero. The glottal admittance will then

be a pure conductance. This conductance will be considered

to have a symmetrical, triangular shape, as the vocal folds

open and close during the glottal air pulse. Though this

representation does not properly reflect the flow dependency

of the glottal resistance, it should yield a good

approximation to the actual glottal flow for small values of

supraglottal impedance, if the variation in projected

glottal area is approximately triangular. The system is










INERTIVE LOADING


Y9 U9
.1 + L



























0 TIME=0


Figure 2-8. Glottal air flow resulting from a symmetrical,
triangular variation of glottal admittance, assuming the
simplified interactive model shown in the figure for the
glottal source and vocal tract. (From Rothenberg, 1981b)
.2



Ug .5










2










TIME

Figure 2-8. Glottal air flow resulting from a symmetrical,
triangular variation of glottal admittance, assuming the
simplified interactive model shown in the figure for the
glottal source and vocal tract. (From Rothenberg, 1981b)


YgMAX








shown in the figure in its analogous electrical circuit

form, where

Yg = 1/R = the glottal conductance

PL = the average alveolar pressure in the lungs

Lt = the sum of subglottal and supraglottal

inertance near FO

Ug = the glottal volume velocity

The form of the resulting current pulse is determined

by the "normalized vocal tract inertance" Lt defined as



Lt = Lt2Y



where Zp is the duration of the glottal pulse, and YgMAX is

the maximum glottal conductance.

The major feature of the air flow waveforms in

Figure 2-8 is that there is a critical range for the

normalized inertance Lt, from about 0.2 to 1.0, in which the

glottal flow changes from a roughly symmetrical triangle to

a rounded sawtoothh" having one major point of slope

discontinuity at the instant of closure. In fact, the

mathematical solution to this idealized case shows that the

slope of the flow waveform becomes infinite at closure for

all values of Lt larger than unity. Since the high

frequency energy produced at a discontinuity of slope tends

to be proportional to the change of slope at the

discontinuity, the high frequency energy produced at the









termination of the glottal pulse can be greatly increased by

inertive loading.

The pulse skewing effect increases with increasing

total vocal tract inductance, with increasing glottal

conductance, decreasing glottal pulse duration and

decreasing lung pressure.

The flow dependency of the glottal conductance was not

considered in the analysis, but it was discussed in

Rothenberg (1985b). Also, Fant (1982a) gave an exact closed

form solution for the flow given lung pressure, a triangular

glottal area function, and a representation of the sub- and

supraglottal impedance by inductance elements only.

Inverse filtering studies and motion pictures of the

glottis during voicing have shown that there is often a

patent air path between the arytenoid cartilages. The

general result of this glottal leakage is to cause a gradual

onset of the glottal flow pulse, and a more gradual offset,

with less high frequency energy produced at both locations.

The reduction of high frequency energy at the instant of

glottal closure is of special interest because of its strong

potential effect on voice quality.

The R, L model in Figure 2-8 does not include the

interaction with the first formant. To include a

first-order approximation to the action of the first

formant, the model can be modified by adding an oral

compliance, Co, as shown in Figure 2-9. This oral

compliance can be considered a lumped approximation to the










DISSIPATIVE FLOW RESISTANCE

INERTANCE OF AN AIR MASS


7N


COMPLIANCE OR COMPRESSIBILITY
OF AN AIR VOLUME


ORAL
CONSTRICTION.
SPHARYNX A
ORAL AIR FLOW
CAVITY AT THE MOUTH
y7,Um
N.A-- l---s'^


SUm


Figure 2-9. An interactive model for the glottal source and
vocal tract that includes the effect of the first
formant. (From Rothenberg, 1981b)









compressibility of the supraglottal air and, at lower values

of Fl, a small component due to the effective compliance of

the walls of the supraglottal tract. In this model, the

supraglottal inertance is split into two parts, one on

either side of the oral compliance. The forward or oral

component is the prime determinant of Fl, in combination

with Co, while the rear or pharyngeal component is more

important in determining the overall asymmetry or tilting of

the glottal air flow waveform, since it acts directly on the

glottis, without the "cushioning" effect of an intermediate

compliance. In this model, a back vowel such as /a/ would

have a high value for the pharyngeal inertance and a low

value for the oral component, while the reverse would hold

for a front vowel such as /i/. Naturally, if this model is

to be useful, a more detailed definition would have to be

worked out from these general principles.

The dissipative elements associated with the vocal

tract, Roc, ROL, and RON, are shown dashed, since not all may

be needed in a simple model. Roc primarily represents the

dissipation associated with the compressibility of the air

flow and the compliance of the cavity walls; ROL represents

the dissipation associated with the velocity of the air flow

(boundary layer effects, etc.); and RON represents any

shunting effects, such as a small velopharyngeal leakage.

For non-nasal vowels with a high value of Fl, the main

effect of oral dissipation is to determine the damping of Fl

during the period of glottal closure, and since the total








dissipative loss is generally very small in this case, any

one of these three components can be used. However, for low

values of Fl or for nasalized vowels, the placement and

distribution of the dissipative loss elements should be

reconsidered.

Though an inertive loading of the glottal source would

produce flow waveforms very much like those observed by

using standard inverse filtering techniques, given a

symmetrical variation of glottal admittance, it still

remains to be shown that this type of glottal-supraglottal

interaction is significant in such activities as speech or

singing. The most direct method might be to measure the

supraglottal impedance, but this requires the measurement of

the pressure just above the glottis, and is difficult to

implement. Using another approach, a nonlinear inverse

filter in which some of the effects of the glottal

supraglottal interaction are removed (Rothenberg and

Zahorian, 1977) can be implemented. It can be seen that in

this case the supraglottal impedance did cause an alteration

of the glottal flow similar to that produced by inertive

loading.

Another approach in measuring the effect of

supraglottal load is to change it while keeping the glottal

area function approximately invariant. One way this can be

done is by changing the vowel value. It is found that

vowels with a constriction closer to the glottis and a

higher first formant tended to have a glottal flow waveform









which was more skewed to the right, with a steeper flow

termination, and therefore might be expected to have more

high frequency energy generated by the termination of the

glottal closure.

Finally, the presence of supraglottal loading effects

can be tested by comparing vocalizations made with air and

with a large proportion of helium mixed with the air. By

reducing the acoustic inertance in the vocal tract, the

helium would be expected to reduce any supraglottal loading

effect, if present. It was found that the symmetry of the

waveform increases significantly with helium displacing some

of the air.



(b) Fant's Studies

Ananthapadmanabha and Fant (1982) calculated the true

glottal flow and its components, based on the assumption

that the source-filter interaction was mainly confined to

the first formant of the vocal tract and that the glottal

area function was given. They derived a linear differential

equation describing the variation of pressure drop across

the first formant load, and solved the equation by making

use of the Laplace transform. In their analysis, the

glottal flow was assumed to be linearly related to the

pressure drop across the first formant load. According to

Koizumi et al. (1985), this was not the case and they solved

a nonlinear differential equation with the glottal flow

properly expressed as a polynomial in the pressure drop









across the first formant load. In the time domain, the

glottal flow has two components:

(a) source residue component it describes the main

pulse shape of the true glottal flow, and

(b) ripple component.

Finite initial conditions of vocal tract energy

storage adds to the ripple component. Since the source

residue component is a smooth function, it can be described

parametrically.

The simplest way to understand the ripple phenomenon

is to consider the single-formant model (Figure 2-10). This

model has been used extensively to study source-tract

interaction effects. The vocal tract is represented to a

first approximation by the RLC resonant circuit for the

first formant. Rg(t) and Lg(t) are the nonlinear and

time-varying glottal resistance and inductance,

respectively, and are controlled by the glottal area

function Ag(t) as well as the current flowing through them,

Ug(t). If the impedance due to Rg(t) and Lg(t) is much

larger than the vocal tract input impedance Zt for all t,

then the glottal volume velocity Ug(t) will be essentially

independent of Zt and there will be no source-tract

interaction. This is true, however, only when Ag(t) is very

small or zero.

During the glottal closed conditions, the formants

prevail with a constant bandwidth, i.e., a constant rate of

decay. During the next glottal open interval, the glottal



























I< FIRST
P, -I FORMANT
LOAD












Zt






Figure 2-10. A simple model to study the source-tract
interaction effects.
Zt



Figue 210. siple ode tostud th souce-rac
inteactin effect








impedance becomes finite and acts as an additional path for

the parallel resonant circuit. The bandwidth increases

because of the extra damping, and the formant decays at a

relatively faster rate. Thus, glottal damping can cause a

truncation of formant amplitudes during the interval of

glottal opening. This truncation effect is especially

apparent in maximally open vowels, especially back vowels of

high Fl, such as /a/.


Summary of All Source-Tract Interaction Effects


On the basis of transient theory analysis, the

following major effects of source-filter interaction have

been identified. These are (1) skewing, (2) truncation, (3)

dispersion, (4) superposition linear, (5) superposition -

nonlinear, (6) superposition mechanical, and (7)

supraglottal.

(1) Skewing: Due to the load on the glottis, the flow

pulse is skewed compared to the area function. This skewing

depends on the input inductance of the load. Acoustically,

the main effect of skewing is to uniformly increase the

level of all the formants.

(2) Truncation and (3) Dispersion: The vocal tract

resonances and bandwidths undergo continuous modulation over

the glottal open phase due to coupling to the subglottal

system and the time-varying nonlinear glottal impedance.

The bandwidth varies considerably, resulting in an

exponential ringing over the glottal closed phase and an








almost complete truncation over the open phase due to the

increased glottal damping.

(4) Superposition linear: In those cases (notably

high pitched voices) where the truncation is not

significant, energy will be carried over from one glottal

period to the next. The degree of the superposition depends

on the relation between pitch frequency and formant

frequency.

(5) Superposition nonlinear: The superposition

within the open phase may affect the glottal flow derivative

at the instant of closing discontinuity and, thus, a change

in the excitation level.

(6) Superposition mechanical: It is suspected that

the presence of a superposition component may, at times,

affect the mechanical vibrations of the vocal folds.

(7) Supraglottal: It is evident that a supraglottal

constriction will affect the transglottal pressure drop and,

thus, the pattern of vocal fold vibrations. This is typical

of voiced fricatives. Bickley and Stevens (1987) have

studied the effects of a vocal tract constriction on the

glottal source. Their results showed that the more

constricted configurations resulted in a longer open times

for the glottis compared to that during the open vowel

configurations.















CHAPTER 3
INCORPORATION OF SOURCE-TRACT INTERACTION



Introduction


In this chapter, we first describe the different ways

possible to synthesize speech that will include source-tract

interaction. Then, our method of incorporating source-tract

interaction effects into the conventional speech production

model is presented. The glottal flow waveforms required for

the model are estimated by the technique of glottal inverse

filtering, and a review of its literature is given. Source

models to fit the glottal flow waveforms are discussed.


Modeling Source-Tract Interaction


Thanks to the linear separability of voice source and

vocal tract system, the conventional model allows for an

unequivocal definition of both the source and the system.

For models in which voice source and vocal tract interact,

source and system can no longer be defined unambiguously,

nor can they be totally separated. There exist various

combinations of a source and a filter function that will

produce one and the same or approximately the same output.








(a) The most complete model of speech production is that of

Ishizaka and Flanagan (1972) who have developed a two-mass

model of the vocal folds incorporated in a complete vocal

tract network including the subglottal system, i.e., the

lungs, bronchia, and trachea and the supraglottal system

including a finite cavity wall impedance and nasal system.

Self-oscillation is insured by appropriate feedback of

pressure/flow states affecting the mechanical system

function of vocal fold vibration, the main power deriving

from the expiratory force as represented by the lung

pressure. This model does not have a specific source in the

linear network sense. The two-mass vibratory pattern is

accordingly under the influence of physiological parameters,

i.e., lung pressure, muscular tensions, the rest position of

the vocal folds, and the mass of vibrating parts to which

are added the acoustic load of the sub- and supraglottal

systems. As long as the flow is not reduced by a

supraglottal constriction comparable to that at the glottis,

the glottal area function remains rather insensitive to

articulatory variations.

This model incorporates both mechanical and acoustical

source-tract interaction. However, the knowledge of

aerodynamic forces within the glottis is not sufficiently

well developed and the vibratory pattern of vocal folds is

too complex and too detailed to be directly modeled in a

practical synthesis scheme.








(b) The glottal area as a function of time, is an

alternative to the vocal-fold model. One could thus start

out with lung pressure and glottal area function and solve

for any flow and pressure within the complete system, e.g.,

the output flow at the lips or the input flow to the

supraglottal system, i.e., the glottal volume velocity flow.

Another possibility is to produce a two-stage

synthesis. In the first stage a glottal area proportional

voltage is fed into a Foster-type cascade of parallel

resonant circuits representing the Fl and F2 vocal

tract-impedance load. The resulting current function is the

input to the second stage which is a conventional cascade

formant synthesizer.

If the two-dimensional projected glottal area function

is used, it cannot represent the complex three-dimensional

movements of the vocal folds. The lower and upper lips of

the folds do not move in phase, the longitudinal component

producing alternatively converging and diverging shapes.



(c) In the third and approximate model, the source function

is the already smoothed version of glottal flow, i.e., the

ripple is excluded, feeding into a vocal tract network with

the glottal impedance (in a more general model in series

with the subglottal impedance) shunting the input and

drawing current during the glottal open phase which produces

truncation and corresponds to the ripple component of the

true glottal flow.








Alternatively, the smoothed glottal flow can be

combined with rules for bandwidth broadening to represent

truncation or even better intraglottal variation of formant

bandwidths and maybe frequencies.

This model includes the acoustical source-tract

interaction only, but not the mechanical source-tract

interaction.


Source-Tract Interaction Incorporation


To incorporate the source-tract interaction effects

into the conventional speech production model, the simplest

way is to adopt a variable glottal pulse model. The

smoothed glottal flow can be modeled here, which may be

represented by a few glottal source parameters. To simulate

the ripple effects, an open phase vocal tract filter which

has higher formant bandwidths and maybe formant frequencies

than the closed phase counterpart is used for voiced sounds.

The proposed speech production model is shown in Figure 3-1.


Measurement of Model Parameters


Measurements of model parameters should be made from

the speech signal, but with the additional knowledge of the

electroglottographic (EGG) signal, more robust processing

can be performed.

For voiced sounds, the closed phase vocal tract

parameters can be obtained from the closed phase covariance

LPC analysis. The glottal flow waveform can then be






















PITCH PERIOD


GLOTTAL SOURCE
PARAMETERS


OPEN/CLOSED PHASE
VOCAL TRACT
PARAMETERS


VOICED/
UNVOICED
SWITCH


Figure 3-1. Speech production model with source-tract
interaction.








obtained by inverse filtering. A source model can be fitted

to the glottal flow waveform to obtain the glottal source

parameters. To estimate the open phase vocal tract

parameters, a new method has to be developed.


Electroglottograph (EGG)


The EGG measures the radiofrequency (RF) impedance

across the larynx and hence the area of contact of the vocal

folds (Childers and Krishnamurthy, 1985). It monitors the

vibratory motion of the vocal folds.

A pair of electrodes is applied to the neck at the

level of the larynx. A high frequency (about 5 MHz) current

passes from one electrode through the neck and is picked up

by the other electrode. As the subject phonates, the

opening and closing of the vocal folds change the electrical

impedance of the neck in the region of the electrodes. This

modulates the radio frequency (RF) current, which is

demodulated using a detector to yield the electroglottograph

(EGG) signal.

The EGG indicates the electrical impedance through the

neck at the level of the larynx and thus monitors variations

in vocal fold contact: glottal closure is associated with a

reduction in tissue impedance. A time lag for the acoustic

propagation delay from the glottis to the microphone is

applied to the EGG signal when it is compared with the

speech signal. The EGG signal is for inverse vocal fold








contact, so that an increase in amplitude denotes glottal

opening.

The steep negative slope of the EGG signal associated

with glottal closure occurs in one or two sample points.

Glottal opening occurs more slowly and makes the true

opening point more difficult to determine accurately

(Childers and Krishnamurthy, 1985).

The EGG signal is immune to the surrounding acoustic

disturbances and provides a robust pitch detector. The

pitch period cannot be reliably estimated from the EGG

waveform by determining the zero-crossing interval because

of noise perturbations and dc level shifts. A 351-point FIR

linear phase high-pass filter with a cutoff frequency of 80

Hz is used to remove the low-frequency variation.

The EGG can be used as a tool for validating speech

processing algorithms and for estimating possible lower

bounds for both computation and performance of these

algorithms. It can also be used for "bench marking" how

well certain speech analyses algorithms perform. Further,

with the aid of the EGG as an exploratory tool one may be

able to invent new algorithms which will work on the speech

signal alone.

The EGG channel can help solve the deconvolution

problem of inverse filtering the speech signal, improve

voiced, unvoiced, and silence detection and fundamental

frequency estimation, and facilitate spectral estimation and

formant tracking (Krishnamurthy and Childers, 1986). The








two-channel (speech, EGG) speech analysis technique leads to

computational and performance improvements over "speech

only" analysis methods due to the added EGG channel. The

EGG-based pitch detection scheme provides the pitch on a

period-by-period basis.

The EGG does not reflect a direct measure of glottal

area. It is postulated that the tissue impedance is

inversely proportional to lateral contact area of the vocal

folds. Both the glottal volume-velocity and EGG waveforms

capture features of the vocal fold motion, but in a

complimentary fashion. The EGG waveform provides more

information during glottal closure, whereas volume flow

provides more information during the open portion of the

cycle. The two taken together are superior in many ways to

the glottal area function determined by photographic means,

in which information is apparently lost in the process of

projecting the three-dimensional glottis onto a horizontal

plane.


Glottal Inverse Filtering


The process of estimating the glottal volume velocity

by removal of vocal tract resonances from speech signals is

known as glottal inverse filtering. The objective is to

find the shape of the vocal fold wave (source of

excitation), since the final speech signal is a function of

both the source waveshape and the vocal tract transfer

function. The vocal folds are located in a rather








inaccessible place as far as making measurements is

concerned, particularly when they are in operation. The

output waves which are generated by the vocal folds have

been thoroughly hidden by the complex acoustical nature of

the vocal tract.

If a closed glottal phase does not actually occur, a

unique glottal volume-velocity cannot be determined from the

speech waveform. Similarly, if zeros are present in the

vocal tract system, as during nasalized speech, the

resulting time lag of the input waveform makes a unique

determination of the glottal volume-velocity impossible

because the glottal waveshape zeros cannot be separated

unambiguously from the vocal tract zeros. Thus, an all pole

model of the vocal tract is used for glottal inverse

filtering, care is taken to avoid nasalized speech and a

closed glottal phase is assumed.

Inverse filtering provides a picture of the true

glottal flow provided that it is an exact inverse of the

transfer from glottal flow to the speech wave. This implies

that frequencies and bandwidths of the inverse filter be set

to represent glottal closed conditions. An accurate

estimation of either the glottal volume-velocity or the

vocal-tract filter allows a determination of the other

quantity to within the limits of the assumed model. Due to

the lip radiation impedance which introduces a zero at dc,

the glottal volume velocity baseline cannot be recovered

theoretically.








Low frequency noise is an ever present problem in

glottal inverse filtering. It was impossible to avoid the

presence of very low frequency noise in the microphone

output due to slight variations in room air pressure, and

air movements caused by breathing and slight body movements.

This noise made it essential to limit the low frequency

response of the system by means of a.c. couplings in the

amplifiers, but even so some remaining noise, mainly in the

region of 10 Hz, caused slight variations of the base line

on the measured laryngeal waves.

The glottal volume-velocity reflects the action of the

vocal folds and is thus an important indicator of laryngeal

function. Any abnormality of the larynx that affects the

vibrational pattern of the vocal folds and the audible

quality of the speech will be evident in the glottal

volume-velocity waveform. However, the resonances created

by the vocal tract make the degree of an abnormality

difficult to quantify in the resultant acoustic speech

waveform. The estimation of the glottal volume-velocity

waveform from acoustic speech thus has an important

application in the study of laryngeal pathology, in the

detection and diagnosis of laryngeal disorders.

To recover the glottal pulse shape accurately the

original speech signal has to be recorded and sampled

without phase distortion throughout the frequencies of

interest. Because standard tape recorders distort phase,

the recording must be made with an FM system or by direct








digital conversion. Standard studio microphones also

introduce considerable phase distortion, so the speech

pressure wave has to be recorded with an instrumentation

condenser microphone. Instrumentation condenser microphones

have the necessary phase characteristics and a frequency

response that permits the recording of considerable detail

in the glottal pulse, but recording in a free field they

cannot capture the dc component of the airflow. This means

that the free-field microphone technique will miss the

continuous part of the airflow that occurs when the glottis

vibrates without making a complete closure during the cycle.

Other drawbacks include the fact that the amplitude of

glottal flow cannot be calibrated and that the microphone is

sensitive to very low frequency changes in pressure in the

environment in which the recording is made.

Time domain inverse filtering reveals more of the

overall pulse shapes relevant for a lower part of the

spectrum than spectral levels in formant regions. Frequency

domain inverse filtering does not demand an extended low

frequency response and may thus be performed from ordinary

tape recordings. One alternative, preserving spectral

amplitude information only, is to start out from a narrow

band harmonic spectrum and subtract on a dB scale the

all-pole transfer function given an estimate of formant

frequencies and bandwidths.








Literature Review


Miller (1959) used an analog inverse network to try to

cancel the first formant. The parameters of the network

were adjusted so as to obtain zero current. His results

indicated that the main excitation of the higher resonances

occurs at the point of vocal fold closure and that the

magnitude of this excitation can be controlled by the talker

over wide ranges.

Holmes (1962) used an inverse filter consisting of a

cascade of five similar networks whose antiresonance

frequencies and bandwidths can be adjusted to remove the

formants. The frequencies and bandwidths of the zeros are

adjusted to produce minimum formant frequency ripple in the

output waveform. He showed that in many cases there were

also well defined instants of excitation of the second and

higher formants at other points in the laryngeal wave (the

instant of opening).

Rothenberg (1973) derived the volume velocity waveform

at the glottis during voiced speech by inverse-filtering the

volume velocity waveform at the mouth. The volume-velocity

waveform at the mouth was captured by means of a

circumferentially vented pneumotachograph mask. Unlike the

technique of inverse-filtering radiated acoustic pressure,

this method provides a signal that is accurate down to zero

frequency, not susceptible to low-frequency noise, and

easily calibrated in amplitude by a constant air flow.








Sondhi (1975) employed a reflectionless uniform tube

to neutralize the effects of the vocal tract transfer

function, so as to measure the glottal airflow directly.

Variations in the male and female glottal wave with

different speakers and different phonetic conditions have

been studied by Monsen and Engebretson (1977) with this

tube. Analysis of the data indicated a wide variation of

the glottal waveform shape, its rms intensity and

fundamental frequency, phase spectrum, and intensity

spectrum. It was observed that as the fundamental frequency

changes over time, the glottal source varies in one of two

different ways. In one type of change, the harmonic

relations in the glottal spectrum become steeper as the

fundamental frequency rises. In a different type of

glottal-wave change, relations between harmonics tend to

remain the same despite a change in the fundamental

frequency; the source spectrum in this case is simply

shifted along the frequency and amplitude axes as a function

of fundamental frequency. To account for these variations

in the glottal source, at least three factors must be known:

the sex of the speaker, the voice register in which he

phonates, and the linguistic context in which the phonation

occurs. The slope of the spectrum for males is less steep

than that of the females. The female glottal waveshape

tends to be more symmetrical. Loud voice typically has a

higher FO than normal voice. Soft voice has a more

symmetrical waveform and a more steeply declining spectrum.








For loud voice, the closing portion of the wave is brief and

abrupt, and there is a consequent increase of energy

particularly in the higher frequencies.

Holmes (1976) used partial inverse filtering to

produce waveforms representing single formants of voiced

speech. His results confirmed the well known fact that the

main formant excitation normally occurs at glottal closure.

However, there is, frequently, evidence of additional

excitation, not only at glottal opening and during the open

phase, but also after closure.

Hunt et al. (1978) described an interactive digital

inverse filtering system in which the advantages of analog

and digital methods are combined to provide a facility with

much greater convenience and power than either.

Wong et al. (1979) suggested a straight forward (but

computationally expensive) approach for performing glottal

inverse filtering from the acoustic speech waveform by

analyzing the normalized linear prediction error sequence

obtained by calculation of the p-pole total linear

predictive error on an M-point window of the speech

waveform. Both the moment of glottal closure and opening

can be determined from the normalized total squared error

with proper choices of analysis window length and filter

order. The window is moved through the speech waveform one

point at a time and after energy normalization the

total-error sequence represents a measure of the fit of a

p-pole model to segments of the waveform. The total error








is at a minimum (ideally, zero) during analysis of a

completely closed phase segment. However, in cases of high

frequency or breathy speech where the closed phase is of

shorter duration, this method may not provide unambiguous

local minimal ranges of the normalized error sequence that

are necessary to indicate closed phase. This problem occurs

when the duration of the closed phase is less than the

length of the analysis window. To estimate the actual

volume velocity waveform, the filter for a single period was

chosen as that corresponding to the minimum normalized

error.

Fant (1982a) has studied the covariation of flow

parameters with voice intensity and pitch using analog

inverse filtering. There appear to be two modes available

to produce an intensity increase. One is a rise in the

overall scale factor of glottal flow pulses which is a main

consequence of increased subglottal pressure. The other is

an adduction of the vocal folds physiologically induced by a

medial compression, which may increase the steepness of the

closing branch of glottal pulses while maintaining or even

reducing the amount of air contained in a single pulse. For

FO-variations, the flow amplitude shows a maximum around 115

Hz and then decreases in inverse proportion to FO. The flow

derivative, indicative of formant amplitudes, shows a

maximum at FO=118 Hz and then exhibits a fall rise contour

indicating increased efficiency at higher pitch.








Veeneman and BeMent (1985) developed an automated

on-line method to determine the glottal volume-velocity

waveform from both speech and EGG signals. A high pass

filtering operation on the speech pressure waveform using an

electret condenser microphone, was combined with a

compensating low pass operation to maintain a flat closed

phase in the derived glottal volume-velocity.

Milenkovic (1986) described a linear model of a

glottal pulse waveform along with a procedure for jointly

determining an AR model of the vocal tract response together

with the parameters of the glottal pulse model. Closed

glottal LPC analysis is based on an implied model for the

glottal pulse, and the inverse filter coefficients are

optimized with reference to that model. Very simply stated,

the model specifies that the glottal pulse is zero valued

over the interval one has chosen to minimize the square of

the inverse filter output signal. An alternative philosophy

to the one underlying closed glottal analysis is to employ a

voice source model which describes the voice source signal

over an entire pitch period, and to optimize the inverse

filter using data from an entire pitch period. Use of a

whole pitch period provides the increased number of speech

samples required for proper analysis of high fundamental

frequency speech. In addition, a model fit that includes

the entire pitch period may be less sensitive to incomplete

glottal closure than a fit that relies on the closed glottal

interval alone. The assumption was made that during the








glottal closure interval, the voice source waveform is flat.

The assumption was also made that the glottal wave begins

and ends at the same amplitude in the course of the open

phase. These assumptions put a constraint on the basis

functions that the time integral of each basis function

over a pitch period is equal to zero.

Hunt (1987) studied the glottal excitation in steady

vowels of several modes of phonation obtained by interactive

inverse filtering. Electroglottograph waveforms were shown

together with simultaneous glottal airflow waveforms and

waveforms for individual formants. Modal voice shows

formant excitation concentrated on the instant of closure.

Falsetto voice shows a triangular or sinusoidal airflow

waveform. Breathy voice shows appreciable formant

excitation both on closure and at the center of the open

phase. Creaky voice shows appreciable excitation at the

start of the open phase as well as its end, and there is

often an alternation in spectral content of the excitation

from cycle to cycle causing the relative intensities of

formants to vary. In examples of extreme creak the airflow

waveforms are complex and difficult to interpret, but they

are similar to the electroglottograph waveforms.

Lee (1988) used a two-pass method to perform the

inverse filtering on the speech signal. In the first pass,

the locations of the main pulses of the LP error signal were

identified. Then, using these main pulses as indicators of

glottal closure, a "pseudo closed phase" is selected as the








analysis interval for a pitch-synchronous covariance LP

analysis to estimate the vocal tract filter, which in turn

is used to obtain the desired glottal volume-velocity

waveform.


Automatic Glottal Inverse Filtering


As long as inverse filtering studies are undertaken in

order to obtain a basic understanding of the nature of the

glottal pulses an extremely high reliability may not be

required. If, however, the inverse filter outputs are

brought to bear to test models of the aerodynamics and

acoustics of speech production, reliability and accuracy

become central issues.

At first, the inverse filtering was done with an

analog inverse filter adjusted to cancel vocal resonances of

recorded signals. The parameter settings are supposed to be

optimal if the output glottal waveform contains a

ripple-free flat interval representing the closed glottal

interval where the air flow should be zero (if the glottis

closes completely) or fairly constant (if, in breathy voice,

an opening in the cartilaginous part of the glottis

remains). Usually this requires the adjustment of the

parameters of the inverse filter by a skilled operator and

the reliability and accuracy of this is in question.

However, with the advent of the digital computer, a number

of (quasi-)automatic inverse filtering implementations have

been reported which do not need operator intervention.








Inverse filtering outputs can also be compared with (almost)

simultaneous physiological registrations to study its

performance (Krishnamurthy and Childers, 1981).

With the additional knowledge of the

electroglottographic (EGG) signal, the glottal closed phase

can be identified more easily, and fully automatic glottal

inverse filtering becomes possible. Glottal closure is

associated with a rapid reduction in tissue impedance.

Glottal opening occurs more slowly and makes the true

opening point more difficult to determine accurately.

The inverse filter is determined by a linear

prediction covariance analysis on the closed phase region of

the speech waveform, as identified from an EGG signal. The

bounds of the potential closed phase region determined from

the EGG will define the maximum frame size. To select a

closed phase analysis region from the many possible, a

closed phase "flatness" measure is used. This yields the

closed phase region that gives the minimum variance glottal

volume-velocity waveform over all the closed phase regions

derived from the sample epoch.

Since vocal tract resonant poles appear only as

complex-conjugate pairs, any real roots of the polynomial

should be removed after factoring. The real pole at zero

frequency will typically occur due to low-frequency

recording noise or a non-zero mean in the short analysis

window. Real poles may also occur when the required filter

order is over specified. The first effect is avoided by








high-pass filtering the speech data, but the second cause

may still lead to a real zero. If it is not removed, "jags"

at the points of glottal closure will occur. A real pole

may also occur at the half-sampling frequency. When it is

of narrow bandwidth, it generally indicates a formant

location nearby, and thus should be retained. If a real

pole occurs due to spectral shaping requirements in the

analysis, without there being a nearby resonance, it will

generally be of wide bandwidth. Including such a pole in

the inverse filter will have a minimal effect on the

results. Therefore, as a practical matter, poles at the

half-sampling frequency are not removed, if they occur. The

derived vocal tract filter was then used to obtain the

volume velocity by inverse filtering the speech signal.

A number of limitations can be raised for closed

glottal interval LPC analysis. The first is that the closed

glottal interval is difficult to locate. For a real-time

voice source analysis in a vocoder, this is a valid

limitation, but in clinical speech situations, human

intervention to identify closed glottal intervals with the

aid of an electroglottograph (EGG) is not an unrealistic

requirement. A more serious limitation is that with higher

pitch voices, the closed glottal interval contains too few

samples to permit an effective least-squares determination

of the AR coefficients. With some voice types, the vocal

folds may not even fully close, and these voice types are of

high clinical interest.









Source Models


Recent efforts to characterize the essential features

of the voicing source waveform for different male and female

voices have led to several new parametric models of glottal

output. Source models can be used to represent the glottal

flow pulse shape in a few parameters. They should model the

skewing effect quite well, and hence the smoothed glottal

flow.



a) Fant's Model (3 parameters)

This model for the glottal flow was introduced by Fant

(1979a) in support of inverse filtering studies with analog

instrumentation. It is given in Figure 3-2. In addition to

the voice fundamental frequency Fo = l/To, its basic

parameters are the peak flow Uo, the glottal frequency

Fg = Og/2x and the asymmetry factor K. The pulse may be

ascribed a starting point t = Ti. The rising branch


1
U=-Uo[l-cosWg(t-Ti) ] T < t < T2
2


reaches the peak value Uo at t=T2.

1
T2- T1 =
2Fg
















Uo





U0
2





0


Figure 3-2. Fant's model.

Ei


ti tp


1 Uo
Td= -
Td =J2K -l U(t=T3)

Closure excitation
H(s) '(t = T3) Uo
H(s) s = ST


Figure 3-3. The LF-model of differentiated glottal flow.








The falling branch


U=Uo[KcosUg(t-T2) -K+1] T2 < t < T3



hits the zero line after a time

1 K-1
T3 T2 =--cos-1 ()-
Wg K


Providing K > 0.5 the termination is abrupt with a slope

I dU 2
U3 = = Uo g K-
dt (t-T3)


If K > 1 this is the maximum slope during the course of the

falling branch. For 0.5 < K < 1 the maximum slope occurs

prior to closure. At K = 0.5 the falling branch is

symmetrical to the rising branch. This is the lower bound

of K in the present use of the model and represents a lowest

degree of excitation strength. The obvious shortcoming of a

model with abrupt flow termination is that it does not allow

for an incomplete closure or for a residual phase of

progressing closure after the major discontinuity.



b) LF-Model (4 parameters)

The properties of the LF-model, which is shown in

Figure 3-3, have been fully described in Fant et al.

(1985a). The four parameters are used to model the

differentiated flow rather than the real glottal flow. The

differentiated flow is commonly used in speech synthesis,








and includes the effect of radiation at the lips. The model

consists of two parts. The first part is an exponentially

growing sinusoid to which three of the four parameters of

the model pertain. This segment is


dU (t)
g =E (t) = Eo e sinogt to < t < te
dt



modeling the flow from glottal opening until the main

excitation occurs (the moment of maximum discontinuity in

the glottal airflow function, which normally coincides with

the moment of maximum negative flow derivative). As opposed

to most other models of glottal flow, the LF-model is a

continuous function until the main excitation, and therefore

does not introduce additional excitations. In comparison,

Fant's model is composed of two different segments; a rising

branch up to maximum flow and a falling branch down to

complete closure. The discontinuity between the two

segments introduces a secondary weak excitation at the flow

peak.

The three parameters pertaining to the first segment

of the LF-model are

(1) Eo which is merely a scale factor.

(2) a = -BX where B is the "negative bandwidth" of the

exponentially growing amplitude.

(3) )g = 27Fg where Fg = 1/2tp and tp is the rising-time (the

time from glottal opening to maximum flow).








The second part of the model is an exponential segment

that allows a residual flow (dynamic leakage) after the main

discontinuity, at time te, when the vocal folds close. The

segment used for this "return phase" is



E (t) = -[e-'(t-t) -e -(tc-t)] t < t < tc
eta


where ta is the fourth parameter of the model. The

parameter ta is the time constant of the exponential curve

and is determined by the projection on the time axis of the

derivative at time te. The parameter e can iteratively be

determined from



ta = 1 e-' (tc-t,)



and for small values of ta, Eis approximately equal to 1/ta.

Ee is the negative amplitude of the excitation spike and tc

is the moment when complete closure is reached.

The effect of the return phase on the source spectrum

is, due to its exponential waveshape, approximately a first

order low-pass filter with a cutoff frequency Fa = 1/(27ta).

This means that the longer the return phase, the lower the

cutoff frequency, and the larger the high frequency

reduction.

By convention tc = to, the time of glottal opening for

the forth-coming pulse period. This implies that the model









lacks a closed phase. In practice this is no drawback: for

normal (small) values of ta, the exponential curve will fit

closely to the zero line, providing,. for all extents and

purposes, a closed phase. The lesser number of parameters

makes the implementation of the model simpler.

Apart from the four parameters, there is a requirement

of area balance,


fT.
E(t) =0



which keeps the zero flow line from drifting.

Other glottal source models have also been developed.

An evaluation of some source models was given in Fujisaki

and Ljungqvist (1986).















CHAPTER 4
IMPLEMENTATION AND RESULTS



Introduction


In this chapter, we first describe how the data used

in our experiments are collected. Then, the implementation

of the proposed speech production model is described in

detail. The method to correct the distorted speech signals

is given next. The glottal flow waveforms obtained from

inverse filtering corrected sustained vowel signals are then

presented. Modeled glottal flow waveforms using the

LF-model and the corresponding synthesized signals which do

not include the source-tract interaction ripple effects are

then shown. Synthesized signals which include the ripple

effects by using different vocal tract filters during the

glottal open and closed phases are also to be presented.


Experimental Data Base


The procedure for collecting the data used in our

experiments is given as follows. Each subject was seated

inside an Industrial Acoustics Company (IAC) single-wall

sound room. An Electro-Voice RE-10 dynamic cardiod

microphone was located at a fixed distance of 6 inches from

the speaker's lips. The speech and electroglottographic








(EGG) signals were collected simultaneously. The

electroglottograph was a Synchrovoice Inc. model. The

speech and EGG data were amplified prior to digitization by

a Digital Sound Corporation DSC-240 audio control console.

The two data channels were directly digitized at a sampling

frequency of 10 kHz per channel by a Digital Sound

Corporation DSC-200 system with 16-bit precision. Both

channels were bandlimited to 5 kHz by passive elliptic

filters with a minimum stopband attenuation of -55 dB and a

passband ripple of 0.2 dB.

In addition, some speech data were collected with a

Bruel & Kjaer (B&K) model 4133 condenser microphone. In

addition, twelve sustained vowels were collected

simultaneously without EGG using both the Electro-Voice and

B&K microphones.

The B&K 4133 condenser microphone has a good

low-frequency response. Its amplitude response is within

1 dB down to 20 Hz, and its phase response is essentially

linear. The -3 dB low-frequency cut-off is around 10 Hz.

This feature is required when the speech signal is used for

glottal source estimation, since the glottal source

waveform, which is to be estimated, has its major energy

components at low frequencies (dc to 1 kHz). However, this

microphone characteristic also makes the B&K 4133 condenser

microphone sensitive to low-frequency breath and ambient

noise, which may cause problems in speech analysis.

Therefore, the Electro-Voice RE-10 microphone was used to








collect most of the speech data. This microphone has a good

frequency response at frequencies above 50 Hz.


Implementation of Proposed Speech Production Model


The proposed speech production model, which includes

source-tract interaction has been implemented as an

analysis/synthesis system. The analysis program extracts

the model parameters from both the speech and EGG signals;

the synthesis program uses the extracted parameters to

recreate the original speech signal. Since we are only

interested in the voiced portions of the speech signal,

which can be determined from the differentiated EGG signals,

unvoiced portions of the speech signal are not analyzed and

are copied directly from the original speech signal analyzed

during synthesis. The analysis of the voiced speech

segments is pitch synchronous. Speech signals are not

pre-emphasized before analysis.

The analysis program stores the differentiated glottal

flow and glottal flow signals, as well as a feature file,

which contains for each frame, the starting point of the

frame, the frame type, and the frame length. For voiced

frames, the following are stored: closed phase covariance

linear prediction coefficients, the instant of glottal

opening, the location of glottal flow peak, and the location

and magnitude of the negative minimum of the differentiated

glottal flow. The synthesis program uses the parameters in

the feature file, as well as the glottal flow, to generate a








modeled glottal flow signal which is then used to synthesize

the original speech signal using the linear prediction

coefficients in the feature file. If the same vocal tract

filter is used in both the open and closed phases, the

resulting synthesized speech will not include the ripple

effects, but ripple effects can be approximated by using a

different vocal tract filter during the open phase which has

a larger first formant bandwidth than the closed phase vocal

tract filter.

Voiced and unvoiced segments in the speech signal are

determined from the differentiated EGG signal. It is known

that voiced sounds have large negative minima in the

differentiated EGG corresponding to the instants of closure,

so a negative threshold is used to locate these minima.

Voicing is considered to start when two consecutive minima

less than the threshold are found, and the duration between

these minima gives rise to a frequency which is within the

normal pitch frequency range of the talker. A range of 50

Hz to 400 Hz is used. Voicing is considered to stop when

the above condition is no longer met. Since we used pitch

synchronous analysis, the frame size is a pitch period. In

order that the LF-model can be fitted to the differentiated

glottal flow, the pitch period is chosen to start at the

instant of glottal opening, and end at the next instant of

glottal opening. The instant of glottal opening is

determined as the location of the maximum between two minima

in the differentiated EGG. To accommodate for error in the








location of the instant of glottal opening, the starting

point of a frame is actually a few points in front of the

instant of opening found. The region between a minimum

which corresponds to the instant of closure and the next

maximum of a differentiated EGG is considered as the closed

phase. To allow for possible errors in the identification

of such minima, the closed phase region is shortened by 3

points at the closure and 5 points at the opening.

We have assumed that there will be a closed glottal

interval of sufficient duration to perform a closed phase

covariance LPC analysis over the closed phases, which are

determined from the differentiated EGG. A time lag of 0.9

msec (9 points for 10 kHz sampling rate) for the acoustic

propagation delay from the glottis to the microphone is

applied to the EGG signal when it is compared with the

speech signal. If the closed phase regions are short, the

LPC analysis may not have enough data samples to be

accurate. For very short closed phases, as is often the

case for female voices, the LPC analysis cannot be applied.

If there are no closed phases, as in breathy voices, but

regions of sufficient duration are mistakenly determined as

a closed phase from the differentiated EGG, the glottal flow

waveforms obtained from inverse filtering may not be

accurate. However, such waveforms may still give a general

idea of what the actual glottal flow waveforms may appear

as.








The default linear prediction order is 12, and the

default region of minimization is 28 samples, which combine

to give a window size of 40 samples. These parameters can

be changed interactively. They are verified to determine if

the LPC analysis window fits in the closed phase interval as

determined from the differentiated EGG; if not they are

changed by the program as necessary. The actual location of

the LPC analysis window is determined by minimizing the

total squared error. To find the inverse filter, the

formant frequencies and bandwidths of the poles are

calculated. Real poles at dc are removed, but real poles at

the sampling frequency are retained. Also, extraneous

formants may occur, such as those with very low frequencies

or very large bandwidths, and they are removed if they

distort the glottal flow waveforms. In order that the

output is stable during synthesis, poles outside the unit

circle are reflected inside the unit circle, even though

this may distort the glottal flow waveforms. However, for

good vowel data, pole reflection seldom occurs, except

possibly at the onset or offset of voicing. The inverse

filter is reconstructed from the remaining poles.

The speech signal inside a frame is inverse filtered

to obtain the differentiated glottal flow, which is then

integrated to obtain the glottal flow. In order to remove

any low-frequency trend from the glottal flow, any dc level

of the differentiated glottal flow in the frame is removed.

The analysis algorithm is summarized in Figure 4-1. The



































Finish up:
write glottal flow,
differentiated
glottal flow, and
close feature file


N (voiced)
Find open/closed
phase from FAIL?
DEGG (unv
SIY (unvoiced)


Figure 4-1. The block diagram for the analysis algorithm.








differentiated EGG is represented as DEGG in the flow chart.

The analysis assumes a normal EGG waveform.

The synthesis algorithm is given in Figure 4-2. The

LF-model is used because it can match the glottal flow

waveforms accurately. To ensure that the programs run

correctly, synthesized data are used to test the programs,

as described in the Appendix.


Correction of Distorted Speech Signals


The inverse filtering results for a sustained vowel

/a/ recorded from a male speaker (DMH) with the

Electro-Voice and B&K microphones are shown in Figure 4-3

and Figure 4-4, respectively. The data collected by the B&K

microphone contains low frequency noise, and was high-pass

filtered, as was the B&K data. Since the phase must be

maintained to obtain undistorted glottal flow waveforms from

inverse filtering, a linear phase high pass FIR filter was

designed with a cutoff frequency of 50 Hz. The output from

the filter was delayed to maintain the synchronization of

speech and EGG data.

The glottal flow waveforms obtained from inverse

filtering the Electro-Voice speech signals did not appear as

expected. This was caused by the slow decay to zero of the

differentiated glottal flow during the closed phase

interval. The glottal flow waveforms obtained from the B&K

data were better, but the closed phase interval was not

always apparent. This is usually because the values of the



























Write modeled glottal
flow, modeled
differentiated glottal
flow, and
synthesized speech


Figure 4-2. The block diagram for the synthesis algorithm.

































25CC r


2000
1C00

00
SIOO

-SOO
4


mi <-m.>
(a)


m (b)
(b)


1 C 1 5


(C)
(c)


15
amn (m>


Figure 4-3. Data for sustained vowel /a/ (DMH), recorded
using the Electro-Voice microphone. (a) Speech signal;
(b) Differentiated EGG; (c) Differentiated glottal flow;
(d) Glottal flow.


10


:z


k


kPWVAAj






















(a)


.mI -m<.
(b)


(c)


L-- <>
(d)

Figure 4-4. Data for sustained vowel /a/ (DMH), recorded
using B&K condenser microphone. (a) Speech signal;
(b) Differentiated EGG; (c) Differentiated glottal
flow; (d) Glottal flow.








differentiated glottal flow during the closed phase are

positive. If values of the differentiated glottal flow are

not near zero during the closed phase, the glottal flow

obtained from integrating the differentiated glottal flow

will not have a flat portion in the closed phase.

By comparing the speech data in Figure 4-3(a) and

Figure 4-4(a), we can see that the characteristics for /a/

recorded with the B&K microphone and Electro-Voice

microphone are quite different from each other, although the

data were taken from the same speaker. Hence, we conclude

that the differences in the data are caused by the different

frequency responses of the microphones, particularly the low

frequency response of the audio equipment and the

microphones.

Since we deduced that the microphone frequency

response is the main source of distortion, we determined

that a calibration of the two types of microphone is

required. Both the magnitude and phase responses are

needed, but the phase response cannot be easily obtained, so

another method was developed.

Calibration of the recording equipment, without the

microphone, with square waves was attempted to determine the

extent that the input signals are distorted. The resulting

digitized output signals for a square wave input of 100 Hz

and 200 Hz are shown in Figure 4-5. It can be seen that the

flat portion of the square wave becomes sloped. This is

thought to be caused by the low frequency distortion of the













x104
1.5


1-


0.5


0-


-0.5



-1


-1.5
0 50 100 150 200 250 300





(a)




x104
1.5


1-


0.5



0-


-0.5


-1


-1.5
0 50 100 150 200 250 300







(b)



Figure 4-5. The distorted digitized output for a square

wave input of (a) 100 Hz; (b) 200 Hz.




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'2017-08-14T14:29:06-04:00'
describe
'37336' 'info:fdaE20081130_AAAAACfileF20081130_AAACYK' 'sip-files00003.pro'
dcefefa120cbac5680503212bef17a87
a4f60f60266603f13e6337018b810a100d19c09d
'2017-08-14T14:30:04-04:00'
describe
'23420' 'info:fdaE20081130_AAAAACfileF20081130_AAACYL' 'sip-files00003.QC.jpg'
25b7b1b618f6fa486e29619b039d0d46
f3451a923db9ac4739ee29ff4913e50c012db30d
'2017-08-14T14:30:12-04:00'
describe
'6577604' 'info:fdaE20081130_AAAAACfileF20081130_AAACYM' 'sip-files00003.tif'
26f843de2eb14f46c54ced94471f9358
38e8e3ebd76339526d1fb682a6cea3f26d563523
'2017-08-14T14:31:02-04:00'
describe
'1694' 'info:fdaE20081130_AAAAACfileF20081130_AAACYN' 'sip-files00003.txt'
8a3f94a1bf9e0ebf3139d491b7b5e8b0
c6121ee41ab4017a28b7191e36671aa7ad189d69
'2017-08-14T14:31:30-04:00'
describe
'5742' 'info:fdaE20081130_AAAAACfileF20081130_AAACYO' 'sip-files00003thm.jpg'
c7b8cdfda2573b663d735be8759cb52b
a12f0bbd00b3048caf818bbf69d39aef2a435a01
'2017-08-14T14:29:02-04:00'
describe
'835101' 'info:fdaE20081130_AAAAACfileF20081130_AAACYP' 'sip-files00004.jp2'
791f276487658c181c7b310fa29a0e64
0d2153794c70c6100e2299c123ba6cfd78854d91
'2017-08-14T14:27:56-04:00'
describe
'44292' 'info:fdaE20081130_AAAAACfileF20081130_AAACYQ' 'sip-files00004.jpg'
b2e0b8c15afdc9aab24ec2bb1d7fb5c6
a5798291460e411f03f4bdb80e56dbbc34b15737
'2017-08-14T14:32:37-04:00'
describe
'23277' 'info:fdaE20081130_AAAAACfileF20081130_AAACYR' 'sip-files00004.pro'
3525d01251fcd184fe3664c9d9f276c4
9668a182506d240454938c94a908cd112c5c7d38
'2017-08-14T14:31:40-04:00'
describe
'14848' 'info:fdaE20081130_AAAAACfileF20081130_AAACYS' 'sip-files00004.QC.jpg'
c344179b3b3622f171a83e069b407b12
85579b617cbb8a40857745e93d71afff8c08622f
describe
'6699308' 'info:fdaE20081130_AAAAACfileF20081130_AAACYT' 'sip-files00004.tif'
d923f7ebd0b87e47c198e707901ecbaf
961d9c4d93c000a9057aaeac4f53fcf0f828305c
'2017-08-14T14:29:05-04:00'
describe
'991' 'info:fdaE20081130_AAAAACfileF20081130_AAACYU' 'sip-files00004.txt'
17cd67bf5b7dc9d91fdca32a28c1af04
44c12db92c19f12e213dee552608396be4aa8b31
'2017-08-14T14:31:42-04:00'
describe
'3961' 'info:fdaE20081130_AAAAACfileF20081130_AAACYV' 'sip-files00004thm.jpg'
41b5fc77a1b708c9654b2b74b961c69d
3f2e39180ba9ac55d48a3a6b0953cf53b6dda08b
'2017-08-14T14:27:20-04:00'
describe
'852557' 'info:fdaE20081130_AAAAACfileF20081130_AAACYW' 'sip-files00005.jp2'
9add3808b4d4a30f51be9b064438b0a3
8c1880e6fcf3b044ecdc8b37b97652d3b2fc2440
'2017-08-14T14:34:21-04:00'
describe
'69423' 'info:fdaE20081130_AAAAACfileF20081130_AAACYX' 'sip-files00005.jpg'
50bf9e701a73f6ab03d04a68e4fe649a
d4e77470d521491627ea8599cd120c42b6299a4e
'2017-08-14T14:33:42-04:00'
describe
'29651' 'info:fdaE20081130_AAAAACfileF20081130_AAACYY' 'sip-files00005.pro'
7aad384baa85417d1791c3a0f27203a3
e0ea41a942a73df2f2ad6ea7148cedadab99d068
'2017-08-14T14:29:32-04:00'
describe
'22098' 'info:fdaE20081130_AAAAACfileF20081130_AAACYZ' 'sip-files00005.QC.jpg'
c5f9e94addae9d937efdd3e8905229fe
e12678614b7ad8362594a9b147608ee6c3f52bf9
'2017-08-14T14:31:05-04:00'
describe
'6837320' 'info:fdaE20081130_AAAAACfileF20081130_AAACZA' 'sip-files00005.tif'
f10283e7f5fb5b476d941d34042a52b9
48387b7a77746035a3cf595c6472ed686974e4df
'2017-08-14T14:31:38-04:00'
describe
'1321' 'info:fdaE20081130_AAAAACfileF20081130_AAACZB' 'sip-files00005.txt'
948f9bb72c79db4f82f78bcae9362fbd
213ceb20a0b76988c3aa218c5c31ae4d621cf8f4
'2017-08-14T14:28:51-04:00'
describe
'5771' 'info:fdaE20081130_AAAAACfileF20081130_AAACZC' 'sip-files00005thm.jpg'
cbf41e2a6cfffa485ba7ac7dffd1828c
7ad36e7ab1af0331172823273291cc8153f819a7
'2017-08-14T14:28:09-04:00'
describe
'829595' 'info:fdaE20081130_AAAAACfileF20081130_AAACZD' 'sip-files00006.jp2'
51199858b6418011c9364f16c54299e6
7ab1d7476e2052db20cd1ab46240ee1c85d27010
'2017-08-14T14:34:19-04:00'
describe
'89045' 'info:fdaE20081130_AAAAACfileF20081130_AAACZE' 'sip-files00006.jpg'
c6019171ac28b4e6b41db9c377a1fb02
2e44f60faa306cbdd40d5a0d262e7560c1c7cf05
'2017-08-14T14:30:48-04:00'
describe
'36543' 'info:fdaE20081130_AAAAACfileF20081130_AAACZF' 'sip-files00006.pro'
02d24c5525ee61a224faf5398df42c0b
92d139c832bc2672815639e25eb802f471e8564a
'2017-08-14T14:29:38-04:00'
describe
'30240' 'info:fdaE20081130_AAAAACfileF20081130_AAACZG' 'sip-files00006.QC.jpg'
575eb6b1ba20dd73077b0f88e3f4bc0c
fd25bf92e43bd8e06f0853fd8263546f2d12c87b
'2017-08-14T14:32:52-04:00'
describe
'6655436' 'info:fdaE20081130_AAAAACfileF20081130_AAACZH' 'sip-files00006.tif'
1a99ac0b318c533d813a039722241582
da6c782df9d84c052a9306f162abe51b16339736
'2017-08-14T14:28:49-04:00'
describe
'1505' 'info:fdaE20081130_AAAAACfileF20081130_AAACZI' 'sip-files00006.txt'
97c188e5be2416dc0ca4b428e2d67182
ea9bd2a12a473135b1ed486f1549a7bfe4cc3cc8
'2017-08-14T14:31:24-04:00'
describe
'8073' 'info:fdaE20081130_AAAAACfileF20081130_AAACZJ' 'sip-files00006thm.jpg'
c3e559d8a4e5b7375248e90ba45fd2f3
113c50210bea8a9f7edde892fe9e78368bbf4d55
describe
'856137' 'info:fdaE20081130_AAAAACfileF20081130_AAACZK' 'sip-files00007.jp2'
7015c6f5c321633b4abb06b45146e8b5
ebd7b54cd0cb23d09201bee2875419094879953c
'2017-08-14T14:32:27-04:00'
describe
'75386' 'info:fdaE20081130_AAAAACfileF20081130_AAACZL' 'sip-files00007.jpg'
b715992a995d93d27c7788b75030a269
71d2846b1d4ca81bbc63b10528cbcad8df8ae10f
'2017-08-14T14:28:06-04:00'
describe
'31280' 'info:fdaE20081130_AAAAACfileF20081130_AAACZM' 'sip-files00007.pro'
67c4f78e3326666302e3f8e657da5a5a
91f5cd6718c928c452a4ea34b9dc7fb99e9e5b75
'2017-08-14T14:33:02-04:00'
describe
'25694' 'info:fdaE20081130_AAAAACfileF20081130_AAACZN' 'sip-files00007.QC.jpg'
255f744eb48c8a4b1bf7b8f48c10979f
591d1808d5c1c53084a25bcf89be1de9416eba57
'2017-08-14T14:33:16-04:00'
describe
'6865676' 'info:fdaE20081130_AAAAACfileF20081130_AAACZO' 'sip-files00007.tif'
120f420316c8f9e1e0a7c4a1945effbc
cf1889f38da9ced521e01a45fc311deb93ae2adf
'2017-08-14T14:27:23-04:00'
describe
'1336' 'info:fdaE20081130_AAAAACfileF20081130_AAACZP' 'sip-files00007.txt'
4ec224f7c6536bf01243763b6fea6983
bc269d225e3db1667ac223f5de84ae80060947d2
'2017-08-14T14:28:01-04:00'
describe
'7001' 'info:fdaE20081130_AAAAACfileF20081130_AAACZQ' 'sip-files00007thm.jpg'
06639448bcfdc0fe1e1d413fe685062f
4183cbda079d001f591bd6cdc98222e90e175dfa
'2017-08-14T14:28:34-04:00'
describe
'863718' 'info:fdaE20081130_AAAAACfileF20081130_AAACZR' 'sip-files00008.jp2'
0469cf2ba7b468c95b9fe88573fe53d3
d44f94fa1c942b3bf1a638faafef0748f2dee06d
'2017-08-14T14:32:33-04:00'
describe
'84056' 'info:fdaE20081130_AAAAACfileF20081130_AAACZS' 'sip-files00008.jpg'
15600df4ab8e570a20a816b8d5bf36c5
c77ea18e554ef64ad25ea5a24839a4aef81a54ec
describe
'35894' 'info:fdaE20081130_AAAAACfileF20081130_AAACZT' 'sip-files00008.pro'
28362f1b43418514fe1b26e805f3f726
9289595d7e9d26509e06c1654856d2ae5a67d14d
'2017-08-14T14:33:50-04:00'
describe
'29323' 'info:fdaE20081130_AAAAACfileF20081130_AAACZU' 'sip-files00008.QC.jpg'
0d55afad9ed5e9b2415034e14943c63f
1d4f69e26ca58e80166ce53213715f5ea26f5f84
'2017-08-14T14:33:11-04:00'
describe
'6926064' 'info:fdaE20081130_AAAAACfileF20081130_AAACZV' 'sip-files00008.tif'
5823ea7121b27727dfabde907c6347cf
522f7c4e506d7eb1ac5fbdb7348a5b56a0327120
'2017-08-14T14:31:16-04:00'
describe
'1498' 'info:fdaE20081130_AAAAACfileF20081130_AAACZW' 'sip-files00008.txt'
dec20bd9401dbd1ccc265178cdf913a2
1ed696ba4dc1776542db62674b7f79661114b840
'2017-08-14T14:34:13-04:00'
describe
'7858' 'info:fdaE20081130_AAAAACfileF20081130_AAACZX' 'sip-files00008thm.jpg'
5692a9535782ee3577379cf955fad1ce
ae96ab2e5aec26e65b5f92307d50e29ce41f425c
'2017-08-14T14:30:34-04:00'
describe
'906276' 'info:fdaE20081130_AAAAACfileF20081130_AAACZY' 'sip-files00009.jp2'
8e4726c6f81713dfacec6514151cbc41
5f856e6ad861fa656659805cef8addaede27f7bf
'2017-08-14T14:30:26-04:00'
describe
'85190' 'info:fdaE20081130_AAAAACfileF20081130_AAACZZ' 'sip-files00009.jpg'
afc8b1d83b9bf110e8899f5fc9138b45
30668648a8c16846908cac1c05d04a2212441412
'2017-08-14T14:34:00-04:00'
describe
'38397' 'info:fdaE20081130_AAAAACfileF20081130_AAADAA' 'sip-files00009.pro'
8e53435ef181bc12031b4912486929ec
8f6e8b025489dd239aac0c02e452e5d324f52a00
'2017-08-14T14:29:29-04:00'
describe
'29100' 'info:fdaE20081130_AAAAACfileF20081130_AAADAB' 'sip-files00009.QC.jpg'
636d2b1edee7773d94f0aa2ee1692ccd
5aebcb23db8c2ddd572c9947968f53c5295c4176
describe
'7266656' 'info:fdaE20081130_AAAAACfileF20081130_AAADAC' 'sip-files00009.tif'
4e83629d502274d2500e83b1173c36bd
b64a884caf74418e5934dcb7b9c031d1bf00d5a8
'2017-08-14T14:30:19-04:00'
describe
'1590' 'info:fdaE20081130_AAAAACfileF20081130_AAADAD' 'sip-files00009.txt'
69a78bae0a251dde25ada3ad26b78e1e
87380559e006fafb76a7f8f8a0d73fb7d32a70cd
'2017-08-14T14:32:39-04:00'
describe
'7558' 'info:fdaE20081130_AAAAACfileF20081130_AAADAE' 'sip-files00009thm.jpg'
211651e7efa0f26551abdc93d073ff70
bc094f3a6fbc3a369e6759b92d3daa412701bc00
'2017-08-14T14:32:23-04:00'
describe
'840675' 'info:fdaE20081130_AAAAACfileF20081130_AAADAF' 'sip-files00010.jp2'
40739c4ae4f33f1375e1f7567d1cacf4
01e8ebaac45694a8ed62e2fa0b895ca93b9c2257
'2017-08-14T14:28:05-04:00'
describe
'81432' 'info:fdaE20081130_AAAAACfileF20081130_AAADAG' 'sip-files00010.jpg'
e86ff5364f7401e20bcb48ca2a989624
33b7d60aad3eea4b7970237d79021c53b4ccabdf
'2017-08-14T14:30:00-04:00'
describe
'34171' 'info:fdaE20081130_AAAAACfileF20081130_AAADAH' 'sip-files00010.pro'
c10b760217907bee8a3d7dd4a5bdbccf
9168316a2abd558531e7588497a8a835727b2b84
'2017-08-14T14:32:45-04:00'
describe
'28042' 'info:fdaE20081130_AAAAACfileF20081130_AAADAI' 'sip-files00010.QC.jpg'
cc2e7337203942cd209cb9630ebee787
fdb36a4b100a240fe0bbf1360e4f952d26a47944
'2017-08-14T14:34:15-04:00'
describe
'6742040' 'info:fdaE20081130_AAAAACfileF20081130_AAADAJ' 'sip-files00010.tif'
9c3605e873f7edeab8870d2141d1e44c
0ea2992454924f7309e544b36b53639eab3e4bb6
'2017-08-14T14:27:47-04:00'
describe
'1442' 'info:fdaE20081130_AAAAACfileF20081130_AAADAK' 'sip-files00010.txt'
b79bd54afa8658ad142bb243656d9379
41b94d55417703d920b8da45313d84ff5d93887c
'2017-08-14T14:29:12-04:00'
describe
'7567' 'info:fdaE20081130_AAAAACfileF20081130_AAADAL' 'sip-files00010thm.jpg'
2ccdda4719c07454754a0ae49a2c9435
15f6fd00eba346247b034e44f48ded09de891ae2
'2017-08-14T14:33:59-04:00'
describe
'1074236' 'info:fdaE20081130_AAAAACfileF20081130_AAADAM' 'sip-files00011.jp2'
6067e34e486b454d71cbdd6d4ee9366e
8221a94de69de29c51a9d545a12c97e816136bfa
describe
'24532' 'info:fdaE20081130_AAAAACfileF20081130_AAADAN' 'sip-files00011.jpg'
493ce4598d8c549f98d9429b71aac34f
1153e5b8f501c18f2dcdbf9d12dc530d1830e212
'2017-08-14T14:28:12-04:00'
describe
'4692' 'info:fdaE20081130_AAAAACfileF20081130_AAADAO' 'sip-files00011.pro'
600c707e9073acb376871a5b32ed3f93
5fa1ad9e9e90cb350c49e2b11c3c0a64df631494
'2017-08-14T14:30:33-04:00'
describe
'7521' 'info:fdaE20081130_AAAAACfileF20081130_AAADAP' 'sip-files00011.QC.jpg'
8e2c59e5888aee162682357cce4cdf65
a61b6e54a2d4993a4e535cd16b32279f0bb55bcf
'2017-08-14T14:29:55-04:00'
describe
'8610988' 'info:fdaE20081130_AAAAACfileF20081130_AAADAQ' 'sip-files00011.tif'
edf53471eaf2f7168e7f378f1d56fd16
723447789441153a29535e10bea243591c20b395
'2017-08-14T14:33:45-04:00'
describe
'218' 'info:fdaE20081130_AAAAACfileF20081130_AAADAR' 'sip-files00011.txt'
952933e98f858a750b2a96a6f8055677
dd9addb86b6ecf34ff4cb08348f2c51a30537b58
'2017-08-14T14:28:48-04:00'
describe
'2438' 'info:fdaE20081130_AAAAACfileF20081130_AAADAS' 'sip-files00011thm.jpg'
dec83e32cfaa9fb57cc2d6a89a0b7ecd
e6188943445121f60d2165e239a853b6da6ed386
'2017-08-14T14:32:55-04:00'
describe
'970028' 'info:fdaE20081130_AAAAACfileF20081130_AAADAT' 'sip-files00012.jp2'
1ea9bc9bde4b71b86bf2338b0dd6ce47
810df5e81446e420bdbf6e1f09ff0f8eedce7794
'2017-08-14T14:31:17-04:00'
describe
'80886' 'info:fdaE20081130_AAAAACfileF20081130_AAADAU' 'sip-files00012.jpg'
57dc688c2a27eefc43df893924ac7e1a
cfd289f30f3cb0a524c4d7c56201561b9b8bffcd
'2017-08-14T14:31:23-04:00'
describe
'39987' 'info:fdaE20081130_AAAAACfileF20081130_AAADAV' 'sip-files00012.pro'
6d1ccea91dd927cd6d0c04240c44d22f
66c295809ba5b43d3082ea95c24b3a1b7a45adae
'2017-08-14T14:34:44-04:00'
describe
'26913' 'info:fdaE20081130_AAAAACfileF20081130_AAADAW' 'sip-files00012.QC.jpg'
c8252157e9ee3414df168730d491df0c
f4097d2429692b69137b04702eaaaa95ecb3ea37
'2017-08-14T14:27:53-04:00'
describe
'7781616' 'info:fdaE20081130_AAAAACfileF20081130_AAADAX' 'sip-files00012.tif'
2f48e26a2f0c26c25c023a45024cd969
91a011aa295e6925141a89ebf8adbb1c257fc74f
describe
'1630' 'info:fdaE20081130_AAAAACfileF20081130_AAADAY' 'sip-files00012.txt'
1fa65232ca35b9260a7f9b31bf7c42ac
26df08b0b902b2a632e2f5c3d3a64d0908c15cfd
'2017-08-14T14:27:52-04:00'
describe
'6929' 'info:fdaE20081130_AAAAACfileF20081130_AAADAZ' 'sip-files00012thm.jpg'
970d80b761a268e690f6646f49ab811c
a1bf4fc89167977204a2c5a3f3f416b73bd59a88
'2017-08-14T14:29:41-04:00'
describe
'970027' 'info:fdaE20081130_AAAAACfileF20081130_AAADBA' 'sip-files00013.jp2'
80bde61f910ec0f6d01bf3f28dbe83cc
c85e03204f376df839d348cadd87b5a68346360f
'2017-08-14T14:28:32-04:00'
describe
'80256' 'info:fdaE20081130_AAAAACfileF20081130_AAADBB' 'sip-files00013.jpg'
5ddbbe6d90d1a2545bcd3fb0dcf7be39
e9802828f628f24de90165050e0c7611b4330760
describe
'39754' 'info:fdaE20081130_AAAAACfileF20081130_AAADBC' 'sip-files00013.pro'
ca039262888cb6aa579859a8d6ceeae1
a8db494809e48b83240e54b6a904a9b836de1ff8
'2017-08-14T14:32:02-04:00'
describe
'26449' 'info:fdaE20081130_AAAAACfileF20081130_AAADBD' 'sip-files00013.QC.jpg'
7b65f8ec9fa37dd84bc282dcee5dab06
bae85983d5b90c51fddf6251ae12f8f2b733d1b7
'2017-08-14T14:27:38-04:00'
describe
'7776572' 'info:fdaE20081130_AAAAACfileF20081130_AAADBE' 'sip-files00013.tif'
9d210e267df32fd08cc8e70bad586e32
11bcb49b9a09465e22aa37d12c17c267dc30cb17
'2017-08-14T14:31:20-04:00'
describe
'1620' 'info:fdaE20081130_AAAAACfileF20081130_AAADBF' 'sip-files00013.txt'
2a279ce88955ccf027be6d224de99195
296dea2f483bd856137f5aa37334cb1c9f51a004
'2017-08-14T14:30:44-04:00'
describe
'6578' 'info:fdaE20081130_AAAAACfileF20081130_AAADBG' 'sip-files00013thm.jpg'
2f5f7d15b69b240d3d632ebd491ce04a
383aae27c921d644a2a17854bda090b6be0cdfd5
'2017-08-14T14:30:22-04:00'
describe
'970017' 'info:fdaE20081130_AAAAACfileF20081130_AAADBH' 'sip-files00014.jp2'
68cb0d502d031477cce7be0c8d2a0530
0e1bfa751fb5e1137e12ffde8825decabc09db5d
'2017-08-14T14:28:07-04:00'
describe
'78812' 'info:fdaE20081130_AAAAACfileF20081130_AAADBI' 'sip-files00014.jpg'
e3d53c01388c1073adc86b6fe80a69c7
9bd86b0322536a6b26f038ba6d96c091d1d1d4a8
describe
'38925' 'info:fdaE20081130_AAAAACfileF20081130_AAADBJ' 'sip-files00014.pro'
f9c2a1c65ef8ba5619248379084cda57
cb9266b0b1dda0138d299bce267313de4b8304bc
describe
'26072' 'info:fdaE20081130_AAAAACfileF20081130_AAADBK' 'sip-files00014.QC.jpg'
d8aeebb9f4cdc68347dc03fd88270e2e
a1fdeab6d05b99ebb510913cc6f8d763dc96c238
'2017-08-14T14:32:15-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADBL' 'sip-files00014.tif'
51ef97f44448bcb54140c070eaf527d7
4bdd7f2456ac605731046d6eac7a837ea72be5d0
'2017-08-14T14:32:56-04:00'
describe
'1586' 'info:fdaE20081130_AAAAACfileF20081130_AAADBM' 'sip-files00014.txt'
3ce564d1fc53421b8ee43beb2bf5e49d
55f430e9d1b4f2f057cd903bd50ae7172283b61f
'2017-08-14T14:29:14-04:00'
describe
'6925' 'info:fdaE20081130_AAAAACfileF20081130_AAADBN' 'sip-files00014thm.jpg'
f6e31a5947ed8efc275b6ed3b850cb69
38a42aca15db1a0f111b2ddb12ea4695ed1add47
'2017-08-14T14:29:04-04:00'
describe
'970025' 'info:fdaE20081130_AAAAACfileF20081130_AAADBO' 'sip-files00015.jp2'
496b4451d1c5e53de66e1381893aa4b1
eaab7d363918be70225c3dc87dc607ae59285b87
'2017-08-14T14:33:26-04:00'
describe
'75756' 'info:fdaE20081130_AAAAACfileF20081130_AAADBP' 'sip-files00015.jpg'
b0c7c38df5b21104a755057518e290ef
b6808bc252c219d5854f7223a42310d7505edf0f
'2017-08-14T14:32:48-04:00'
describe
'37179' 'info:fdaE20081130_AAAAACfileF20081130_AAADBQ' 'sip-files00015.pro'
da19057c74098932aacfb52bfaa45620
33a573c5afa77e64f4c9bfe51fb3dedf4632e1c3
describe
'25181' 'info:fdaE20081130_AAAAACfileF20081130_AAADBR' 'sip-files00015.QC.jpg'
987198c83819a8c2d30562bbd603b564
c2ffbe65391241b9e503348ee603ffe817a80caa
'2017-08-14T14:32:36-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADBS' 'sip-files00015.tif'
670e6147d40b013c83921550f14c6484
41fd690f223e8f8a022a4ed19e3b872ded6885cd
'2017-08-14T14:32:46-04:00'
describe
'1523' 'info:fdaE20081130_AAAAACfileF20081130_AAADBT' 'sip-files00015.txt'
9a3268014b54f8f845d1ee020813c1e7
3696430a45460d710b3e12c295c95cedb7ec792f
describe
'6775' 'info:fdaE20081130_AAAAACfileF20081130_AAADBU' 'sip-files00015thm.jpg'
f4e59f64e62f8a9e48a73c5cfe6a3c21
7f0477976e91b9b2565cc4205e5b7965e4c75fa6
'2017-08-14T14:32:30-04:00'
describe
'970033' 'info:fdaE20081130_AAAAACfileF20081130_AAADBV' 'sip-files00016.jp2'
03a490e1eb7e73c42b64428de38d2026
a709368ddfa8846c5b30b1a6d66393582fe108e9
'2017-08-14T14:33:38-04:00'
describe
'76750' 'info:fdaE20081130_AAAAACfileF20081130_AAADBW' 'sip-files00016.jpg'
fe43bb4c6c2c5de04d90bc81f8c540c4
8ba1d603b384e7dd0abbedc6abd7e3c3ac5af226
'2017-08-14T14:32:32-04:00'
describe
'37650' 'info:fdaE20081130_AAAAACfileF20081130_AAADBX' 'sip-files00016.pro'
5110fceff3f765df10d392a6fb53d756
c93144a295573be895c080ee696960d03610b19d
'2017-08-14T14:32:08-04:00'
describe
'25428' 'info:fdaE20081130_AAAAACfileF20081130_AAADBY' 'sip-files00016.QC.jpg'
17cf33ea624ffdcd1af11a7728d1fb56
ad02b563642257475b0e90370b5e7b9a5746eca5
'2017-08-14T14:28:50-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADBZ' 'sip-files00016.tif'
bc906dab67c7c0ab69d418c3c4004434
3b7d528ea1ccce9d6be24135de5285ac700e9a74
'2017-08-14T14:31:19-04:00'
describe
'1556' 'info:fdaE20081130_AAAAACfileF20081130_AAADCA' 'sip-files00016.txt'
8de6073c8b423867e25db1d00a48f356
aea5613a6fea212e99d963b33efcf7ccfe782f1d
'2017-08-14T14:34:18-04:00'
describe
'6467' 'info:fdaE20081130_AAAAACfileF20081130_AAADCB' 'sip-files00016thm.jpg'
4bfe8170a082c66d7a29b60c59b6101b
e9d55a911ffd9ce85421a47312647fe41ca66224
describe
'969994' 'info:fdaE20081130_AAAAACfileF20081130_AAADCC' 'sip-files00017.jp2'
ebafde951651c26527b8fd70cd675d3d
5cb20fbac5c4529a566c8cd7552519d41cd11221
'2017-08-14T14:33:28-04:00'
describe
'77777' 'info:fdaE20081130_AAAAACfileF20081130_AAADCD' 'sip-files00017.jpg'
00eb3450e6d94f130ff86dd10320501a
141b6b6aa4e37d6474d6fb39bc64fa536c5f3550
describe
'38811' 'info:fdaE20081130_AAAAACfileF20081130_AAADCE' 'sip-files00017.pro'
b4e2a9e6f9932a1849e3bb53e663afa3
854af7f72ded92896c192177745c1ea59a040e9c
describe
'26245' 'info:fdaE20081130_AAAAACfileF20081130_AAADCF' 'sip-files00017.QC.jpg'
15be3c800d326df8aa092b8f13cd35f4
6c980cc78a4a14e8223ebe410370bc68e00fb117
'2017-08-14T14:27:27-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADCG' 'sip-files00017.tif'
1fc14c3e2c0d2a6674339c23d2282263
1b6a9f2ae5c139ca279bc7558d298ac0518ed19b
describe
'1576' 'info:fdaE20081130_AAAAACfileF20081130_AAADCH' 'sip-files00017.txt'
0089ad89a93d78142b001c9ad26e32cf
3f107a6e0373fee8db733159bee10abc6cae5e52
'2017-08-14T14:30:49-04:00'
describe
'6720' 'info:fdaE20081130_AAAAACfileF20081130_AAADCI' 'sip-files00017thm.jpg'
bfa3b3e265df633cb7a0bea526e0559f
99ca88e515aceaeac6806259a474412dd5132a28
'2017-08-14T14:33:53-04:00'
describe
'970031' 'info:fdaE20081130_AAAAACfileF20081130_AAADCJ' 'sip-files00018.jp2'
a318c5a4a616fa017f7ab4b748f6a6aa
0afcd6b43d53bc3c67a1ba0abecf8c700553eed6
'2017-08-14T14:33:03-04:00'
describe
'79361' 'info:fdaE20081130_AAAAACfileF20081130_AAADCK' 'sip-files00018.jpg'
b83330501a9010c9694f04650fad3a58
9762cb5a78733e029faaa29d7248c2e226b0dc6f
'2017-08-14T14:31:41-04:00'
describe
'39366' 'info:fdaE20081130_AAAAACfileF20081130_AAADCL' 'sip-files00018.pro'
6e80a7e3ba48bab43c446d057e228255
83edbb4ebe7c45044f3d45b39bc7a9d9f32a3ce3
'2017-08-14T14:30:03-04:00'
describe
'26647' 'info:fdaE20081130_AAAAACfileF20081130_AAADCM' 'sip-files00018.QC.jpg'
3e7bf627fdee49ba40c57d4a49a00739
fb14d9bcc7797fd4f37f119d296778f1c6cb908d
'2017-08-14T14:27:37-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADCN' 'sip-files00018.tif'
522cabb5ad7d7bef1bedb7b21cedc4ef
d9c71991990d9b85247a98203447b92f28674215
'2017-08-14T14:30:37-04:00'
describe
'1613' 'info:fdaE20081130_AAAAACfileF20081130_AAADCO' 'sip-files00018.txt'
d037b0a1cbe5eab298eccd291dbbd21b
82b536ed2c7d6c4c5c6f7481c0999c28fab839b2
'2017-08-14T14:33:22-04:00'
describe
'6557' 'info:fdaE20081130_AAAAACfileF20081130_AAADCP' 'sip-files00018thm.jpg'
40a87b233ba9bff62a1f778b069675c7
4f37c6f62784c514e5b970810151eed55f791428
'2017-08-14T14:34:09-04:00'
describe
'970026' 'info:fdaE20081130_AAAAACfileF20081130_AAADCQ' 'sip-files00019.jp2'
b8fdf88289be66cf4cae2d3d0b8bf491
a510be273a2777936dc93f155bc603715bf9aa57
describe
'80759' 'info:fdaE20081130_AAAAACfileF20081130_AAADCR' 'sip-files00019.jpg'
4981f2d5333ed987cd2b243376aa83bd
54552932aeb091a8e3c365af103981e922367563
'2017-08-14T14:34:16-04:00'
describe
'41249' 'info:fdaE20081130_AAAAACfileF20081130_AAADCS' 'sip-files00019.pro'
395eb2f298782b4aac535296e3df0152
e61b4b9981ba950c3b3087fe986ede2e5ae597eb
describe
'27215' 'info:fdaE20081130_AAAAACfileF20081130_AAADCT' 'sip-files00019.QC.jpg'
31eef528b62090b24800031029e61fb3
7a19b955c89355260bc71a074e5781a946f84d23
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADCU' 'sip-files00019.tif'
4ab432191e5c4c87a51a8ada23c78094
c64879ecd0f03475830eaf0a17eb859ae29bbf57
'2017-08-14T14:28:47-04:00'
describe
'1662' 'info:fdaE20081130_AAAAACfileF20081130_AAADCV' 'sip-files00019.txt'
299a678c1a50eeaf9ae28d11d7f937c5
0d6c04facb8f065bc4877a940dcbb3069b3836d2
'2017-08-14T14:29:24-04:00'
describe
'6864' 'info:fdaE20081130_AAAAACfileF20081130_AAADCW' 'sip-files00019thm.jpg'
c2715dfc581dbb863827a04a4bd505d8
e6f24dc00e8edcb547c0d3ded5ea768cad2cfa00
'2017-08-14T14:32:53-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADCX' 'sip-files00020.jp2'
e86c71767e7d9dd9d420aa8ee60c720c
fd81da1f59e6f948adbddcca437ec87c1f0c32e7
describe
'81297' 'info:fdaE20081130_AAAAACfileF20081130_AAADCY' 'sip-files00020.jpg'
ac95d9d5343e02ea9b4b8a49dbe0f6b0
12fc463e396af7894661a5bcefaf3f6852d603b7
'2017-08-14T14:34:29-04:00'
describe
'40933' 'info:fdaE20081130_AAAAACfileF20081130_AAADCZ' 'sip-files00020.pro'
b8f00f306071ef6abb4c863ff2a43f30
eb7f94bb197fff1db98efd3820333170affea479
'2017-08-14T14:32:59-04:00'
describe
'26986' 'info:fdaE20081130_AAAAACfileF20081130_AAADDA' 'sip-files00020.QC.jpg'
1b3768000775fe8893e40d69392e9dbd
68e1351543b15371c85728f623e0a8a7f2bb71b8
'2017-08-14T14:33:07-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADDB' 'sip-files00020.tif'
759e6dfed696b7f24f0564e16821906a
e84dcf44470fef68248339f95e2151bab95c0d5a
'2017-08-14T14:34:41-04:00'
describe
'1649' 'info:fdaE20081130_AAAAACfileF20081130_AAADDC' 'sip-files00020.txt'
d273862a4ac44ddf5f661a58c0e89922
07936e31ab485e79c3e491543c089d05e4a21584
'2017-08-14T14:34:32-04:00'
describe
'6897' 'info:fdaE20081130_AAAAACfileF20081130_AAADDD' 'sip-files00020thm.jpg'
2d24999f0a0eed34110abf6da689a86a
9bb95ea1f662c619c790dcc9629320af45c7e3a7
'2017-08-14T14:29:53-04:00'
describe
'970034' 'info:fdaE20081130_AAAAACfileF20081130_AAADDE' 'sip-files00021.jp2'
a2509bcd19a39a5f748b008a18cf4f78
693ca9f25e191ab42b9234b6b05322edae725b32
'2017-08-14T14:33:39-04:00'
describe
'79108' 'info:fdaE20081130_AAAAACfileF20081130_AAADDF' 'sip-files00021.jpg'
379d846a8f4ec3b3ce8ffa624d001521
ee45802a495684d688f71eeca8f3005074bb1f46
'2017-08-14T14:28:10-04:00'
describe
'40385' 'info:fdaE20081130_AAAAACfileF20081130_AAADDG' 'sip-files00021.pro'
c0f8f8a82a849f7163e39269527456d1
e12c081a904446196504d0f69190fccae997bc14
describe
'26736' 'info:fdaE20081130_AAAAACfileF20081130_AAADDH' 'sip-files00021.QC.jpg'
5516dbd5bb7d463e401cda476a7e5e20
bcbcebe3c5a03b6c409eda235c881af0c3bfa2ef
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADDI' 'sip-files00021.tif'
119a8abb4cfaa159d220ad6369b2a4e3
3d54c4ad250a66cabf579bdd064ca2fe53ab8df1
'2017-08-14T14:30:47-04:00'
describe
'1640' 'info:fdaE20081130_AAAAACfileF20081130_AAADDJ' 'sip-files00021.txt'
b9f3f34ccef12e42598f3c268316b3e3
2bb213017d19b2607c1b3665587484e9330126e3
'2017-08-14T14:30:25-04:00'
describe
'6810' 'info:fdaE20081130_AAAAACfileF20081130_AAADDK' 'sip-files00021thm.jpg'
8df3f44d2481f442c5392a1dee5a3244
5326b5cd8d16a9df5a1042fc95e793a51d73e9a7
'2017-08-14T14:31:49-04:00'
describe
'969971' 'info:fdaE20081130_AAAAACfileF20081130_AAADDL' 'sip-files00022.jp2'
679622f04fc7aa011236ff5a67bfe8ca
fea1bc67d665a940fb1ea06701436905d612ebd4
'2017-08-14T14:28:08-04:00'
describe
'80034' 'info:fdaE20081130_AAAAACfileF20081130_AAADDM' 'sip-files00022.jpg'
c7f727b023893aa1d2aa6433553ff222
e540f78fe6ecad2ce1d4aa56476b1f60c206e0cd
'2017-08-14T14:32:31-04:00'
describe
'39544' 'info:fdaE20081130_AAAAACfileF20081130_AAADDN' 'sip-files00022.pro'
d18bb461b02ef9e6e5e5d02706c9d9a7
427940f1b4008b72511c379686c6222f725f0346
'2017-08-14T14:34:20-04:00'
describe
'27117' 'info:fdaE20081130_AAAAACfileF20081130_AAADDO' 'sip-files00022.QC.jpg'
10e60a12f7a0edf3ef2d6a9a64a15426
26049afb1448816da5a79c615dc6026747a9c4eb
'2017-08-14T14:28:58-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADDP' 'sip-files00022.tif'
a54d07af5218d2b12e1b4721fb793406
cb45e65b1ba14ca23ef14b65ce61f6b12623b73d
'2017-08-14T14:27:11-04:00'
describe
'1589' 'info:fdaE20081130_AAAAACfileF20081130_AAADDQ' 'sip-files00022.txt'
1b93a7e272fb84e611297b2fddcba216
78eef55c9022be911eede490c690302770f09274
describe
'6718' 'info:fdaE20081130_AAAAACfileF20081130_AAADDR' 'sip-files00022thm.jpg'
353c9369b18f66f39d9df8e62c9b084f
771044161afac31f3455b7f779680ea1fb21ccbb
'2017-08-14T14:31:03-04:00'
describe
'970002' 'info:fdaE20081130_AAAAACfileF20081130_AAADDS' 'sip-files00023.jp2'
706991f5c64d1cf5dedaeafc9fc61a97
39c3cb00dbf8da8d090358709dce47e33f01bd96
'2017-08-14T14:29:43-04:00'
describe
'43856' 'info:fdaE20081130_AAAAACfileF20081130_AAADDT' 'sip-files00023.jpg'
42570ab07e4fb511394fedf5ec304f30
3d8c9ab5cd5f2d1b2ef6afba699a61bfa3747271
'2017-08-14T14:27:13-04:00'
describe
'19377' 'info:fdaE20081130_AAAAACfileF20081130_AAADDU' 'sip-files00023.pro'
44d419e5639b3d1d5a5ee9e5a263bf50
f08816d08aa1173261ad92278569e1659d4a3b7e
'2017-08-14T14:27:55-04:00'
describe
'14247' 'info:fdaE20081130_AAAAACfileF20081130_AAADDV' 'sip-files00023.QC.jpg'
9912314fd155b00a11a23289e07eb943
8e2d2bb43304c9831688dd7b1f097203ea4a85cd
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADDW' 'sip-files00023.tif'
57ba5dee3c97bd01f9d84f2fb3f74b40
3c662c62791e1e457a144b41d98c1707093d18b2
'2017-08-14T14:29:40-04:00'
describe
'803' 'info:fdaE20081130_AAAAACfileF20081130_AAADDX' 'sip-files00023.txt'
82c5675152db85cbfebe164f4d76ad48
245663e15bc5629ccbe19f914f4f97ddb0b0c1c5
'2017-08-14T14:31:22-04:00'
describe
'4027' 'info:fdaE20081130_AAAAACfileF20081130_AAADDY' 'sip-files00023thm.jpg'
17d8cd4e4b3a8018ab535eee0c1157b2
96b559a6cc9f8a0b534964007f66cc656e5e5aa1
describe
'970032' 'info:fdaE20081130_AAAAACfileF20081130_AAADDZ' 'sip-files00024.jp2'
36683df5c0418f64e05eb2ae5ac525c0
1db21d0176deec1cb1e73ca81740fa24de030bec
describe
'59094' 'info:fdaE20081130_AAAAACfileF20081130_AAADEA' 'sip-files00024.jpg'
8945c4349afda690f6665ded11f275b7
98b346c0826fa01940eb197f02ea78cfa2deecd5
describe
'28432' 'info:fdaE20081130_AAAAACfileF20081130_AAADEB' 'sip-files00024.pro'
bd23c5dae72e2eb19afcc9f4a1f03380
782eeeebc0ff4ff7387b5995441ca416d00be41d
'2017-08-14T14:31:09-04:00'
describe
'19299' 'info:fdaE20081130_AAAAACfileF20081130_AAADEC' 'sip-files00024.QC.jpg'
0864c6d9f9d78855e5993ffa9eb8de43
575578c1c1b6f097b1bb6868e184f0e87b3522da
'2017-08-14T14:31:33-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADED' 'sip-files00024.tif'
3cf99882082918d9bf063ae7f6b4d076
6e2ddb451cd8b9d330e016d7436a85736fc93ca1
'2017-08-14T14:31:34-04:00'
describe
'1286' 'info:fdaE20081130_AAAAACfileF20081130_AAADEE' 'sip-files00024.txt'
b5799ff34af7befbb80287c306e864b3
5e3f135d6b90d659995c4a5aff1be06fe7332ad2
'2017-08-14T14:28:37-04:00'
describe
'5030' 'info:fdaE20081130_AAAAACfileF20081130_AAADEF' 'sip-files00024thm.jpg'
4540c4718f8fa02cb26c3853ed152cba
2880ba41646c4c108751455ca6440ada273aa5e6
'2017-08-14T14:33:08-04:00'
describe
'969972' 'info:fdaE20081130_AAAAACfileF20081130_AAADEG' 'sip-files00025.jp2'
f68ecfbd6d7cad06fe5f4eb5d025c1c5
d20e3b51908036d9d46e3d67a63ef06bee80e241
'2017-08-14T14:30:36-04:00'
describe
'76583' 'info:fdaE20081130_AAAAACfileF20081130_AAADEH' 'sip-files00025.jpg'
6bfc4d7a783b5d6785b61d9bbeac5cdf
ed640bd8e9ea79800ed4109d8a6fb3bc0b18b6f5
'2017-08-14T14:27:41-04:00'
describe
'38485' 'info:fdaE20081130_AAAAACfileF20081130_AAADEI' 'sip-files00025.pro'
5a4eefaac1f2970d47503b06c8cdc931
32791c22dbea5af6eff7911fa4dd6183575914b6
'2017-08-14T14:32:14-04:00'
describe
'25622' 'info:fdaE20081130_AAAAACfileF20081130_AAADEJ' 'sip-files00025.QC.jpg'
2f0f350c0516adccb53864060281946f
977571ca11803bc5c07478a321939ace92e8389b
'2017-08-14T14:27:50-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADEK' 'sip-files00025.tif'
881f1248a733876f6f29ecac7cb563c4
bd382defa3d45f429e006dbe8c01623fb3ee1411
'2017-08-14T14:29:16-04:00'
describe
'1571' 'info:fdaE20081130_AAAAACfileF20081130_AAADEL' 'sip-files00025.txt'
c38de366cd16c53b8f8a137097a7d953
e5c3798d9210bc7221336fc6b2f0569ea5ace4ef
'2017-08-14T14:33:35-04:00'
describe
'6881' 'info:fdaE20081130_AAAAACfileF20081130_AAADEM' 'sip-files00025thm.jpg'
8fcc68799f19e99e6ea2594d5acee54d
1e6970c96bea42e2f66d44787a0b1aad18a2435c
describe
'1063869' 'info:fdaE20081130_AAAAACfileF20081130_AAADEN' 'sip-files00026.jp2'
a894847a49874a3fb8ed0c6207d627d6
7d80ddaeac008953a0de8100a85592aa4deedf30
'2017-08-14T14:30:31-04:00'
describe
'50276' 'info:fdaE20081130_AAAAACfileF20081130_AAADEO' 'sip-files00026.jpg'
0647decf02a2870651c9d3f39e5d0d50
68046da49368485c344f55d75811350f2e3e4d75
'2017-08-14T14:30:52-04:00'
describe
'11913' 'info:fdaE20081130_AAAAACfileF20081130_AAADEP' 'sip-files00026.pro'
a9f56a128ed9ec24a536f429f2710d11
4a09a320e0fda61abedd9e738405fa6f804b3a95
'2017-08-14T14:34:06-04:00'
describe
'16989' 'info:fdaE20081130_AAAAACfileF20081130_AAADEQ' 'sip-files00026.QC.jpg'
d3b8ce7373c0f44efd00d0c02898a58b
bd7485c6547db029479b10b179f6448813a22aa9
'2017-08-14T14:28:30-04:00'
describe
'8527372' 'info:fdaE20081130_AAAAACfileF20081130_AAADER' 'sip-files00026.tif'
a5a077b282f0a3a5c661a7aa8cd90b38
4c1256815e901468729e634d790ab529055d0b70
'2017-08-14T14:30:41-04:00'
describe
'612' 'info:fdaE20081130_AAAAACfileF20081130_AAADES' 'sip-files00026.txt'
b0baa3f3108d6d0dbf44ab1a828d6cf7
37b3954d1e9361945b2fa7992b5454eb959ae529
'2017-08-14T14:32:35-04:00'
describe
'5197' 'info:fdaE20081130_AAAAACfileF20081130_AAADET' 'sip-files00026thm.jpg'
bcd5ec0ef59635ba26ac1ec4b86d4720
7c7b0e34ac8c0323621d3ba43e3655b1c757c14a
'2017-08-14T14:29:54-04:00'
describe
'970021' 'info:fdaE20081130_AAAAACfileF20081130_AAADEU' 'sip-files00027.jp2'
0de1d1ea86de17f48093b0d0d2fccd14
3a9d48b31d77cca6cabbeef97c4559782c1293b2
describe
'75512' 'info:fdaE20081130_AAAAACfileF20081130_AAADEV' 'sip-files00027.jpg'
59790b56c64c449498c3e1f9fcae936d
36e9128d709d54e187b611f88ba18d52a23bf436
'2017-08-14T14:30:53-04:00'
describe
'37600' 'info:fdaE20081130_AAAAACfileF20081130_AAADEW' 'sip-files00027.pro'
5d516281394893d949552ae1d663b4ff
81d293739cf8558b590bdc8379475df5e8190b11
'2017-08-14T14:28:59-04:00'
describe
'25318' 'info:fdaE20081130_AAAAACfileF20081130_AAADEX' 'sip-files00027.QC.jpg'
7ea6f08e3d9d670fd62ab52b38b8f46e
db6f8ab15646f086b14785edf031f787b312c851
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADEY' 'sip-files00027.tif'
f4772c0edb03872d28d64b0d60578493
a9bb2b6d60197367ff2423805504d602cdef0d62
describe
'1536' 'info:fdaE20081130_AAAAACfileF20081130_AAADEZ' 'sip-files00027.txt'
1fab0451549501e784085546a37efdb3
62c604323f18518ba3deca9d8aa5207717b51a61
'2017-08-14T14:31:04-04:00'
describe
'6579' 'info:fdaE20081130_AAAAACfileF20081130_AAADFA' 'sip-files00027thm.jpg'
f64f9de6be9ee98c46b670c399cd7628
d1e35c3b7d52de7f4128718cc677fe1c5b50de37
describe
'1063040' 'info:fdaE20081130_AAAAACfileF20081130_AAADFB' 'sip-files00028.jp2'
38b814a5932cfff061f353b590c5a1a2
7c9cb3bf083d49c02002d36f5eed671c717f04c0
'2017-08-14T14:33:37-04:00'
describe
'33147' 'info:fdaE20081130_AAAAACfileF20081130_AAADFC' 'sip-files00028.jpg'
0aa31366b6c2a145b1c630fd1db4564a
334b6fd336e66b57833a396e7d1e8f4293d3e355
'2017-08-14T14:32:19-04:00'
describe
'5344' 'info:fdaE20081130_AAAAACfileF20081130_AAADFD' 'sip-files00028.pro'
1d7507e26ff26b4872800078a1755d7e
3bd3e9b1da85cc87c2dbe8d32ddb4a2876a28adf
'2017-08-14T14:30:45-04:00'
describe
'11168' 'info:fdaE20081130_AAAAACfileF20081130_AAADFE' 'sip-files00028.QC.jpg'
65b81900b61e56509f4835fc4c5a0809
3e93ac27513df54d64926942c9249c5375fb01d9
'2017-08-14T14:33:33-04:00'
describe
'8522248' 'info:fdaE20081130_AAAAACfileF20081130_AAADFF' 'sip-files00028.tif'
904aca2cff42a6ff718aa4fff6ac8e13
a9390204d333a0ac5dd8772de78d0baaa970fdff
'2017-08-14T14:30:16-04:00'
describe
'256' 'info:fdaE20081130_AAAAACfileF20081130_AAADFG' 'sip-files00028.txt'
03f6401e3b0735467ac839b7e421c9c1
8ebaa22888186379ec0935b97c5f7f491d6ce8eb
describe
'3536' 'info:fdaE20081130_AAAAACfileF20081130_AAADFH' 'sip-files00028thm.jpg'
ef078e86c0f4cce7536c2a58eb0a08dd
727cef85a729a5b0e5fbfc92118640db11474859
'2017-08-14T14:32:07-04:00'
describe
'970000' 'info:fdaE20081130_AAAAACfileF20081130_AAADFI' 'sip-files00029.jp2'
687d872f723fdada43e08eb2b391d426
eec8591dbbd9374c4d716417c60d59259bfce16e
describe
'77044' 'info:fdaE20081130_AAAAACfileF20081130_AAADFJ' 'sip-files00029.jpg'
e3d864c787aa38de78b6579a87004b97
1f1c3aba256b00197b7782822e4754ab8dcf22e2
'2017-08-14T14:32:16-04:00'
describe
'38556' 'info:fdaE20081130_AAAAACfileF20081130_AAADFK' 'sip-files00029.pro'
e2aa81b4491ddd8f06c95ed822f3741c
7af94c4cb6a37060afa89b88ec9d160181b0014e
'2017-08-14T14:28:33-04:00'
describe
'26288' 'info:fdaE20081130_AAAAACfileF20081130_AAADFL' 'sip-files00029.QC.jpg'
a633713ae6064eb920efd6c1c619ed18
0751da2ec04fc09d29b2aced7780e97e502118fa
'2017-08-14T14:32:50-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADFM' 'sip-files00029.tif'
d367645baa771a693576b5c790735c3e
03f5f93ce02f0e32c3b7665de9c6f888a042eb24
'2017-08-14T14:30:10-04:00'
describe
'1563' 'info:fdaE20081130_AAAAACfileF20081130_AAADFN' 'sip-files00029.txt'
1193ad136417da3668c7aa1fca0a4d18
78791934ffa52140c9ddb9b85ad5c7eafe9953e3
'2017-08-14T14:34:43-04:00'
describe
'6424' 'info:fdaE20081130_AAAAACfileF20081130_AAADFO' 'sip-files00029thm.jpg'
4c76e3af448412c9ba4a0a17ec2eda4e
4740c5e2352ce1a8555cfcaf40bafa3a63798bad
'2017-08-14T14:29:13-04:00'
describe
'969986' 'info:fdaE20081130_AAAAACfileF20081130_AAADFP' 'sip-files00030.jp2'
1f783102a50bcb9e967651240c9c35ad
ef660812d0835ce3e01dbce62e493814a80aa130
describe
'63452' 'info:fdaE20081130_AAAAACfileF20081130_AAADFQ' 'sip-files00030.jpg'
f8d488c05c061408024a5bea15fa607c
28ade2856c7c5731d77f494f0cab21b96814e58a
'2017-08-14T14:30:40-04:00'
describe
'30545' 'info:fdaE20081130_AAAAACfileF20081130_AAADFR' 'sip-files00030.pro'
b0c479e101b63b7c11131e0f272cc686
6ba9994032ba01598bead1c189e4e169f6983b55
'2017-08-14T14:31:50-04:00'
describe
'21021' 'info:fdaE20081130_AAAAACfileF20081130_AAADFS' 'sip-files00030.QC.jpg'
3c68444a678e09d0b066b3e1b1fa6a9a
8fda23c02769788c80fbd5f6b710eb80ae3d7c2a
'2017-08-14T14:33:30-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADFT' 'sip-files00030.tif'
94baf0068658c34ff46f89ac7a7995bc
1105e255c40bd341e78dfdd1d7ef4550b7f0ee0a
describe
'1283' 'info:fdaE20081130_AAAAACfileF20081130_AAADFU' 'sip-files00030.txt'
c0098b6c05fb93582286cfc6e144ceea
63a2e41f34ff4321dec3b3392de897fb6d7e2e8d
describe
'5758' 'info:fdaE20081130_AAAAACfileF20081130_AAADFV' 'sip-files00030thm.jpg'
a46a7145a806f10cba161893a3e0844e
59f4a5ecf76fbc0d3e046a3cae5e025527449472
describe
'970035' 'info:fdaE20081130_AAAAACfileF20081130_AAADFW' 'sip-files00031.jp2'
fa00682721cf8bf1185d7ce1b35b3739
20626fb28220663bd23ee4df2ce72200e2b45124
describe
'78664' 'info:fdaE20081130_AAAAACfileF20081130_AAADFX' 'sip-files00031.jpg'
f94fd9595e29640857bdb9243ed6f5e4
051aedd1f406a3c1c0da9893939eb7425b58292f
'2017-08-14T14:33:55-04:00'
describe
'39035' 'info:fdaE20081130_AAAAACfileF20081130_AAADFY' 'sip-files00031.pro'
81801fe12631ac285a97a64d426e3dd0
28a86858420f65d87df867d1268e29cb94b8f67d
'2017-08-14T14:28:11-04:00'
describe
'26677' 'info:fdaE20081130_AAAAACfileF20081130_AAADFZ' 'sip-files00031.QC.jpg'
691d9011271e5b338c5fe5a5373f5519
3d3c19a866d0b7327d1579a1c8088f3442c57280
'2017-08-14T14:32:47-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADGA' 'sip-files00031.tif'
979e7ecbf764125b0074ab72dc0f52ce
dba51d99d721c9d478c50fa47a1fbbf4ec16e74e
describe
'1591' 'info:fdaE20081130_AAAAACfileF20081130_AAADGB' 'sip-files00031.txt'
482c3d9f74b474b4facd9382fea3e559
87c8f514fe0db38f6d535c9201a911e0d3fbdc97
'2017-08-14T14:29:01-04:00'
describe
'6800' 'info:fdaE20081130_AAAAACfileF20081130_AAADGC' 'sip-files00031thm.jpg'
98a4b82429371cded064f7cefc3610ec
c00be58992073446b458298410450321cfb24c76
'2017-08-14T14:28:24-04:00'
describe
'1051922' 'info:fdaE20081130_AAAAACfileF20081130_AAADGD' 'sip-files00032.jp2'
aa7740ab12513178a441e7064fe24a42
44f7028c24d20f9dad9c4b9ed4dd98c2cefcbf1d
'2017-08-14T14:30:56-04:00'
describe
'28084' 'info:fdaE20081130_AAAAACfileF20081130_AAADGE' 'sip-files00032.jpg'
fb9c6e7143a9da5759c59f0bb6d97f86
58a3b2d8d1215f175c128479e1041e7c3549991f
'2017-08-14T14:32:58-04:00'
describe
'6892' 'info:fdaE20081130_AAAAACfileF20081130_AAADGF' 'sip-files00032.pro'
f47d408d6541103d4d88c690e85c2603
61f4d9c245a2df2a61a1835ed95c1d29ef9da08f
'2017-08-14T14:33:09-04:00'
describe
'9334' 'info:fdaE20081130_AAAAACfileF20081130_AAADGG' 'sip-files00032.QC.jpg'
9603fe7f7f731a69fc52dc34979872d7
9eca27db98bc7b9c4e1c614fe85e58109f864c9f
'2017-08-14T14:30:35-04:00'
describe
'8431956' 'info:fdaE20081130_AAAAACfileF20081130_AAADGH' 'sip-files00032.tif'
f46adf47b401326be8f7ba8089269df2
183c1e3234a1455f42f8254108556f90679fa88d
'2017-08-14T14:27:19-04:00'
describe
'341' 'info:fdaE20081130_AAAAACfileF20081130_AAADGI' 'sip-files00032.txt'
5f83062eeb315d3568244806649b19bf
e597695372ce2343fb2be732492f6c2065c0d0b4
'2017-08-14T14:27:34-04:00'
describe
'3384' 'info:fdaE20081130_AAAAACfileF20081130_AAADGJ' 'sip-files00032thm.jpg'
47f42a176072bcfbc8610b2a082ac10d
c3c81984d4e6277bb042815e5e4a6ee2ceb13258
'2017-08-14T14:30:01-04:00'
describe
'970018' 'info:fdaE20081130_AAAAACfileF20081130_AAADGK' 'sip-files00033.jp2'
17ac31c79620272eabdb940f39fadef1
f0bf3e39011e0295ab5d616d87725f612764fc51
'2017-08-14T14:33:56-04:00'
describe
'75684' 'info:fdaE20081130_AAAAACfileF20081130_AAADGL' 'sip-files00033.jpg'
68676ab9362ba0b9bf8ffb12f1cc4d0e
f2ed56e09efeb5474221d226a05515f25aec6d6a
'2017-08-14T14:33:48-04:00'
describe
'38016' 'info:fdaE20081130_AAAAACfileF20081130_AAADGM' 'sip-files00033.pro'
d4b1b875666849353ccaca65d5f1d8bd
0386004563f2958907d82f5ae976f7594778830a
describe
'25613' 'info:fdaE20081130_AAAAACfileF20081130_AAADGN' 'sip-files00033.QC.jpg'
4cd5b51ecc7d772cb2b4c3e528c9dcf1
1b6a2c3752a838789679a26f7579f770c9c5e430
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADGO' 'sip-files00033.tif'
389148ab95caf482d1ece2528624d8ba
7bf8163515f2cf6c59ad31b6857a65a566628cf8
describe
'1542' 'info:fdaE20081130_AAAAACfileF20081130_AAADGP' 'sip-files00033.txt'
15719ee068ded46d777f47e3e90e829e
973687ffbde5a6bb3b9258babaa5287b6a47a1e1
'2017-08-14T14:29:30-04:00'
describe
'6372' 'info:fdaE20081130_AAAAACfileF20081130_AAADGQ' 'sip-files00033thm.jpg'
06daaae1b61252adeee6ebee1c0d9c29
0e13fc44c8ca9f9c47a57c7aa7b19cd2d1be9996
'2017-08-14T14:30:58-04:00'
describe
'970030' 'info:fdaE20081130_AAAAACfileF20081130_AAADGR' 'sip-files00034.jp2'
ce3c72c169c37ca84436beab40c548de
d12daec970e21962e7771fd9ed8cf778b613f4aa
'2017-08-14T14:32:42-04:00'
describe
'82700' 'info:fdaE20081130_AAAAACfileF20081130_AAADGS' 'sip-files00034.jpg'
b24c83c8d59d4523f838f638700be0ee
aa39c57c7374679159d263f4ce1321779ddd85a1
'2017-08-14T14:33:25-04:00'
describe
'41061' 'info:fdaE20081130_AAAAACfileF20081130_AAADGT' 'sip-files00034.pro'
214590d914758845f9ea30e441cf33b7
0ddf60ec4bfae034d4f5f1088ef72d41e9e8185d
describe
'28180' 'info:fdaE20081130_AAAAACfileF20081130_AAADGU' 'sip-files00034.QC.jpg'
86b0e2bd84dfcabcfd04d501ccbbb949
aab8a59acf7de90a756964fc8610a5fc648e2024
'2017-08-14T14:34:03-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADGV' 'sip-files00034.tif'
574cad8b02fee0b3274b2df9db9dca9b
32a7dd69fd0082e87e01d018a9f27d47befa8569
'2017-08-14T14:27:26-04:00'
describe
'1665' 'info:fdaE20081130_AAAAACfileF20081130_AAADGW' 'sip-files00034.txt'
05bfe1ccea6b43290963e0dc53bf71b1
de15a0cb1c585a70fbed14c41a4fec64ad8c0783
'2017-08-14T14:34:26-04:00'
describe
'6819' 'info:fdaE20081130_AAAAACfileF20081130_AAADGX' 'sip-files00034thm.jpg'
425558ce7cc4dfcf1f05b1b61adab44e
51bfbabad5fb305cd42f00e6e1dfc6259ed4c4e6
'2017-08-14T14:33:54-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADGY' 'sip-files00035.jp2'
764a33661edcdc9d5fdfab32882177e7
401dea0a55e28231826661a9ab5d959e755758b9
describe
'79765' 'info:fdaE20081130_AAAAACfileF20081130_AAADGZ' 'sip-files00035.jpg'
ccf103ec79f53977402655fffe175fa9
2687deaa5c5bd390f92b393c72dd963529629780
'2017-08-14T14:31:01-04:00'
describe
'39281' 'info:fdaE20081130_AAAAACfileF20081130_AAADHA' 'sip-files00035.pro'
64db12dfd92a625b232f3e8b06ce0dab
20f209c62019c23eb095cac04f3c7f3d023210bc
'2017-08-14T14:28:27-04:00'
describe
'26911' 'info:fdaE20081130_AAAAACfileF20081130_AAADHB' 'sip-files00035.QC.jpg'
80d07cd56474b2d4b8e5c7fb9aa2d556
eaa6141e1f848d8f5db6f13eadfce32d804dc4fb
'2017-08-14T14:32:20-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADHC' 'sip-files00035.tif'
c12e40651471768147144468ea645848
a3aed355d2e4a3f77d2aa9a66a4cb528cfe79891
'2017-08-14T14:29:23-04:00'
describe
'1577' 'info:fdaE20081130_AAAAACfileF20081130_AAADHD' 'sip-files00035.txt'
67d54ef444090986f0c9d6b9f87834b6
642230f23b4fdc41b0b068e46d1774d65c7013eb
describe
'6651' 'info:fdaE20081130_AAAAACfileF20081130_AAADHE' 'sip-files00035thm.jpg'
c654e12e5b67d1aa4b4edc0665493ab9
240569342acdc66505d138d33431f69463c4038d
'2017-08-14T14:31:57-04:00'
describe
'970020' 'info:fdaE20081130_AAAAACfileF20081130_AAADHF' 'sip-files00036.jp2'
b891c005e5e751b88d3df5d5617edf57
5868edd635cae9bdae714fab24ff32ed15e72983
describe
'75609' 'info:fdaE20081130_AAAAACfileF20081130_AAADHG' 'sip-files00036.jpg'
4f914099da8f41acaa1dd367d621c3b5
acae353a6c60407d6542183d29dccbb261dc3948
describe
'36830' 'info:fdaE20081130_AAAAACfileF20081130_AAADHH' 'sip-files00036.pro'
bce65c90e056843ac1a68075ffa4571d
4c2278c9a3d40a6a731615fcfb4a9ff7c558fbc7
describe
'24823' 'info:fdaE20081130_AAAAACfileF20081130_AAADHI' 'sip-files00036.QC.jpg'
5e31297188dde0377344c496282fc57c
3ceb47549e7f0f99d07ad537e4359afc962cde32
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADHJ' 'sip-files00036.tif'
3f99a77c54dcb25c198cf735b60a60bc
2ac278bf10cef2d4299dec92c28c15b7e651068e
'2017-08-14T14:28:40-04:00'
describe
'1514' 'info:fdaE20081130_AAAAACfileF20081130_AAADHK' 'sip-files00036.txt'
072491c7e9aec828db3c20c66f550ede
ecb3f23cc77f6f81ec66184899b93077cdce6c4f
describe
'6470' 'info:fdaE20081130_AAAAACfileF20081130_AAADHL' 'sip-files00036thm.jpg'
f216a7a94111f2c552a373403b59b248
df16a125c4b45145cfc9b4ae960e1a33f3bc3323
describe
'969995' 'info:fdaE20081130_AAAAACfileF20081130_AAADHM' 'sip-files00037.jp2'
6281de7112b61c01747df9f5b4241878
2edde5175028c262fc38a230e5234aef8d1b1b08
'2017-08-14T14:30:23-04:00'
describe
'74691' 'info:fdaE20081130_AAAAACfileF20081130_AAADHN' 'sip-files00037.jpg'
c7d0f69d1b4a5593a0feee5246fbb2f3
bcf606af567a537daa1af21a7f9d6b58171369ea
describe
'36360' 'info:fdaE20081130_AAAAACfileF20081130_AAADHO' 'sip-files00037.pro'
e8e1b613102365d67048d0dff3d43d70
3fd3fa3f5f242fb329d545d588f270427512b89f
describe
'24732' 'info:fdaE20081130_AAAAACfileF20081130_AAADHP' 'sip-files00037.QC.jpg'
17e1bdee9f5472dfbedb1c5418146d55
9250b765f06508a1865d4492f9b5b393ecc299fb
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADHQ' 'sip-files00037.tif'
0218a2a25c194ee0e89b5fe1c42ea5e9
dbfd7169b2b617afeb39c56363c92e3b524dfa37
'2017-08-14T14:29:44-04:00'
describe
'1506' 'info:fdaE20081130_AAAAACfileF20081130_AAADHR' 'sip-files00037.txt'
09c0ed9eba49917983896fe4afea1618
08acb82ad042920d306bc0a739a9b5105b4462c5
describe
'6515' 'info:fdaE20081130_AAAAACfileF20081130_AAADHS' 'sip-files00037thm.jpg'
d5b03986dca5858a075c81b443e68cb6
2c20747de1af2a6b1953e45f909dd6b4da861290
'2017-08-14T14:28:43-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADHT' 'sip-files00038.jp2'
c64c163ce9bab266b007be5bb19f6a83
2c76c95e4d183b02e1a6a263db466e184eec6033
'2017-08-14T14:32:10-04:00'
describe
'81102' 'info:fdaE20081130_AAAAACfileF20081130_AAADHU' 'sip-files00038.jpg'
e8644c5242777c06e540e3ef40402459
2c094d8c7773c5dab4a880ce4ea36d22ad27cf40
describe
'41350' 'info:fdaE20081130_AAAAACfileF20081130_AAADHV' 'sip-files00038.pro'
a12278cff039db206747a9d023d892c5
aa3ba2d3f3c0707d7aa8d6fb09abc17a8d6ebd42
'2017-08-14T14:30:38-04:00'
describe
'27695' 'info:fdaE20081130_AAAAACfileF20081130_AAADHW' 'sip-files00038.QC.jpg'
b4bfd972684982f929cf358a1026e5b1
7908ae86631a06a25b1123bafb699a240dc50f76
'2017-08-14T14:30:42-04:00'
describe
'7776564' 'info:fdaE20081130_AAAAACfileF20081130_AAADHX' 'sip-files00038.tif'
f8d83758bc05427c010c077ea5a191e9
5f1514765c6b793c8931b676cf82357d05374cfb
'2017-08-14T14:33:00-04:00'
describe
'1673' 'info:fdaE20081130_AAAAACfileF20081130_AAADHY' 'sip-files00038.txt'
7a3b880c24ae85fa9307ee2fdfccee85
4d96438eaf349c449fc9902010ac5c6d38231e99
describe
'6837' 'info:fdaE20081130_AAAAACfileF20081130_AAADHZ' 'sip-files00038thm.jpg'
4bf532868ce76f22b0f15a4a096166a6
002948d9cf79837407d8059f5b634e4f9924357a
describe
'970015' 'info:fdaE20081130_AAAAACfileF20081130_AAADIA' 'sip-files00039.jp2'
ce21ec1d2f5440f51cbb8357beae7ab9
677128934b77ab3ae7b53e3a925e3c7041c0178f
'2017-08-14T14:32:13-04:00'
describe
'79227' 'info:fdaE20081130_AAAAACfileF20081130_AAADIB' 'sip-files00039.jpg'
fcb71b3af0ec34f8e438673a2120d237
78db6995a91b72fd30e9f2de9cdd55f267a73943
describe
'38969' 'info:fdaE20081130_AAAAACfileF20081130_AAADIC' 'sip-files00039.pro'
3205c8c3e759a01894ffeddf29671394
417e59162c87b4ece7464650791e9f70e5392156
describe
'26541' 'info:fdaE20081130_AAAAACfileF20081130_AAADID' 'sip-files00039.QC.jpg'
13591b01b23df20c4f7600a9a38b2ddf
c4f76c2c620e54029add6293a04b6a3876003d86
'2017-08-14T14:28:00-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADIE' 'sip-files00039.tif'
1809fc9765e5b9a7991ee634ff0a8733
37459a513a650416a117fa63c7f81400f451aa08
describe
'1595' 'info:fdaE20081130_AAAAACfileF20081130_AAADIF' 'sip-files00039.txt'
57c847ffd41078e05bbf9c45c1cd1182
0d4d11b40b6e5cb7da266ec44a372bdfd4a5e633
'2017-08-14T14:28:31-04:00'
describe
'6855' 'info:fdaE20081130_AAAAACfileF20081130_AAADIG' 'sip-files00039thm.jpg'
b56b005e88571d0caf2199298c21639a
f1d28e1b78ecc9197fe5942a920d43d50307d1db
describe
'970016' 'info:fdaE20081130_AAAAACfileF20081130_AAADIH' 'sip-files00040.jp2'
52238f26c2e975a1211e0a9eaa86e83c
454a97b5c01e8a3104e6201a514fdfcfabb04abc
'2017-08-14T14:30:14-04:00'
describe
'64467' 'info:fdaE20081130_AAAAACfileF20081130_AAADII' 'sip-files00040.jpg'
9361cdde036a8d2c84cb6503fc128e3c
374b9c27e58ff11723d07e8d627eb9c0febc6ffb
describe
'32286' 'info:fdaE20081130_AAAAACfileF20081130_AAADIJ' 'sip-files00040.pro'
80474f4494c6fe219bb60fd0ee5b50c2
8bf33878afd026f973c4c2a827a1aa0262ba2f14
'2017-08-14T14:29:39-04:00'
describe
'21799' 'info:fdaE20081130_AAAAACfileF20081130_AAADIK' 'sip-files00040.QC.jpg'
78935329736f7352e6eeaea811691070
56623280af330e20fcf23c1feda7b60c789ebc18
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADIL' 'sip-files00040.tif'
49bd6d6e99d29c58fa332e07a7127352
aa541f07da627c498ea465d9988c02caf5b2c3e7
describe
'1421' 'info:fdaE20081130_AAAAACfileF20081130_AAADIM' 'sip-files00040.txt'
40e07c336943a9e338988a7bc83fe449
29d0d8ea96b0ed0d3154434f41cbae9759ecd909
describe
'5738' 'info:fdaE20081130_AAAAACfileF20081130_AAADIN' 'sip-files00040thm.jpg'
6f20b5847565b96c4f08ef2c6668036e
2f6c16a21da1ccf295ba29153ae1541c1dbd9c8b
'2017-08-14T14:27:51-04:00'
describe
'970011' 'info:fdaE20081130_AAAAACfileF20081130_AAADIO' 'sip-files00041.jp2'
b888183f8c77f46e1cee46e6bee2ecc9
272b136e54a2d03abd239abd35d75b71687124e4
describe
'83883' 'info:fdaE20081130_AAAAACfileF20081130_AAADIP' 'sip-files00041.jpg'
11d7acdeb54077fcc1a8e07e89fe3404
414eca592c821ed5d7c6e826a2bc58ee2db36c22
'2017-08-14T14:30:28-04:00'
describe
'41382' 'info:fdaE20081130_AAAAACfileF20081130_AAADIQ' 'sip-files00041.pro'
b1659ce9087e13fd4634361c2d568068
95a1cc61cab5daafb561cfa7758ecb9197c0e37d
describe
'28334' 'info:fdaE20081130_AAAAACfileF20081130_AAADIR' 'sip-files00041.QC.jpg'
36a43258ba5c2d7fc9e3fd7685ce347d
5b18735eb778b5521dd5e6345b7b19fe64257960
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADIS' 'sip-files00041.tif'
a1704ead891d8a0b4857b53bc8e55e53
ebc6eb5f45f76eb9d9e8f00d1e274e9e15bce5a3
describe
'1684' 'info:fdaE20081130_AAAAACfileF20081130_AAADIT' 'sip-files00041.txt'
8247ae95681b5bca2cf4f895e9981459
505d2c67d81b7a70bc4b004f79268dd090b58709
describe
'6981' 'info:fdaE20081130_AAAAACfileF20081130_AAADIU' 'sip-files00041thm.jpg'
835f8ee034bfd5a4dd905c67f0fe160b
28e0f465176cde9805a15953749340996a8f10fb
describe
'969943' 'info:fdaE20081130_AAAAACfileF20081130_AAADIV' 'sip-files00042.jp2'
29282fa7dccecf2014ff40735122e00a
df9782b6d9e559e070ffc54726802273c0f653c4
'2017-08-14T14:34:36-04:00'
describe
'55328' 'info:fdaE20081130_AAAAACfileF20081130_AAADIW' 'sip-files00042.jpg'
cb5d6003cb116776a46c5820d471f722
92b5aa74fe9cfc150db068ec81d831e05ba304ce
describe
'26393' 'info:fdaE20081130_AAAAACfileF20081130_AAADIX' 'sip-files00042.pro'
ae659b226ddc1b0a6e7c1dfee7bce408
ebd81c04bc8a03a058070fa8abf38d1e8e105fb2
describe
'18106' 'info:fdaE20081130_AAAAACfileF20081130_AAADIY' 'sip-files00042.QC.jpg'
9ee7bee9789a4a34ee5981da45b8ef00
ebaf1fe045bdc3eccf34784dfc329ded472c490e
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADIZ' 'sip-files00042.tif'
e504d82dbf35c0944dce1db22078a282
6aedfb428072c4cf1a805b3121b0812e4680b631
describe
'1198' 'info:fdaE20081130_AAAAACfileF20081130_AAADJA' 'sip-files00042.txt'
722bfecaa755cb5a8ba354f096a4e996
b314a712dd3254ee86fc49d9e167bc0d368c0361
describe
'5052' 'info:fdaE20081130_AAAAACfileF20081130_AAADJB' 'sip-files00042thm.jpg'
03a2b4c4365bea9724d672d9b5fda5dd
97944b009a98a3d89c79dcb50db60223297e52b1
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADJC' 'sip-files00043.jp2'
a0b2b25f6799f8f2000781427378d7a2
58825d33385358a99bf768883464e86693e9b3c6
'2017-08-14T14:27:07-04:00'
describe
'81876' 'info:fdaE20081130_AAAAACfileF20081130_AAADJD' 'sip-files00043.jpg'
d7ef73f25eeec532940733724e6c6453
0e416951a9073d5a0c04b1e783834ba23eb5222e
'2017-08-14T14:32:54-04:00'
describe
'41604' 'info:fdaE20081130_AAAAACfileF20081130_AAADJE' 'sip-files00043.pro'
045e537549d4ee10cb50c865c37f3fda
9164b189b2cef846b9d579382375e21f48071be4
'2017-08-14T14:28:38-04:00'
describe
'27840' 'info:fdaE20081130_AAAAACfileF20081130_AAADJF' 'sip-files00043.QC.jpg'
a17616e005d2b6ce39ec10781eeb610d
9feb61c55b994085741751d0d7f4cd88820a5b64
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADJG' 'sip-files00043.tif'
d641931a6be3a97c7d99c833f86c6c7b
89cf56250458d776231c1f29351750b671ba17e2
'2017-08-14T14:31:31-04:00'
describe
'1699' 'info:fdaE20081130_AAAAACfileF20081130_AAADJH' 'sip-files00043.txt'
f2cd70a9927a4c7297f250db9dbe260d
cd98f03581bebc16a81adcb2e87226debd954675
describe
'6797' 'info:fdaE20081130_AAAAACfileF20081130_AAADJI' 'sip-files00043thm.jpg'
9e428294cc00dd6ad58d74637e2e821a
2815918803daee4b9ac8c882e70e4ac07c63578c
describe
'1063159' 'info:fdaE20081130_AAAAACfileF20081130_AAADJJ' 'sip-files00044.jp2'
12bfd5dfdfb3d46cea9ce86c53349fb0
bd61c9d1772b9cec8c4807a34f359defe0440c2c
describe
'32399' 'info:fdaE20081130_AAAAACfileF20081130_AAADJK' 'sip-files00044.jpg'
6ed73bc10ab32964adb4bf85b2a492b2
208bd7f1bcdf16025c9f4d373c63d4feb2749f11
'2017-08-14T14:28:13-04:00'
describe
'8138' 'info:fdaE20081130_AAAAACfileF20081130_AAADJL' 'sip-files00044.pro'
4e94260b243640b36fc555726636e3fb
298c0512168d1be2f69e2e3be4244dc92520a1c9
describe
'10688' 'info:fdaE20081130_AAAAACfileF20081130_AAADJM' 'sip-files00044.QC.jpg'
538434540d76dca95df8c9cdf6243825
92199abd184b7d7ee8d46377b211aa71f2be7c62
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADJN' 'sip-files00044.tif'
9edde147c7c1251b5c051f082fc0ea77
547829e8c468c4fb8e0d1461dab78e96ee07e9eb
'2017-08-14T14:31:18-04:00'
describe
'563' 'info:fdaE20081130_AAAAACfileF20081130_AAADJO' 'sip-files00044.txt'
569b3bc12e2ca06ebbfa5696262f3dc4
e655ed3323cb7161ba66afea7412851aa1c787b7
describe
'3506' 'info:fdaE20081130_AAAAACfileF20081130_AAADJP' 'sip-files00044thm.jpg'
2eadcca74d8e9c9e0d2588347fdef0ee
684c94d2b181b1bede2a3e27bd14c4e7f1c2999b
describe
'970014' 'info:fdaE20081130_AAAAACfileF20081130_AAADJQ' 'sip-files00045.jp2'
2ad426f0d13eb2858e13da9b6b99d678
08e323bac9b93716605103b59f7d9308e01ab092
describe
'79176' 'info:fdaE20081130_AAAAACfileF20081130_AAADJR' 'sip-files00045.jpg'
d4b3ab554ba42b1a10696bd3f7cdffd8
590ae560ccaebf904e448c9a2b1a842061f8e8ab
describe
'40465' 'info:fdaE20081130_AAAAACfileF20081130_AAADJS' 'sip-files00045.pro'
b65528223ddc6e35ba18771d75d6537f
677ea93107782707c508146981012da32ca28f9e
describe
'26958' 'info:fdaE20081130_AAAAACfileF20081130_AAADJT' 'sip-files00045.QC.jpg'
62c8e0b2d8a02e3e1c62dcc5f9bf158c
9b97218d173efad25bff36be37b4ed702a1b16af
'2017-08-14T14:34:24-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADJU' 'sip-files00045.tif'
2a0c619b2e9fa8b3cbac88659324892b
d12cbb9ed2c7296d87fdc6fd69867e893c63b3f6
'2017-08-14T14:31:07-04:00'
describe
'1636' 'info:fdaE20081130_AAAAACfileF20081130_AAADJV' 'sip-files00045.txt'
d55715545a8d2dca1063ea316d66ec59
849928dc25c969e98f92ea85b9edc0f80f1e6113
describe
'6741' 'info:fdaE20081130_AAAAACfileF20081130_AAADJW' 'sip-files00045thm.jpg'
f96e7cc86244bead303b0583552d0220
3c64b4ce83d9f5984ccd2010ebcd100f240ac138
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADJX' 'sip-files00046.jp2'
81b32a66fc46a91c80a42443b8407a78
b45cfb74c664213bae77b5e5c19db9928270016e
describe
'75829' 'info:fdaE20081130_AAAAACfileF20081130_AAADJY' 'sip-files00046.jpg'
079d6ecddb93cc1c4d90cf1b4d577ec1
9810b28c935f49ac0788b97bdb0ff7c1e90cc090
'2017-08-14T14:28:16-04:00'
describe
'37388' 'info:fdaE20081130_AAAAACfileF20081130_AAADJZ' 'sip-files00046.pro'
cc458a96a59bd5fbdfaf900be0ecdd7f
9ce0000e44ce935affa5f42970461cffa1eb76e9
'2017-08-14T14:33:51-04:00'
describe
'24750' 'info:fdaE20081130_AAAAACfileF20081130_AAADKA' 'sip-files00046.QC.jpg'
637b691f3a5b79559bc8b31a0853161b
83b804afe11b6b6aa32f8c15cc5d96d458e3c949
'2017-08-14T14:31:48-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADKB' 'sip-files00046.tif'
786bf6ff537ce85c6757afbab12d3db7
4ff94f458b23b3cf3e9879f250168cb410f1cdbd
describe
'1543' 'info:fdaE20081130_AAAAACfileF20081130_AAADKC' 'sip-files00046.txt'
5a26f5fca109186841af064be9810c54
6100906bbfbb0135a878c2f7f3107f6b1274fded
'2017-08-14T14:28:52-04:00'
describe
'6524' 'info:fdaE20081130_AAAAACfileF20081130_AAADKD' 'sip-files00046thm.jpg'
48eb2b49e0bff5209f346b68f039a037
97a429b6a4ed5fcbcf49881b86c1af384cf79787
'2017-08-14T14:32:41-04:00'
describe
'970013' 'info:fdaE20081130_AAAAACfileF20081130_AAADKE' 'sip-files00047.jp2'
b4eba936f7912a158822851a09694325
0ff82d9ae8b489443ae749075445f435db8d9ab9
'2017-08-14T14:31:55-04:00'
describe
'78983' 'info:fdaE20081130_AAAAACfileF20081130_AAADKF' 'sip-files00047.jpg'
cc669d69092843369dbb4d93376fca15
2fbe9ec5f6c373f9e3658b9d34735a89412dab98
describe
'39096' 'info:fdaE20081130_AAAAACfileF20081130_AAADKG' 'sip-files00047.pro'
9851b88a406199ead4211d92addd3809
8789166343a3723918165de3ab748ff4bcc2f859
'2017-08-14T14:33:06-04:00'
describe
'26584' 'info:fdaE20081130_AAAAACfileF20081130_AAADKH' 'sip-files00047.QC.jpg'
63e271279a163932c3bf8561c531dd38
088b08f2fa52084beb1e9cbae6e7e8feab35cffd
'2017-08-14T14:32:51-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADKI' 'sip-files00047.tif'
c458be7a4b09ee56830c292116f45b7d
40845b114a93ea964096a6b5e3512471a666e264
describe
'1588' 'info:fdaE20081130_AAAAACfileF20081130_AAADKJ' 'sip-files00047.txt'
9e3f8dde2f3aa67d3d19986e01ab062b
19bccd4a5c961ef7522b63fd7f0a66753b2716f5
describe
'6705' 'info:fdaE20081130_AAAAACfileF20081130_AAADKK' 'sip-files00047thm.jpg'
cdaebd1520d26fa10d80adabb7919710
eaac2f66bf8d033407abb7efe7b1821f591033bd
'2017-08-14T14:34:11-04:00'
describe
'970022' 'info:fdaE20081130_AAAAACfileF20081130_AAADKL' 'sip-files00048.jp2'
0e7ceecba7d3fcc8ac34ff6d553405e7
c78b9b9ac171acf453c682669b53815fb1cefb54
describe
'79984' 'info:fdaE20081130_AAAAACfileF20081130_AAADKM' 'sip-files00048.jpg'
9efbc4217c1bede0b372de8483d00e37
2abb3dcca97a5248874d229fbad6c8fc90be1e63
'2017-08-14T14:32:17-04:00'
describe
'39993' 'info:fdaE20081130_AAAAACfileF20081130_AAADKN' 'sip-files00048.pro'
0ad38ff7d15ac7221f09bdef5c631e4a
6101499c24fee3649ce638bfa93fc4e8d03a3449
'2017-08-14T14:27:40-04:00'
describe
'26561' 'info:fdaE20081130_AAAAACfileF20081130_AAADKO' 'sip-files00048.QC.jpg'
fa4f50d6f82fb593208d2790f6154951
6e3c89053167d6da70e2a226b7c0281266bc54e4
'2017-08-14T14:31:10-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADKP' 'sip-files00048.tif'
bdb9819c4d9d17f1e4b6c37f4273f3d9
fc7fce140ca079dd4a6a5734c6656672062c988e
'2017-08-14T14:31:15-04:00'
describe
'1644' 'info:fdaE20081130_AAAAACfileF20081130_AAADKQ' 'sip-files00048.txt'
351a520633a9c4054a56b1e51581d012
b27737f4956ba70225fb9fd11cc2b683b5babb5e
describe
'7034' 'info:fdaE20081130_AAAAACfileF20081130_AAADKR' 'sip-files00048thm.jpg'
34bed94dd7f8ecc3d64135f809ae8e2e
c30f91ef92f0b0adf4b9fbf0888860f9391f1802
'2017-08-14T14:30:39-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADKS' 'sip-files00049.jp2'
64a9b0168b84726a1a54fd9c8a43bafe
5b411751bc47981b3acada0c00ad0f75ae9738e6
describe
'79214' 'info:fdaE20081130_AAAAACfileF20081130_AAADKT' 'sip-files00049.jpg'
7373a1fb111302f1be23d8c1c55f76ce
4f5423fc3c8c3a69b7c1d466a40ee1b0cd52834b
describe
'40067' 'info:fdaE20081130_AAAAACfileF20081130_AAADKU' 'sip-files00049.pro'
7698b6d72e5951b1f0a55864f851cd63
81f54dfee64c0b09e55a88533217583dd14e298d
describe
'26955' 'info:fdaE20081130_AAAAACfileF20081130_AAADKV' 'sip-files00049.QC.jpg'
fcc7f01634f9b864599d12cc322c0bba
81345e820c82568bcb70aac105f78498ce14fbd4
'2017-08-14T14:32:21-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADKW' 'sip-files00049.tif'
85e6fe54f3246bdd1dfe1c9270b56ca1
9c7d6805abe34768d8ce615dfb1fef0d28bfcdaf
'2017-08-14T14:31:56-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADKX' 'sip-files00049.txt'
5ab4747b40aba20ce96a8749b0ed8c6a
2e56cf0fd532680f52dd3cc21761f5f7a5702f2d
describe
'7058' 'info:fdaE20081130_AAAAACfileF20081130_AAADKY' 'sip-files00049thm.jpg'
b7a2eaaa04b85a667c475494df83f7fd
b53f9ae5e815dd72c422737cd4f8250f842b469b
'2017-08-14T14:31:59-04:00'
describe
'970009' 'info:fdaE20081130_AAAAACfileF20081130_AAADKZ' 'sip-files00050.jp2'
01bc661cb0058778b814ef38cde48bde
378189abcb40666a846f0888ce6402ec629353ee
'2017-08-14T14:28:46-04:00'
describe
'78980' 'info:fdaE20081130_AAAAACfileF20081130_AAADLA' 'sip-files00050.jpg'
0900f10683e4b1599d2d15376345f37c
c07106088030e0fc28070e1ced9f89f4f21c6881
describe
'40515' 'info:fdaE20081130_AAAAACfileF20081130_AAADLB' 'sip-files00050.pro'
45dd52d016d0627cd4ce6a5bef3c8cfc
3c2e125fbe89c7deff5662633b0b5836179284b3
describe
'26779' 'info:fdaE20081130_AAAAACfileF20081130_AAADLC' 'sip-files00050.QC.jpg'
a2bf775f5592baa7a92217675540709e
ca65d527f4ab22d6384d3a7552303c4429c80031
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADLD' 'sip-files00050.tif'
5b8226ab124d61edd20af4251e2f1fa7
290e0213a67f8b0f3db28d3f56be27aaf5288728
'2017-08-14T14:31:45-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADLE' 'sip-files00050.txt'
49566ce09ce5c8eab43f3f0587568be6
49ca3a9a8190f7af282df3922bd9d3bb4115cd5a
describe
'6859' 'info:fdaE20081130_AAAAACfileF20081130_AAADLF' 'sip-files00050thm.jpg'
2d02f04b241519f37110e93f9a271579
86a2dc65e7b5aac780bcdd8489b922d1ab08de96
describe
'1064503' 'info:fdaE20081130_AAAAACfileF20081130_AAADLG' 'sip-files00051.jp2'
631ff584e99ac0532b2d9aa3c8875b35
5ec933f4cdde21c92f60fc21453ecca0ba080572
describe
'46823' 'info:fdaE20081130_AAAAACfileF20081130_AAADLH' 'sip-files00051.jpg'
ea85b40a21e9d86e76f9c73e3e7b4576
d75f321028f696731cf6094cfc798e2f011b0224
'2017-08-14T14:34:10-04:00'
describe
'16260' 'info:fdaE20081130_AAAAACfileF20081130_AAADLI' 'sip-files00051.pro'
3fe488625a1fef534efbfcefd3c60144
470b854447a1de6f3406092db6c37d7b59ada604
describe
'15321' 'info:fdaE20081130_AAAAACfileF20081130_AAADLJ' 'sip-files00051.QC.jpg'
9b74e7c0595507147628ccd772268bed
0bda68e0c18dd7cca69d771e2676cd702c60f54d
'2017-08-14T14:31:32-04:00'
describe
'8532492' 'info:fdaE20081130_AAAAACfileF20081130_AAADLK' 'sip-files00051.tif'
2e3104440c61cf9297a6a06b0a5e7715
2ebeb5e1513fa51db7b85c14102a31429036356b
describe
'946' 'info:fdaE20081130_AAAAACfileF20081130_AAADLL' 'sip-files00051.txt'
83b1686c48e653eb5898534aa148a66a
00388cb28bd1f166e0df321e88feceff8a2f24e2
'2017-08-14T14:30:30-04:00'
describe
'4777' 'info:fdaE20081130_AAAAACfileF20081130_AAADLM' 'sip-files00051thm.jpg'
3e310a2a759bc09adf0994fc68ce15d3
f03e61f75226ca2f5a3615942108f7273e0ea51e
describe
'969987' 'info:fdaE20081130_AAAAACfileF20081130_AAADLN' 'sip-files00052.jp2'
fa67c61d6a2d4b34c9f98553638bb1e9
66eb15a5bfc6c6117f8f1b018dc23e133b498a1c
describe
'63119' 'info:fdaE20081130_AAAAACfileF20081130_AAADLO' 'sip-files00052.jpg'
ffd9c2df1388d8061ad3c7f4d1fd7643
1a57c42134696b923c0d5ec5a7d1543054ed4eff
describe
'30652' 'info:fdaE20081130_AAAAACfileF20081130_AAADLP' 'sip-files00052.pro'
ff1e9020d6c69b4755de463171ed86d7
e377c0766838d20e708d62ba44a3c28c884eb5db
'2017-08-14T14:28:21-04:00'
describe
'20771' 'info:fdaE20081130_AAAAACfileF20081130_AAADLQ' 'sip-files00052.QC.jpg'
28ace24343c552ca51bb0b615ad77dea
9719386736d3c565ebceabcda05b643b3096e489
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADLR' 'sip-files00052.tif'
f35cbf4bb51aa83d1535b9b2b4ef62b0
9886e9c5af731e5d6f2d2ef4b0e7a2114fbd9e7b
'2017-08-14T14:33:34-04:00'
describe
'1333' 'info:fdaE20081130_AAAAACfileF20081130_AAADLS' 'sip-files00052.txt'
1e54ba83d5996dd539455978b58f1faa
56c17628f4cac8517d678ab44f848b1a5635e095
describe
'5713' 'info:fdaE20081130_AAAAACfileF20081130_AAADLT' 'sip-files00052thm.jpg'
1a0986e4bf8aea5f43c39b77c8c5c499
796221a99307252e1d4a38231b07126b6d5bacb3
describe
'977390' 'info:fdaE20081130_AAAAACfileF20081130_AAADLU' 'sip-files00053.jp2'
18d39a78d2d29df938a8bbfc0d3416e3
19386b90127e4c579585f900e90c9b7618c217b3
describe
'75800' 'info:fdaE20081130_AAAAACfileF20081130_AAADLV' 'sip-files00053.jpg'
c384cd9e59ced727490002f49dd29c90
ef17989d54dd5b94b9bcbc761dd8f20d655a5781
describe
'38575' 'info:fdaE20081130_AAAAACfileF20081130_AAADLW' 'sip-files00053.pro'
148d25b7c1a737540c65d65f00887908
04c58fe8976273362873b0c8e661580de5d97388
describe
'26007' 'info:fdaE20081130_AAAAACfileF20081130_AAADLX' 'sip-files00053.QC.jpg'
9ac47c21ead6aa0a17dd86bd58fa618f
8562aeb7aa645508aa0bce326087aee24a75a953
describe
'7836984' 'info:fdaE20081130_AAAAACfileF20081130_AAADLY' 'sip-files00053.tif'
4343e687c56967415fbc4bfbe89951e9
550bdb2e7258d8a6218660fc78b98ac3c387ccad
'2017-08-14T14:27:57-04:00'
describe
'1598' 'info:fdaE20081130_AAAAACfileF20081130_AAADLZ' 'sip-files00053.txt'
c4c7f4958072d3d0fb6fa4a498d1c0fe
6f9a727b3772c87b5cc57c2c7c89ab64dab8bfec
describe
'6702' 'info:fdaE20081130_AAAAACfileF20081130_AAADMA' 'sip-files00053thm.jpg'
df17a9dfdc8cd806cb682de57343f84d
f154e423344d221cd3b62a07db247b5dedf4956d
describe
'1065113' 'info:fdaE20081130_AAAAACfileF20081130_AAADMB' 'sip-files00054.jp2'
938af673eb832187880f130c5bb86d61
1f3bb7ab559f06d865231e668ec6becea08bea00
'2017-08-14T14:27:49-04:00'
describe
'43369' 'info:fdaE20081130_AAAAACfileF20081130_AAADMC' 'sip-files00054.jpg'
00b736da325ea0ebe515aa14d4574aa0
0ff27f34037a3241692ed35c024b8d495cd3a37a
'2017-08-14T14:27:46-04:00'
describe
'10503' 'info:fdaE20081130_AAAAACfileF20081130_AAADMD' 'sip-files00054.pro'
e12bc8834a299c8bb46dff09f14b3d14
3be89e35d67de31c332efbc4e5048cdfcfddeda7
describe
'14544' 'info:fdaE20081130_AAAAACfileF20081130_AAADME' 'sip-files00054.QC.jpg'
afa4dbe21ff19593df31b1058f3c786a
5f6d03c15ed9312cf555e2fce91db24d7a8415ca
describe
'8537616' 'info:fdaE20081130_AAAAACfileF20081130_AAADMF' 'sip-files00054.tif'
aaaac7a1ecdcf52732af3be6bf163c66
855c4159c83498b823160ae99c2133b8ad06719e
'2017-08-14T14:33:14-04:00'
describe
'519' 'info:fdaE20081130_AAAAACfileF20081130_AAADMG' 'sip-files00054.txt'
3e47b45b47902750f089de33f4a18a50
98b11429fa75c322702d9a750aaf0c7a45a2dfbc
'2017-08-14T14:30:17-04:00'
describe
'4528' 'info:fdaE20081130_AAAAACfileF20081130_AAADMH' 'sip-files00054thm.jpg'
e59c4f3949ba9fcd06677ac70f4e4e86
88b2876060316debcbff2aa0cbb40480cee96539
describe
'970019' 'info:fdaE20081130_AAAAACfileF20081130_AAADMI' 'sip-files00055.jp2'
99892a5953f887dfe3789d7d41cbffd4
2b8c6864a147e0a72ef4dd9ead90281b3eb5a082
describe
'82229' 'info:fdaE20081130_AAAAACfileF20081130_AAADMJ' 'sip-files00055.jpg'
6d7579cc196a51669905c5bf037925ae
9088c9a059c55e9886842bf38cb94fed6f2252a4
describe
'41629' 'info:fdaE20081130_AAAAACfileF20081130_AAADMK' 'sip-files00055.pro'
c8b3e6d60b639b825df2dfe6eb039239
47af19350402941aa32b7881bc6e0f0a9d5d3eb2
describe
'28046' 'info:fdaE20081130_AAAAACfileF20081130_AAADML' 'sip-files00055.QC.jpg'
2db364a1b3cd2dc369449267ae366cf4
2bad2a71ac3e50987f42fd8b80853b8d52aff969
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADMM' 'sip-files00055.tif'
f660fc0e4e55de4833c5f5db48ad6151
f50adb7a2fd065744d49f85a7433ae5c14ca2efc
'2017-08-14T14:27:31-04:00'
describe
'1667' 'info:fdaE20081130_AAAAACfileF20081130_AAADMN' 'sip-files00055.txt'
1255e335903b502c746d2c55e63775ef
cbe520b3f802e135395479574d3e7c8c9b28aec8
describe
'6896' 'info:fdaE20081130_AAAAACfileF20081130_AAADMO' 'sip-files00055thm.jpg'
0b9779a853aec7388a612077b2616ff2
ed0acaa3744bf9ac62fb2a9191d070e756fc5f04
describe
'969967' 'info:fdaE20081130_AAAAACfileF20081130_AAADMP' 'sip-files00056.jp2'
f7b734d988277a349378057a15996368
c6826b2c1586c2096498644b3874f58bbd3efef5
describe
'76145' 'info:fdaE20081130_AAAAACfileF20081130_AAADMQ' 'sip-files00056.jpg'
3097217d1956542d7ee8ac0045bb312d
27d381cc6b65f665d9e12b8e9cc43b78fca1a728
describe
'38995' 'info:fdaE20081130_AAAAACfileF20081130_AAADMR' 'sip-files00056.pro'
4214ba2089c5c9848a4bf44c0782c455
1e981b6052797300229f637034dfe0103b37f784
describe
'25790' 'info:fdaE20081130_AAAAACfileF20081130_AAADMS' 'sip-files00056.QC.jpg'
a4536eb41d9361c1d051fe0299ef50d8
b309f45accfbf49bede5813c71e2fe6d023c8951
'2017-08-14T14:30:02-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADMT' 'sip-files00056.tif'
b1bf135cc8e94626c9f0e911c2cfe6b8
da29c83a87929bf0f4affc0e7307b1da6f75c3d0
'2017-08-14T14:29:33-04:00'
describe
'1592' 'info:fdaE20081130_AAAAACfileF20081130_AAADMU' 'sip-files00056.txt'
dd48deb7f2a8482abf0ad304869bb8a2
789a8280c9f12c0ab9142c29710d02e66169df20
'2017-08-14T14:29:00-04:00'
describe
'6375' 'info:fdaE20081130_AAAAACfileF20081130_AAADMV' 'sip-files00056thm.jpg'
39a5deb781f8124c85f79f8973237906
d1da4682a287ee65b9ed74b3a1ffa588c667c47d
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADMW' 'sip-files00057.jp2'
33a746c56dda1dadf6e6d83278500142
d049ebb25dfdb7ff2fbe081d5e5ca258e4ca8023
describe
'76191' 'info:fdaE20081130_AAAAACfileF20081130_AAADMX' 'sip-files00057.jpg'
5fb8830684a6db47be5e73cbf84447ce
eb46329cd60a8f2a6e13e370a1229c0b7ac6785c
'2017-08-14T14:30:13-04:00'
describe
'36837' 'info:fdaE20081130_AAAAACfileF20081130_AAADMY' 'sip-files00057.pro'
13a7eb1a1d20509556a819148b74b227
70cff8212ffef0b24c79cc5624b4826f65d1ce98
'2017-08-14T14:29:59-04:00'
describe
'26047' 'info:fdaE20081130_AAAAACfileF20081130_AAADMZ' 'sip-files00057.QC.jpg'
309027e5a62d1168c86e113834cc80b4
386fa6346212e19aa2408d43e4849542f39da771
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADNA' 'sip-files00057.tif'
37863142368cfc2069df10aa0816070f
9346fe39c8177e0a43bd3f40da4bc0222855286f
describe
'1489' 'info:fdaE20081130_AAAAACfileF20081130_AAADNB' 'sip-files00057.txt'
8b9eed25ad82928970e95e6563f9617d
39491dabf5b2b3457402a7d4139dd7cad14efa3f
'2017-08-14T14:30:20-04:00'
describe
'6234' 'info:fdaE20081130_AAAAACfileF20081130_AAADNC' 'sip-files00057thm.jpg'
7b4720044ed4612bbe3c452e7f389d11
ea0885bf7f62c2b418f968209344332ea9250522
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADND' 'sip-files00058.jp2'
fbcada4c42ce363310a74b5f9654bd09
bbe63c298d62a6b8a3d2b4d5f82742e955c29dfe
'2017-08-14T14:27:09-04:00'
describe
'72021' 'info:fdaE20081130_AAAAACfileF20081130_AAADNE' 'sip-files00058.jpg'
a2650fdd42762c0136eefc10d25914b3
734d1ce23ae11f37276759c82a8d47372b856aae
describe
'36663' 'info:fdaE20081130_AAAAACfileF20081130_AAADNF' 'sip-files00058.pro'
c90b3488b52ec7b968d0d7025691a713
6d0067902e4f574f72e1b2ad1dc0ea8af1c242fc
describe
'24678' 'info:fdaE20081130_AAAAACfileF20081130_AAADNG' 'sip-files00058.QC.jpg'
f91761ecaaeba961705bbec07c162ef8
630148ae9df9deeb5932823022a0e0a622720aa1
'2017-08-14T14:29:26-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADNH' 'sip-files00058.tif'
1645dc076354091668e2c8574c2c6ada
36cd402e165ad5b899ed24ba91bd2f25d07ff8c9
'2017-08-14T14:31:35-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADNI' 'sip-files00058.txt'
06ac35650ea7cb93803d62841bc89783
e77927be2d1ad5a1bcc96d930c3486e103ff4885
describe
'6296' 'info:fdaE20081130_AAAAACfileF20081130_AAADNJ' 'sip-files00058thm.jpg'
13071ae254b01363a2e568e815323ab4
7e473881c3de61f0617e501dc2e71feb5ba4f7a9
'2017-08-14T14:33:17-04:00'
describe
'1075827' 'info:fdaE20081130_AAAAACfileF20081130_AAADNK' 'sip-files00059.jp2'
dba324ffe062bbae281258c396198473
9f6082baf706102acbf87d84984a346181f1044a
describe
'22200' 'info:fdaE20081130_AAAAACfileF20081130_AAADNL' 'sip-files00059.jpg'
4fe1cff7b94d968882d5f7a36301ceae
8353a0351fad022c04939639b57e532080ec3118
'2017-08-14T14:27:54-04:00'
describe
'6087' 'info:fdaE20081130_AAAAACfileF20081130_AAADNM' 'sip-files00059.pro'
38665e391918f240c2bf29d9d0efaa57
65180786d3b119b713e03ac18184246a107258e9
'2017-08-14T14:29:42-04:00'
describe
'6934' 'info:fdaE20081130_AAAAACfileF20081130_AAADNN' 'sip-files00059.QC.jpg'
e9c73f2578de0f830a4df1069c434e0f
80f8dad66c29ca39abbeeac9be54469d78dac679
describe
'8623292' 'info:fdaE20081130_AAAAACfileF20081130_AAADNO' 'sip-files00059.tif'
1f70f911a573bf5aa96e83edbd87ae65
e4919c297e0edbac3ed9faefc1be6e007925c761
'2017-08-14T14:32:38-04:00'
describe
'495' 'info:fdaE20081130_AAAAACfileF20081130_AAADNP' 'sip-files00059.txt'
84182fd45296dcf36d5e9eeaa68e9b32
164d30f21f928daad8f467d709d14a263841b683
'2017-08-14T14:31:00-04:00'
describe
'2515' 'info:fdaE20081130_AAAAACfileF20081130_AAADNQ' 'sip-files00059thm.jpg'
7ce02531058ef1c1c19a26da9114ea36
08a706bdbb95621f48534cfa4437c7dd6db1db22
'2017-08-14T14:34:34-04:00'
describe
'969982' 'info:fdaE20081130_AAAAACfileF20081130_AAADNR' 'sip-files00060.jp2'
6d762db8d4814cc1dc12414f7bee4544
80ceb2e36a0240298b47e91f45563feeeaa27edc
describe
'72863' 'info:fdaE20081130_AAAAACfileF20081130_AAADNS' 'sip-files00060.jpg'
dd7ef94aabe8b22ba2e61341a977c077
423800aba00f093c2032c0acbab20f1831b95124
describe
'36678' 'info:fdaE20081130_AAAAACfileF20081130_AAADNT' 'sip-files00060.pro'
8ec0519007bf167b2cb39cd53250ecd6
1a4d85100b468459eee5f0db358020a506448ceb
describe
'24312' 'info:fdaE20081130_AAAAACfileF20081130_AAADNU' 'sip-files00060.QC.jpg'
3a06b2e728ecdd47a5044fde865bf90b
3c644fadc4bad6139810105414ad00a1b674a03d
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADNV' 'sip-files00060.tif'
4c026632299f77f24ee44b7361a8fd6a
32bc2946e45bb1aab527265c217ca805779ca02b
describe
'1513' 'info:fdaE20081130_AAAAACfileF20081130_AAADNW' 'sip-files00060.txt'
b6a5cc08c7cfeffb7616b87d92316e82
dc6aab7225dd7a4640d9cb5c682b446db3551bdb
'2017-08-14T14:29:51-04:00'
describe
'6457' 'info:fdaE20081130_AAAAACfileF20081130_AAADNX' 'sip-files00060thm.jpg'
93b51242d7fe39a16608516ae9ba0bdb
b574121d83d578cfb0b2f81670c38ed3b9260720
describe
'970024' 'info:fdaE20081130_AAAAACfileF20081130_AAADNY' 'sip-files00061.jp2'
6e442dc5ec53ee71e11dfaf5d6c223f2
965ce6acd13326f54f25689c240149e51b7db2c1
'2017-08-14T14:33:10-04:00'
describe
'63994' 'info:fdaE20081130_AAAAACfileF20081130_AAADNZ' 'sip-files00061.jpg'
0f2fed0cd6f145e5ed6966dfd85510ef
143c00f7f234d322e22c9b9ed8720ea2694d2055
'2017-08-14T14:30:59-04:00'
describe
'32066' 'info:fdaE20081130_AAAAACfileF20081130_AAADOA' 'sip-files00061.pro'
7b24bd8b3a93145db2bef4759d3e9713
4611e8900ab60ed89254bdbcfc6f7001a602e088
'2017-08-14T14:32:06-04:00'
describe
'21229' 'info:fdaE20081130_AAAAACfileF20081130_AAADOB' 'sip-files00061.QC.jpg'
ebbae5020d1b3a03e391c37dc3716633
769aafe78e6da814803521036d38293065bdae53
'2017-08-14T14:27:24-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADOC' 'sip-files00061.tif'
1f25695454a84e3cf20195a4a7eef6b5
a3b8f8f98d06633e79018993c6b574d704a2e741
describe
'1342' 'info:fdaE20081130_AAAAACfileF20081130_AAADOD' 'sip-files00061.txt'
6d7f9eb4b744c09cd8263ceb109f8887
2a0b056333e17735f1ef93a247fb7e79e79ce887
describe
'5833' 'info:fdaE20081130_AAAAACfileF20081130_AAADOE' 'sip-files00061thm.jpg'
6e0be4412841b4b2173a645120d461a1
b60935b72fb5e0aade8414ffff07e0650119d066
describe
'969925' 'info:fdaE20081130_AAAAACfileF20081130_AAADOF' 'sip-files00062.jp2'
2236caff0a9b8df6090944fab36063a3
002388498732e5b085311e9df35e390fce72dee8
describe
'57527' 'info:fdaE20081130_AAAAACfileF20081130_AAADOG' 'sip-files00062.jpg'
cc32cb7eb63bc8e1011f39884c728f7f
6d73813b74b987c4ef1a13c37baa393b5fef8e4f
'2017-08-14T14:33:47-04:00'
describe
'27550' 'info:fdaE20081130_AAAAACfileF20081130_AAADOH' 'sip-files00062.pro'
50171835b66189b1c2e51737b62179ee
efc563d141475008d13569412562298a7bad62a0
describe
'19030' 'info:fdaE20081130_AAAAACfileF20081130_AAADOI' 'sip-files00062.QC.jpg'
3acf4e12c150ca45683a65ed71f311df
ea6e0a2322aa65884b6faac56b675e78d4b99f10
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADOJ' 'sip-files00062.tif'
db6059118d759a681156047728a4328a
218a08a52cb0615107d97b1960084a1a531c7d32
describe
'1210' 'info:fdaE20081130_AAAAACfileF20081130_AAADOK' 'sip-files00062.txt'
86a438d4e9bef3fdd69ca51b2208d4b6
df809646d690c646a397b6d2f8702b9921daa074
'2017-08-14T14:31:52-04:00'
describe
'4987' 'info:fdaE20081130_AAAAACfileF20081130_AAADOL' 'sip-files00062thm.jpg'
b1fbdbbfe1abffcb3824e9c17d31ec0f
2b5452fe308480dd8afd84c4d03ab558ab53b412
describe
'970005' 'info:fdaE20081130_AAAAACfileF20081130_AAADOM' 'sip-files00063.jp2'
deda7773269924dfc0c365970406255c
ecaa1f0d8f73b53daeac2745dbe64323500473e2
'2017-08-14T14:29:34-04:00'
describe
'77250' 'info:fdaE20081130_AAAAACfileF20081130_AAADON' 'sip-files00063.jpg'
cc60c470e1e2a0c995a24c291b00b2dc
2d5b777b7435a07bca3d16b12fdb9712a279445d
describe
'38398' 'info:fdaE20081130_AAAAACfileF20081130_AAADOO' 'sip-files00063.pro'
e558dedccfc5c578a26c5f59f61bae9e
6937da9e1ffef6f690de09d545d16b0897ff2c79
describe
'26115' 'info:fdaE20081130_AAAAACfileF20081130_AAADOP' 'sip-files00063.QC.jpg'
357e2047736fda2ee427d9b2e61a6a66
a4a8fe3891f54ba442d17fae10b71528b969b87a
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADOQ' 'sip-files00063.tif'
d8a0b563037bfa25e2ffe3837e099dd7
caac9956cee5941ee43a4bed450a9ee0c3191fa1
describe
'1570' 'info:fdaE20081130_AAAAACfileF20081130_AAADOR' 'sip-files00063.txt'
9e3727eb18c3f5b91ff112f4958449e4
139d6ce70554c1c714c83115c74009814132856c
'2017-08-14T14:32:49-04:00'
describe
'6518' 'info:fdaE20081130_AAAAACfileF20081130_AAADOS' 'sip-files00063thm.jpg'
14477dc9a1041090f1bdf470ec9ec826
3ab465c6d2d6b14b970816a2eb2f8f945f0d3d90
describe
'969959' 'info:fdaE20081130_AAAAACfileF20081130_AAADOT' 'sip-files00064.jp2'
66f1bb9d25e299bbb06d113933405594
ba048e0299f7777369aa7ad58a20aa17587bc0d3
'2017-08-14T14:29:37-04:00'
describe
'74609' 'info:fdaE20081130_AAAAACfileF20081130_AAADOU' 'sip-files00064.jpg'
1d76ed53470ed85af91d4d3f6238b7f6
98e9eea6d9e0f4fbdaff33f6ea69e4f7935e5737
describe
'37954' 'info:fdaE20081130_AAAAACfileF20081130_AAADOV' 'sip-files00064.pro'
efb30d85b7e09409a31a8992cd6a6dbf
406bd353e4dbd77964749dfe9692e8cf3ce43633
describe
'25362' 'info:fdaE20081130_AAAAACfileF20081130_AAADOW' 'sip-files00064.QC.jpg'
bb65973b067a38160c66aeeb70174eff
4d26f133e4b8afcfd6102236b3651f908b3bd3c0
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADOX' 'sip-files00064.tif'
776d82051af0bfb66f4bc43c8d2a3c22
f9ea0e0dfb8a10b972e81c4175e03df2190dffd9
'2017-08-14T14:34:04-04:00'
describe
'1547' 'info:fdaE20081130_AAAAACfileF20081130_AAADOY' 'sip-files00064.txt'
5a2abbca1492848db768f6bf9266c185
e1f780f490ab6e21d6a93e8736ecd4ea2075bc3f
'2017-08-14T14:34:27-04:00'
describe
'6546' 'info:fdaE20081130_AAAAACfileF20081130_AAADOZ' 'sip-files00064thm.jpg'
70ae0938583150ef503dd0b89cee1ba1
c1b06a23186b92ba63c3b926b590a0e3a1a8c813
describe
'970023' 'info:fdaE20081130_AAAAACfileF20081130_AAADPA' 'sip-files00065.jp2'
349d438d87e07ce5c42ceab68d8e9092
01d7c5d6bfe584a5944a6488320b01b1f4ffd613
describe
'72392' 'info:fdaE20081130_AAAAACfileF20081130_AAADPB' 'sip-files00065.jpg'
a02a02c033e0ae3bf7eea9433cac5315
c34c8ca090583a8ef35ad71dd3f29143f539efb3
'2017-08-14T14:29:45-04:00'
describe
'34050' 'info:fdaE20081130_AAAAACfileF20081130_AAADPC' 'sip-files00065.pro'
df5ad501d95784c73e737460801ca0c2
54f8ce7190d6d54a001b2011560a7d58f6be666c
describe
'23342' 'info:fdaE20081130_AAAAACfileF20081130_AAADPD' 'sip-files00065.QC.jpg'
a0238877aa29d9e60eb1929b86096d81
725716c45038e748745cf7bae8d32c2b18278edd
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADPE' 'sip-files00065.tif'
d1948d3319ba58e338f9be7270657dc8
047727df21be78f4656bbf388ed26ff98f0673fa
describe
'1449' 'info:fdaE20081130_AAAAACfileF20081130_AAADPF' 'sip-files00065.txt'
c9d3d905a421c69bfb6cefe2f0c288e7
09e92713e5335d13156a05eaf6d3640f4618c9c8
describe
'6367' 'info:fdaE20081130_AAAAACfileF20081130_AAADPG' 'sip-files00065thm.jpg'
1af051fd8fd9a9c7a6bef1e9ad4fd289
2f49a31a15f94e219da0b203a3ef00f17130bbed
'2017-08-14T14:28:57-04:00'
describe
'1052514' 'info:fdaE20081130_AAAAACfileF20081130_AAADPH' 'sip-files00066.jp2'
0fe9e3a1c12633a218c1cd480aa0314f
8109cc10828a2bde5a6170bbff892bdc6967877c
describe
'25533' 'info:fdaE20081130_AAAAACfileF20081130_AAADPI' 'sip-files00066.jpg'
619c130c563bb9cc06f5ce7cac00811c
db2c750ad092d58ab0a7ef70eae208b8d07da621
'2017-08-14T14:34:37-04:00'
describe
'5257' 'info:fdaE20081130_AAAAACfileF20081130_AAADPJ' 'sip-files00066.pro'
8b1e098ed7891956b9c7a641c039579b
bd5885ead1b625e21ad6ddd702ce6a4f0ea4aa08
describe
'8755' 'info:fdaE20081130_AAAAACfileF20081130_AAADPK' 'sip-files00066.QC.jpg'
8939b15a06e3ed6879c7ad3b28f7755b
f0157f802b0d18514073b9d9e67eb36ba4a3a2fe
describe
'8437040' 'info:fdaE20081130_AAAAACfileF20081130_AAADPL' 'sip-files00066.tif'
d1137fb3c0ee506a7b2e322355a7b286
c2249af1efe2a00354dd14cdd618383b34ce32a1
describe
'254' 'info:fdaE20081130_AAAAACfileF20081130_AAADPM' 'sip-files00066.txt'
82d4f67ac394e1abce0dd1ed5311368b
049bc3aaab75c27320ad2c9fb1259286d54bbd2d
describe
'2942' 'info:fdaE20081130_AAAAACfileF20081130_AAADPN' 'sip-files00066thm.jpg'
ac41b6b9d209a7c41880984cda96665e
88ab6ffb370366691c2f169d757ea1bb4ce59d49
'2017-08-14T14:28:45-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADPO' 'sip-files00067.jp2'
3dee29404c5bfad61e4467a8331d900c
a56383aa9fba2b4fe711a7ebd241e3b98b1b2d0e
describe
'72142' 'info:fdaE20081130_AAAAACfileF20081130_AAADPP' 'sip-files00067.jpg'
c78a7024a18469b04dee5ad0a16411fb
c09bd2d4daeb8978d2692cee6318a9932c4ec278
'2017-08-14T14:33:18-04:00'
describe
'35619' 'info:fdaE20081130_AAAAACfileF20081130_AAADPQ' 'sip-files00067.pro'
5066c074fa25778aa2fa3d75049f4e3b
e12d1bd99f77a6f791dbdcd6d061e26ea6e30e8b
describe
'24682' 'info:fdaE20081130_AAAAACfileF20081130_AAADPR' 'sip-files00067.QC.jpg'
d5a7d4e4e08ecb8ff5d6373688c0868c
efdadceab2542761001032584a8e83e57ffbe7a1
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADPS' 'sip-files00067.tif'
75afe7bf3f52d44d19856af621f9fe04
d6ce6cb59de064d59260602977404e0873a55245
describe
'1477' 'info:fdaE20081130_AAAAACfileF20081130_AAADPT' 'sip-files00067.txt'
6b38e4e5c948b88c47d0f825da0529e2
d715a51b537f9b710d69f32cb71da9de09c08cef
describe
'6414' 'info:fdaE20081130_AAAAACfileF20081130_AAADPU' 'sip-files00067thm.jpg'
750eb334b60c51fd51de837446cffb4b
9f5558bec5cba9e9e9458350207b59450c6719d5
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADPV' 'sip-files00068.jp2'
a5db590f0e3a8736fa60b8796219cb6b
383ffb2df68246a9ff6c34ec04d89cd42442ac3e
describe
'76309' 'info:fdaE20081130_AAAAACfileF20081130_AAADPW' 'sip-files00068.jpg'
79f86653cebbb08ac7aef52ee93af8c0
f0f34930d67ea18edefa95075e873427d617c12d
describe
'37818' 'info:fdaE20081130_AAAAACfileF20081130_AAADPX' 'sip-files00068.pro'
1ca768673b2c307be3fff9ea5b9976c4
4cd26175709a3f9c77da736ddf2135d6ee274e3e
'2017-08-14T14:31:08-04:00'
describe
'25664' 'info:fdaE20081130_AAAAACfileF20081130_AAADPY' 'sip-files00068.QC.jpg'
c32ffc4028d1a7848ae3e05957a9597b
dd10209b08c40c81e5642d78f2db06101f462798
'2017-08-14T14:31:28-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADPZ' 'sip-files00068.tif'
b245de1f826d0127972bcf0e84da82ec
67829768b2dd10f64d11932541506235639e3571
describe
'1546' 'info:fdaE20081130_AAAAACfileF20081130_AAADQA' 'sip-files00068.txt'
bb8a14c47ee59adb2a47c6aa0b9d178e
c77ab9794236c5c0a7480b8f0b78d0fcb0003b88
describe
'6717' 'info:fdaE20081130_AAAAACfileF20081130_AAADQB' 'sip-files00068thm.jpg'
55527b5bf0c72e95b982e40a3fe792f9
b7d378472f36548fdbf59f90ec251d61b5004a3f
'2017-08-14T14:28:20-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADQC' 'sip-files00069.jp2'
d8f647781dd9488687883fa68d622ea2
0794e7607070be972bf77db82dcb21df189f9f76
describe
'74341' 'info:fdaE20081130_AAAAACfileF20081130_AAADQD' 'sip-files00069.jpg'
4016a756fe23db6c63edb933140843d4
a6b7eaf9d8074d0c43038c076b16d70787c93f34
describe
'36736' 'info:fdaE20081130_AAAAACfileF20081130_AAADQE' 'sip-files00069.pro'
052c816a41bc5945b6b31d95deb60a72
9067f3c52f7748c21ea0e104e69c9a1de954a626
'2017-08-14T14:29:25-04:00'
describe
'24221' 'info:fdaE20081130_AAAAACfileF20081130_AAADQF' 'sip-files00069.QC.jpg'
788f9369c18152bb2acd782e59feae0e
4a0c8372222bb2c70b799a25de3eee9801afc513
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADQG' 'sip-files00069.tif'
c6909e81495aa9ff5f3e30d193c387a1
bc7213d224fc5bc1d60adb6d3fe7b3029fc91c90
describe
'1526' 'info:fdaE20081130_AAAAACfileF20081130_AAADQH' 'sip-files00069.txt'
5865f1613aca10bc0eb3e54ce61b3ca3
b2fff5b429ea2a78a833ada544597696359bb186
'2017-08-14T14:34:22-04:00'
describe
'6484' 'info:fdaE20081130_AAAAACfileF20081130_AAADQI' 'sip-files00069thm.jpg'
b782766e1a81d781a8681b3663e9a78f
1dd8e9fec5428d72749cb57a4c9904bc340c4e39
'2017-08-14T14:34:30-04:00'
describe
'970029' 'info:fdaE20081130_AAAAACfileF20081130_AAADQJ' 'sip-files00070.jp2'
b610519acdb91de2ec58a0e747a77b85
2e6caa0ea418e13cf45570bcecd63429c23fc313
describe
'76788' 'info:fdaE20081130_AAAAACfileF20081130_AAADQK' 'sip-files00070.jpg'
23444f1036f1bec9cb325e58163441d5
6feb4918f46eb67b092f3defcac38cdce67a76c9
describe
'38324' 'info:fdaE20081130_AAAAACfileF20081130_AAADQL' 'sip-files00070.pro'
41f1e9df956956700d42a5c91bd9ab47
c30866aa558979b897b61e93032cdad04506863a
describe
'25518' 'info:fdaE20081130_AAAAACfileF20081130_AAADQM' 'sip-files00070.QC.jpg'
58fc64ab78db75789d43ffed60d9f4a4
64ee0bc6d48b7806ac07d4e4f16e55e4da131218
'2017-08-14T14:29:20-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADQN' 'sip-files00070.tif'
16daaaa604f17c5a97914d58ea7f485e
78984300dc50224bb1c3a997246f861e60edbdcb
'2017-08-14T14:27:33-04:00'
describe
'1561' 'info:fdaE20081130_AAAAACfileF20081130_AAADQO' 'sip-files00070.txt'
709d446e2c733a4cbcb4ef0eb4bbac0f
24335634bb19ce46808c916977bb4969042fd47a
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADQP' 'sip-files00070thm.jpg'
0cf8594c0eac2e73c15ede07c0c25817
643a46224b1340490235af81f492b81a317173a1
describe
'969989' 'info:fdaE20081130_AAAAACfileF20081130_AAADQQ' 'sip-files00071.jp2'
f8d2905074bc88ecf47836641556c3da
2c34a01962e0353f3d7c20edddde27895746610a
describe
'79597' 'info:fdaE20081130_AAAAACfileF20081130_AAADQR' 'sip-files00071.jpg'
8f3798644673f68d77a6ca33df39cf08
b7964a8bf710d2a6054671f25d171f874f889996
'2017-08-14T14:29:21-04:00'
describe
'39803' 'info:fdaE20081130_AAAAACfileF20081130_AAADQS' 'sip-files00071.pro'
55d2fe6b1e7daebcf6d6477685cfdfcd
eb69927aeda74b8cac341b180b652c000a7b05de
describe
'26650' 'info:fdaE20081130_AAAAACfileF20081130_AAADQT' 'sip-files00071.QC.jpg'
729e669670176dc463e3fb0c921448bb
dd16b52f5b93cfa3cf166b1d683276944991d776
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADQU' 'sip-files00071.tif'
0b22f1a34f57f2ee56a7190a2a55688b
c4c0385f18e7991153234acf322c4423a60576cb
'2017-08-14T14:33:23-04:00'
describe
'1615' 'info:fdaE20081130_AAAAACfileF20081130_AAADQV' 'sip-files00071.txt'
a2d691eb28d212e27c01c28cba6b951f
35c5b5ea3ad21bc62543e651871ee6c3b0fadab8
'2017-08-14T14:27:42-04:00'
describe
'6829' 'info:fdaE20081130_AAAAACfileF20081130_AAADQW' 'sip-files00071thm.jpg'
8b10b1c5ac83568929d58fad95fc5914
d5e1525431ff5dce9b0f294045b9c2b73f66d632
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADQX' 'sip-files00072.jp2'
3ad52c8860db77c25f49a6f9b313b540
ef366e67aff8543d16c82a4088fb76f1d31177b4
describe
'75382' 'info:fdaE20081130_AAAAACfileF20081130_AAADQY' 'sip-files00072.jpg'
c75a84fbb6bb3c8e5eee9615c56c1cd3
aae9928915ad8aa3b24439cfbbcb64774e9d3db7
'2017-08-14T14:27:08-04:00'
describe
'36859' 'info:fdaE20081130_AAAAACfileF20081130_AAADQZ' 'sip-files00072.pro'
f9c0822898e0e0766888cb78b6c2d9e7
36fe3054fea69cf16b4377cba9ea845f536d3234
describe
'25243' 'info:fdaE20081130_AAAAACfileF20081130_AAADRA' 'sip-files00072.QC.jpg'
51a9474c6d574e5ed2b32708c5c2bfbf
f9ac5afbf61143c8e6df288e9c15462b3786b956
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADRB' 'sip-files00072.tif'
a4fa3946e7e3dfbb4d6df841c88d5cba
6b476032c63fb38dbd69580e73c94115e120ec02
describe
'1486' 'info:fdaE20081130_AAAAACfileF20081130_AAADRC' 'sip-files00072.txt'
5c01c0ccfbaa986344d9f918c975b7f6
1c55fabff932d8dd14a0a4468a3e1fc82ebd0873
describe
'6292' 'info:fdaE20081130_AAAAACfileF20081130_AAADRD' 'sip-files00072thm.jpg'
36b7be34ff0654799f84d186137cb742
4d125f559b2538d066dd79a2d9961c75cbe7883a
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADRE' 'sip-files00073.jp2'
43762aa26f165603653c103daf29370b
890e88258c7ac208a9670e479a18d6a820865455
'2017-08-14T14:29:48-04:00'
describe
'75844' 'info:fdaE20081130_AAAAACfileF20081130_AAADRF' 'sip-files00073.jpg'
6093374787d4e0ff20d76cf45491c86b
f2d5880b1cef4eeec8eed36fd5655fc7ea17f3fb
describe
'37113' 'info:fdaE20081130_AAAAACfileF20081130_AAADRG' 'sip-files00073.pro'
95af34735dff57601560b7f7c4a36d0c
a7f1a61a2a61739c4847cd36ad96bd6f2c136d2d
describe
'25449' 'info:fdaE20081130_AAAAACfileF20081130_AAADRH' 'sip-files00073.QC.jpg'
7169b1f01ad57611bab651c46b1be665
7856974a22f1c3aeb31d81068768a51aad6b0190
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADRI' 'sip-files00073.tif'
c74435750de0d1e68a57998a6ee87411
0909d6d564e871a1fb6b0ad0d8988b167d54736a
describe
'1522' 'info:fdaE20081130_AAAAACfileF20081130_AAADRJ' 'sip-files00073.txt'
c38bef420c484eba2f8d450b640a9024
9f834059df620537e5e8eb9e97e11750fef656ee
describe
'6499' 'info:fdaE20081130_AAAAACfileF20081130_AAADRK' 'sip-files00073thm.jpg'
d5239ab89a76f17d6e8e5f443162e6c5
ac8d61a03d617a945320f42ea94affe622c1acae
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADRL' 'sip-files00074.jp2'
efc2049903e9f957b59a9fc2c4889d96
0f6b11c6449b9f7c91b81db7341a7d00d0792e83
describe
'80478' 'info:fdaE20081130_AAAAACfileF20081130_AAADRM' 'sip-files00074.jpg'
305399010d9ba6d4fd2b5c1b1d81dd12
839fdb2e1260135c251e76190974a8da806569da
describe
'41073' 'info:fdaE20081130_AAAAACfileF20081130_AAADRN' 'sip-files00074.pro'
d1aa0a0cfe7d8723ecfc303d6c12c2a7
d1262f17ce78389447058004fbdfdec1b9d119aa
describe
'27359' 'info:fdaE20081130_AAAAACfileF20081130_AAADRO' 'sip-files00074.QC.jpg'
6a32236f835a2c08db6d4d2d1056f666
8ad7f9eb9a63b710f89e66691c2729e3d42d2b51
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADRP' 'sip-files00074.tif'
cfa204d4d36e5e83f261c6429ed4071c
0d0f94f3e79c85134a6b9c5bc2bf97560f59bf70
describe
'1678' 'info:fdaE20081130_AAAAACfileF20081130_AAADRQ' 'sip-files00074.txt'
3fa4df61861169ef31cd83e4ec3e675f
ed182e033cb457aafa900a064bd7c8e79acf049b
'2017-08-14T14:33:29-04:00'
describe
'7006' 'info:fdaE20081130_AAAAACfileF20081130_AAADRR' 'sip-files00074thm.jpg'
c44823d7c6bf76725eb970e2c06587b6
12835e339ea1e328333114e30e89877b2d81fcfa
'2017-08-14T14:33:43-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADRS' 'sip-files00075.jp2'
9b2c9902302f4b43448f072eb7fe3a51
f136bb558a6110fbe54f27b1fce4a575d16f3c14
describe
'79439' 'info:fdaE20081130_AAAAACfileF20081130_AAADRT' 'sip-files00075.jpg'
cb63ab763f995856cc1ae74eba3ac34a
7b432e26c34b1543433e92c2db98ad40b58b8505
describe
'39899' 'info:fdaE20081130_AAAAACfileF20081130_AAADRU' 'sip-files00075.pro'
66a838028909fd9babe58aec248c90e8
468f54be5fd058b5b8aa6332b00f3f4c1c9965e9
describe
'26423' 'info:fdaE20081130_AAAAACfileF20081130_AAADRV' 'sip-files00075.QC.jpg'
f2f10c0f0b209320d38851f4f66663a4
5a10a3808f1e77d17006b851d99d89957319a70e
'2017-08-14T14:34:07-04:00'
describe
'7776568' 'info:fdaE20081130_AAAAACfileF20081130_AAADRW' 'sip-files00075.tif'
bfb1f46043ea9b90b2f27a03c2d94aad
45699cc7f49e7c24da5bac8b8a057b83c120d278
'2017-08-14T14:27:16-04:00'
describe
'1637' 'info:fdaE20081130_AAAAACfileF20081130_AAADRX' 'sip-files00075.txt'
e173d2fe3a1052fc143f5ad8da9afbc8
58ead8469d95af6514d90b6a172e683f1d3963a1
describe
'7045' 'info:fdaE20081130_AAAAACfileF20081130_AAADRY' 'sip-files00075thm.jpg'
aaf2514479fb3d810554aa818050d667
90e435e545e507c9e9429137e2795a45552de792
describe
'969970' 'info:fdaE20081130_AAAAACfileF20081130_AAADRZ' 'sip-files00076.jp2'
dbd4be378d86f1fe4c0e8cf6072a97f0
1a50cb684b78b2d3691dd439c1c2867a3108db4b
describe
'78436' 'info:fdaE20081130_AAAAACfileF20081130_AAADSA' 'sip-files00076.jpg'
a9be1a0de584c6dab933b740526ee0c3
509f480e574629e30f80b47525d7398b1937cf9d
describe
'38571' 'info:fdaE20081130_AAAAACfileF20081130_AAADSB' 'sip-files00076.pro'
68d23d729b3aca80793365f0ac4b7555
9b177a30173da16835859f5982fdd01c5141408d
'2017-08-14T14:31:11-04:00'
describe
'26017' 'info:fdaE20081130_AAAAACfileF20081130_AAADSC' 'sip-files00076.QC.jpg'
83278f8f4efacc9ef29885077d49024c
75abe08805f7c634a21dc845604a4dc7d8ec2633
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADSD' 'sip-files00076.tif'
8ba0741ddd3445a9a65e131df5d425cc
2fcca6d1592c89146b85c99f670daff28d3535fa
'2017-08-14T14:33:12-04:00'
describe
'1555' 'info:fdaE20081130_AAAAACfileF20081130_AAADSE' 'sip-files00076.txt'
7a58b407053e0ec5e089ff74cb76e006
cfa7033d738994d4a731c56ded5f87183cecb0de
describe
'6663' 'info:fdaE20081130_AAAAACfileF20081130_AAADSF' 'sip-files00076thm.jpg'
0cba7ce8401b37f8b9a8dbc08ba0a9bd
590290c2db95c5e6f6a47521823e8c9388894a9d
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADSG' 'sip-files00077.jp2'
5bbe60a15b896eac045b1c580bd07962
95fcf57e4d742a36711a681a43c64418ee2d1c5c
describe
'82794' 'info:fdaE20081130_AAAAACfileF20081130_AAADSH' 'sip-files00077.jpg'
28b8f70710b32c1f75711ebe37680c54
c42cca54460efbf48f906e69762234e4e63938f4
describe
'41439' 'info:fdaE20081130_AAAAACfileF20081130_AAADSI' 'sip-files00077.pro'
5117d8d61075f61671e046effb848947
374e833234e53bd3dd243130f8e4e9454891b4bc
'2017-08-14T14:28:28-04:00'
describe
'27455' 'info:fdaE20081130_AAAAACfileF20081130_AAADSJ' 'sip-files00077.QC.jpg'
5658b154c1bf6089c80cd84052aef3f5
0b90679e855f7b7aef72cbbf76e97f221730a96c
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADSK' 'sip-files00077.tif'
5540edd0590297b9854f64469718156e
40d86da046c81f8c5715594fb512f3fa20eecb9b
'2017-08-14T14:29:56-04:00'
describe
'1676' 'info:fdaE20081130_AAAAACfileF20081130_AAADSL' 'sip-files00077.txt'
bb81c32974c0c30d4ab8ea2525d4e430
4fbb739d02b04bf7bdebb2e068411417c6e0d6cf
'2017-08-14T14:32:01-04:00'
describe
'6951' 'info:fdaE20081130_AAAAACfileF20081130_AAADSM' 'sip-files00077thm.jpg'
ff4585d5061cfc4a539b3a58adb0fb45
685846ff8879c76b8ae7401575b2fb8b79b6f4e0
describe
'970004' 'info:fdaE20081130_AAAAACfileF20081130_AAADSN' 'sip-files00078.jp2'
a93b82e50ab4017060b9424f0d0045d5
55e76e4ee1005326bec5911922d668042f76c441
describe
'80104' 'info:fdaE20081130_AAAAACfileF20081130_AAADSO' 'sip-files00078.jpg'
affa6744b4d5c33276f5726a229bb7fe
6b05d925d3e5ecb91ce54e362d58e765ee8fbcad
describe
'40811' 'info:fdaE20081130_AAAAACfileF20081130_AAADSP' 'sip-files00078.pro'
5bba4456f6e77d062e74b737db26c28e
7fc0edc53b6e402e3f12cf54c18ece5aa98e8217
describe
'27238' 'info:fdaE20081130_AAAAACfileF20081130_AAADSQ' 'sip-files00078.QC.jpg'
5f84854931b1ae842b9d598a0866675e
c17510e5d8374e657f3d859a9461430151dd7dc0
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADSR' 'sip-files00078.tif'
83dfaee1850b9d14ac409c3a163726d2
9b4ce85a45a313606f561c0b9d7509778a4feb29
describe
'1645' 'info:fdaE20081130_AAAAACfileF20081130_AAADSS' 'sip-files00078.txt'
b7fc32f27d44fa1723b99db8f36bbb2f
d3468ef1013068e96c55699bbe812415b1eca5e3
describe
'6914' 'info:fdaE20081130_AAAAACfileF20081130_AAADST' 'sip-files00078thm.jpg'
5f0e7d8f2799b2652ebfe8462e179198
edfe5262997e31fd55117da5114a78ac547db883
'2017-08-14T14:34:33-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADSU' 'sip-files00079.jp2'
49c4951c05bc373218f163ba67ebae6c
31a83e77a145046f4dcb4edc325ac7e3ef203d9f
'2017-08-14T14:28:41-04:00'
describe
'74045' 'info:fdaE20081130_AAAAACfileF20081130_AAADSV' 'sip-files00079.jpg'
e26860450109249edca76fb766ef07e5
282c07594b604671ad842dbf87fc7e781a385f12
describe
'36846' 'info:fdaE20081130_AAAAACfileF20081130_AAADSW' 'sip-files00079.pro'
9a26eb77622f68b645c54c1b1fbbee6d
7e533d4d92981ab0baf6f4f39309e2820ddae56f
describe
'25058' 'info:fdaE20081130_AAAAACfileF20081130_AAADSX' 'sip-files00079.QC.jpg'
4c95059b29aedf8837aeb14051a0ace7
f59ccb7bbfd028b3dea285ca4350af879d8ec21c
'2017-08-14T14:27:30-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADSY' 'sip-files00079.tif'
902469b659589aad43b6c06989a627a7
6a6e9bda3c8c663493845d1677748cc7378fb3f2
describe
'1497' 'info:fdaE20081130_AAAAACfileF20081130_AAADSZ' 'sip-files00079.txt'
c4eda6bcbc2d0239b8d2619d55ac153a
3de0f2465d549a6b921fc80d63e222abe058339d
describe
'6520' 'info:fdaE20081130_AAAAACfileF20081130_AAADTA' 'sip-files00079thm.jpg'
f7ec203e028697145e441f132d7c3a27
6817f42a6fef0b17176a6f4dff64c146e32fe1d7
describe
'969965' 'info:fdaE20081130_AAAAACfileF20081130_AAADTB' 'sip-files00080.jp2'
2332fe21453aafc3b947789bc4c89480
04feff6f481adf1c085d811358fe9f0bee46738a
describe
'79020' 'info:fdaE20081130_AAAAACfileF20081130_AAADTC' 'sip-files00080.jpg'
49f0f184fce0d8a5428638a12e7991e5
9d96460a6d4761647c61b977c78a65ebbd59ccf6
'2017-08-14T14:31:25-04:00'
describe
'40009' 'info:fdaE20081130_AAAAACfileF20081130_AAADTD' 'sip-files00080.pro'
85b0851e1410b67d230c087b1b066801
c5634e4c416b71fcc767176a775daf24da22bee9
describe
'26895' 'info:fdaE20081130_AAAAACfileF20081130_AAADTE' 'sip-files00080.QC.jpg'
26eedd511a35f850f8ad38d02337d776
6f016e9a6b7f966e416278c82dedb32d13331988
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADTF' 'sip-files00080.tif'
3a553805b63472840faea57ea38fb894
bf791800677625acb3929ca5951420942c4642dd
describe
'1648' 'info:fdaE20081130_AAAAACfileF20081130_AAADTG' 'sip-files00080.txt'
06ef6d4ebde094c0eb59e9c2fcd90c93
9ce6afa70b67e922d06f2617155affd5a0393785
describe
'6944' 'info:fdaE20081130_AAAAACfileF20081130_AAADTH' 'sip-files00080thm.jpg'
07ca70e21b0b507ee07c7814c51bd9a3
445defcefa1aa9818ed0d5dc7372b9099b194e72
'2017-08-14T14:32:57-04:00'
describe
'969956' 'info:fdaE20081130_AAAAACfileF20081130_AAADTI' 'sip-files00081.jp2'
9e70950876c059fe9a2439af38431329
1455e715cbebb5ab45098306fa6fde564e521609
describe
'78585' 'info:fdaE20081130_AAAAACfileF20081130_AAADTJ' 'sip-files00081.jpg'
686c067a7e32ff5635ae7035435096ea
8b0c156559c204c9c1f77ede2077c93f9c5cfe1f
'2017-08-14T14:34:45-04:00'
describe
'40415' 'info:fdaE20081130_AAAAACfileF20081130_AAADTK' 'sip-files00081.pro'
b27f2f50cd200dcc4ba75d9b6820ecb1
6d52784e93118f0ff058c3a59c72c3aed5724c0b
describe
'26390' 'info:fdaE20081130_AAAAACfileF20081130_AAADTL' 'sip-files00081.QC.jpg'
f8b2309c9aea6db23e2d398eb73b88ec
e3f642745ba432b23316c37011a175777c425be7
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADTM' 'sip-files00081.tif'
e846c0b0900517aa85b853f7f35b6e5a
cd0310cdfd21c695555094e810ded571b4d46f80
'2017-08-14T14:29:17-04:00'
describe
'1635' 'info:fdaE20081130_AAAAACfileF20081130_AAADTN' 'sip-files00081.txt'
b9543933bc06de4200c9b393189784a4
614862dfc9c3a0bd52c4b2d646ae3393a7e89b84
describe
'6607' 'info:fdaE20081130_AAAAACfileF20081130_AAADTO' 'sip-files00081thm.jpg'
6ec774b6dd254fcffbd8333ba789b5a6
755f446fc93072fb0f5bf0a593c583e6de8901a5
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADTP' 'sip-files00082.jp2'
57cdab67c959ccadcbe6e70066f1546e
38fde751f26e378ad2112943bd8c8cbaf7b2cc7a
describe
'49197' 'info:fdaE20081130_AAAAACfileF20081130_AAADTQ' 'sip-files00082.jpg'
1b4bc7f7479081c863d1e986c8e2aa62
6068c941a3e207fddae668d54199941d57486ed0
describe
'23726' 'info:fdaE20081130_AAAAACfileF20081130_AAADTR' 'sip-files00082.pro'
442fc42fc29650b15909b02ee1840b31
9502a9714f319e7585b3e21c3201e1aa710da7f3
describe
'16420' 'info:fdaE20081130_AAAAACfileF20081130_AAADTS' 'sip-files00082.QC.jpg'
adb3a6bf9e17e6bf5f3322b31249214d
918b9a4b9896d7ca49dc0a19e5e6991c6598fa9f
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADTT' 'sip-files00082.tif'
697a82d0669f8326e991c6b35ea8a9b7
3ec71646c9bce0ae81ea609375c2f338845c08e9
describe
'1087' 'info:fdaE20081130_AAAAACfileF20081130_AAADTU' 'sip-files00082.txt'
9270b092bd892e295375fc1837d8fe7e
573f4590f8cd0426fc5fe3f526e8a2473794f894
describe
'4560' 'info:fdaE20081130_AAAAACfileF20081130_AAADTV' 'sip-files00082thm.jpg'
0a548b2cb212daf3f09a40914d971644
3b68b61159669e4c5202ccc7d7c558616d31c912
'2017-08-14T14:27:39-04:00'
describe
'1062537' 'info:fdaE20081130_AAAAACfileF20081130_AAADTW' 'sip-files00083.jp2'
0d718412853350d545e7646370fc6542
4307f04ec48d91706f6b22e2ca8b09f32aad5b8a
describe
'28689' 'info:fdaE20081130_AAAAACfileF20081130_AAADTX' 'sip-files00083.jpg'
0ad405305d5199c594d73ebf8450b470
1d2d77be29ef56bb8a3f3acd20f591eb42e16b26
describe
'6089' 'info:fdaE20081130_AAAAACfileF20081130_AAADTY' 'sip-files00083.pro'
e1510f613b5b1dece9a435aba255b908
99117a355b38f4ff2d5a9b94f22aba9d5791698d
describe
'9852' 'info:fdaE20081130_AAAAACfileF20081130_AAADTZ' 'sip-files00083.QC.jpg'
4930b5c1871229e191ab79427825b0a0
144346b57ca122381cec8a91eb4ccc7decf5c87c
describe
'8517128' 'info:fdaE20081130_AAAAACfileF20081130_AAADUA' 'sip-files00083.tif'
2e1bd0091da30b91dbe12fd789fa3ad1
f5ed3e84386e944e9da4a7090039633146b93edb
describe
'330' 'info:fdaE20081130_AAAAACfileF20081130_AAADUB' 'sip-files00083.txt'
1163620023d29b5b7d41be44acea2de0
52af604826076e4bab566aa4e6f4d6d40ce83f95
describe
'3462' 'info:fdaE20081130_AAAAACfileF20081130_AAADUC' 'sip-files00083thm.jpg'
2717036b4b27bf2431e8c65ac41df95f
fa1372201b81dae49db119d3751b03589ac38671
describe
'969902' 'info:fdaE20081130_AAAAACfileF20081130_AAADUD' 'sip-files00084.jp2'
5bb76d94d7a38d00916c51fec41cc9bc
94db3d6a9b257d5d6daccbf3d8463b61db12e6f1
describe
'57188' 'info:fdaE20081130_AAAAACfileF20081130_AAADUE' 'sip-files00084.jpg'
69ab4241e1a395da5b00768a8d0a3a1d
58d45c8c458dd28fce20a54a1f3652b1fc42cfb3
'2017-08-14T14:31:47-04:00'
describe
'28389' 'info:fdaE20081130_AAAAACfileF20081130_AAADUF' 'sip-files00084.pro'
26ca9d9eaaaf40e48ea09ff3065bbdca
b142d07e2a7d0f0237ff324fc7bc7939b6919fe9
'2017-08-14T14:31:14-04:00'
describe
'18774' 'info:fdaE20081130_AAAAACfileF20081130_AAADUG' 'sip-files00084.QC.jpg'
7c97be35c99cdcd7fedd79735ba365f9
47223d8ac1df6abf32ae0176b1b743e96568829f
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADUH' 'sip-files00084.tif'
8586cb0c7eaf57b65bae7b296f2253a6
2503f57fdc8752336d6b7efcb47f659ee912cd76
describe
'1260' 'info:fdaE20081130_AAAAACfileF20081130_AAADUI' 'sip-files00084.txt'
42a822bbe82bdf66db413250ed131812
a058a696b8488beb35be7cb848ff35f5e5714991
describe
Invalid character
WARNING CODE 'Daitss::Anomaly' Invalid character
'5521' 'info:fdaE20081130_AAAAACfileF20081130_AAADUJ' 'sip-files00084thm.jpg'
d0f940f82e53ed9f9056443b1e03348a
3b0a78637dd07c02ac31a7048bf27af5d0351459
'2017-08-14T14:33:32-04:00'
describe
'969960' 'info:fdaE20081130_AAAAACfileF20081130_AAADUK' 'sip-files00085.jp2'
da19bf7218675ee2054ee6553c62b7b1
931a5328d254c252b844eacfd5978f92b6766158
describe
'65571' 'info:fdaE20081130_AAAAACfileF20081130_AAADUL' 'sip-files00085.jpg'
669a33def8e661fb3d4c8a51e89b25d5
fddd6117fba3845cb427ad0f1df752acc25673ac
describe
'32615' 'info:fdaE20081130_AAAAACfileF20081130_AAADUM' 'sip-files00085.pro'
1a5d757ba2b672c3783e543acef78b55
786a8084ffaa8c55b54d27d2e5f0f50e2b7c1b50
describe
'21769' 'info:fdaE20081130_AAAAACfileF20081130_AAADUN' 'sip-files00085.QC.jpg'
7454218da1202b5e138792a5569928bc
ffb2d6a85c128025d68847c79a3b513ffd234067
'2017-08-14T14:32:11-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADUO' 'sip-files00085.tif'
0258c03c1754917cf31632b7bbf78a91
ba48286a17437d9a1f362bf1392939333f443466
describe
'1348' 'info:fdaE20081130_AAAAACfileF20081130_AAADUP' 'sip-files00085.txt'
033e842c91d50b259de5b852c12a81a4
9ef092462aa2821cdbd1751d08045bff45f66f52
'2017-08-14T14:34:40-04:00'
describe
'6060' 'info:fdaE20081130_AAAAACfileF20081130_AAADUQ' 'sip-files00085thm.jpg'
bddb414c1035d0c65f8cadb8e8b485d4
cd5b9e2638880c462296cfe0c3c71cc891605ca5
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADUR' 'sip-files00086.jp2'
d134d0a5470107951e9c38e37b8f8d44
fb82a32d776ace3c6fe916253ed7c2166caa344e
'2017-08-14T14:30:57-04:00'
describe
'59903' 'info:fdaE20081130_AAAAACfileF20081130_AAADUS' 'sip-files00086.jpg'
d97013bdb0e1f8a1686030f79aec5790
f5abd146ddc509d252aaeb5f1ab7286c3e6c9261
describe
'30016' 'info:fdaE20081130_AAAAACfileF20081130_AAADUT' 'sip-files00086.pro'
5450d74c5d1d5452687f2daf71a56e3f
f029f126e22db1620efb4430343cf6ebf519af55
describe
'20047' 'info:fdaE20081130_AAAAACfileF20081130_AAADUU' 'sip-files00086.QC.jpg'
7ea2ae95fe389c523978eb1a02673422
5a7296d0918fa8ae5e1ca0430ddf5b1302b5aae7
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADUV' 'sip-files00086.tif'
0b33cab4caed9f0993bde42d4b91a6d4
cd84e6d2f6b1affa5eb73f2e78ee52197bb8da72
'2017-08-14T14:27:36-04:00'
describe
'1261' 'info:fdaE20081130_AAAAACfileF20081130_AAADUW' 'sip-files00086.txt'
3419d8b8a59359db4faade3b0ab58afc
ad638078964b10b7e8a3c7335ced0db67cf06371
describe
'5519' 'info:fdaE20081130_AAAAACfileF20081130_AAADUX' 'sip-files00086thm.jpg'
c4a7346d3f2643c34abc081872f81393
468d9f61317ec9c29dee79f450634805d240739b
describe
'969905' 'info:fdaE20081130_AAAAACfileF20081130_AAADUY' 'sip-files00087.jp2'
8dec113f45a2f91838e62837badc53fa
4bb7b65ed366621da437e5cf06a45f1ed7f935cf
describe
'34824' 'info:fdaE20081130_AAAAACfileF20081130_AAADUZ' 'sip-files00087.jpg'
7ef88d8d188eed2588edc0fb2e8c57e8
5ca69d1ef0e0cff06e997e1cd1ff7478bcac4b0b
describe
'14671' 'info:fdaE20081130_AAAAACfileF20081130_AAADVA' 'sip-files00087.pro'
878d78dfa1ec342e0c880f4c221c9e2d
08aa880f83d0f72831561d9a0ee66a616339a42e
'2017-08-14T14:31:37-04:00'
describe
'11251' 'info:fdaE20081130_AAAAACfileF20081130_AAADVB' 'sip-files00087.QC.jpg'
e66e424e567d335920cf7a268efeaff2
3b42809736852f061c19522760ba41767464266d
'2017-08-14T14:34:08-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADVC' 'sip-files00087.tif'
43cfbc86b8b481bb61056f0e5ffb79d8
23b094bb53c9e3ef5b56e77af9466185bbfa93a9
'2017-08-14T14:29:09-04:00'
describe
'627' 'info:fdaE20081130_AAAAACfileF20081130_AAADVD' 'sip-files00087.txt'
78eafb006ef5ce52fc65dcd5bbe53051
95082ceb7847af0b564eb746a2697d08e36f15ba
describe
'3072' 'info:fdaE20081130_AAAAACfileF20081130_AAADVE' 'sip-files00087thm.jpg'
4354fea3d4a6bd5d6b096ae4a8615277
84c1cf40b1aa108a458e4fb85735935a838b9e27
'2017-08-14T14:31:26-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADVF' 'sip-files00088.jp2'
6ef9698b427d1d40db239fb053fe5d11
ea94e8a15cde17cdf11ac8bb8bc49c6c72996953
describe
'63070' 'info:fdaE20081130_AAAAACfileF20081130_AAADVG' 'sip-files00088.jpg'
5a2efa72555685694c86f9b2848c5dee
5309846008cdb57958308870bded54a36a30480e
describe
'29781' 'info:fdaE20081130_AAAAACfileF20081130_AAADVH' 'sip-files00088.pro'
a93ad319669fafd7f392b2098e618e36
f33ead93e52bddafd9c80e8e2e2e2267cb694ff7
describe
'20788' 'info:fdaE20081130_AAAAACfileF20081130_AAADVI' 'sip-files00088.QC.jpg'
5842be02d9de12f6c63e3199b7ce1cf5
120820cc76b7016b9021f9e3cdb60eea2afee786
'2017-08-14T14:31:12-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADVJ' 'sip-files00088.tif'
944bde44e0b94a6e2b929449a6919fab
5e854f5b11b3b628c2bd22a02d3350a48d1ca255
'2017-08-14T14:34:28-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADVK' 'sip-files00088.txt'
b45520064c9a6c4c7a3026c3892767a4
d94b874105180dc3073416601e395cd679b714dc
describe
'5432' 'info:fdaE20081130_AAAAACfileF20081130_AAADVL' 'sip-files00088thm.jpg'
0c0224009633ba9ba82e3ca3875bd897
0c3f859c2b62b97a650e940f8d82a070a7913ecc
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADVM' 'sip-files00089.jp2'
a86ef05c1c48831738f3521c128f710c
0856949bb92a5e88db14a366a0d962bdafc471e0
'2017-08-14T14:31:54-04:00'
describe
'77984' 'info:fdaE20081130_AAAAACfileF20081130_AAADVN' 'sip-files00089.jpg'
4ea813c2867030e0570f65c0717c9f27
5638d986d2aacb4cb5872588b3b495d86ee4742b
describe
'39669' 'info:fdaE20081130_AAAAACfileF20081130_AAADVO' 'sip-files00089.pro'
983c149db1e5a371a4c0aa29c3b106b8
83b2ad0d24d6ea7decf448461452147bcf914645
describe
'26446' 'info:fdaE20081130_AAAAACfileF20081130_AAADVP' 'sip-files00089.QC.jpg'
384ccd98bbeec515129e0988f6702499
809d63575965b3ea8a7573e54f00d71ca7a19397
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADVQ' 'sip-files00089.tif'
6900b59d36d69bac73d1827f79f2cfb0
66e6013edd8ab40257a0c60f194492ac4971388a
'2017-08-14T14:33:27-04:00'
describe
'1633' 'info:fdaE20081130_AAAAACfileF20081130_AAADVR' 'sip-files00089.txt'
929c4801558d7ad650255671491ae270
ed38c56b64441dc6484f7bd2faaee7fc1bb393c3
describe
Invalid character
Invalid character
'6883' 'info:fdaE20081130_AAAAACfileF20081130_AAADVS' 'sip-files00089thm.jpg'
04ef27a7371e9ebcba2d0f9ba49c97d0
c4c7fe79c5a532676b723c8d539751151ecadca2
describe
'969993' 'info:fdaE20081130_AAAAACfileF20081130_AAADVT' 'sip-files00090.jp2'
9dd591e5eb31c4e6ce21b2587548d43a
c2b106979174220287018d3ebda671df475a479f
describe
'80431' 'info:fdaE20081130_AAAAACfileF20081130_AAADVU' 'sip-files00090.jpg'
28cc065349894e3844f6a4983a211352
bbb979e99d6b135151ae83584eb96c6ff6cdc735
describe
'39063' 'info:fdaE20081130_AAAAACfileF20081130_AAADVV' 'sip-files00090.pro'
bbddcc84d622195d119cf7531d137180
330c276fa2c297b90549f907cac4a9fc0aba6563
'2017-08-14T14:28:03-04:00'
describe
'26150' 'info:fdaE20081130_AAAAACfileF20081130_AAADVW' 'sip-files00090.QC.jpg'
d32da8795e025424e14ada036f42dd5e
ef7af30473037963c78950be2b7cb1099e822ced
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADVX' 'sip-files00090.tif'
5fc2dcfc1f4cbe267ff2e47b1a6b7c93
a9f29b7aad62fe69a0c748153d9d75ebcffe7b80
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADVY' 'sip-files00090.txt'
c289f84e809b979152c6ef4c2012adf6
42a8f9571fab2b6c0d558db7ba47848c5c21a2c4
describe
'6788' 'info:fdaE20081130_AAAAACfileF20081130_AAADVZ' 'sip-files00090thm.jpg'
76c7431f1c082352303d6df23cb9ee3b
40fd035d7040264722c9b1bc3c7abbc17d1731c9
'2017-08-14T14:27:14-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADWA' 'sip-files00091.jp2'
29e2a707d02c949475b5b695bd6e326c
fc441468beb755dff921df1b3190c2441121aa9e
describe
'80696' 'info:fdaE20081130_AAAAACfileF20081130_AAADWB' 'sip-files00091.jpg'
f3d001f7e5f6bc6ef93e3f89ec9aa9b4
90d8973acb9662f61167e90129cef859d623d46b
describe
'41005' 'info:fdaE20081130_AAAAACfileF20081130_AAADWC' 'sip-files00091.pro'
291512e92d73abea3c22c94d69bffb48
6e7cdfddec9cd3b2e15b79c3da3aadf9b8169987
'2017-08-14T14:29:15-04:00'
describe
'27219' 'info:fdaE20081130_AAAAACfileF20081130_AAADWD' 'sip-files00091.QC.jpg'
32953e655fb56f5b0762a9ef25ce3be4
c45cfe74c64bfa726b1085077bf4189c1c249002
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADWE' 'sip-files00091.tif'
9d68493539f4c14858e2939aeae340c0
394330ea4c7b11a9ea34810abe27693e9a75d71e
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADWF' 'sip-files00091.txt'
a5fccad528aceb278b2af952ad205a1f
aed3888d7819eb1fc3cf3f9e316e919c1e8dc985
describe
'6899' 'info:fdaE20081130_AAAAACfileF20081130_AAADWG' 'sip-files00091thm.jpg'
fa8c71b26a2fefde2706bcdd003be92b
cc95186276d5aaeefa0a734982be764620a47a59
'2017-08-14T14:27:25-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADWH' 'sip-files00092.jp2'
cf9ff858251d73cd4d0d5d5d523d670a
821cdb92ade57817701ed07367e62bc7b16099cb
'2017-08-14T14:29:11-04:00'
describe
'77039' 'info:fdaE20081130_AAAAACfileF20081130_AAADWI' 'sip-files00092.jpg'
cd93153811a4e21ea3242217935ba950
a6e0b0901baf95802836acb95cf3b92999367123
describe
'38159' 'info:fdaE20081130_AAAAACfileF20081130_AAADWJ' 'sip-files00092.pro'
6c3484af042e1522d13dfdffea0e4e38
8626e2d363404a434d5e761daa15c0ea844c7142
describe
'25591' 'info:fdaE20081130_AAAAACfileF20081130_AAADWK' 'sip-files00092.QC.jpg'
52551b72a256f6d239f836db1d07c524
7a4ed8d661e66cfbc7b7721ed433d12bf114cab9
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADWL' 'sip-files00092.tif'
24596a2ffdf1977dea7bdc79e68075d1
c11395c18e630d71fddb76c9c0e834c0c3c5f017
describe
'1541' 'info:fdaE20081130_AAAAACfileF20081130_AAADWM' 'sip-files00092.txt'
0511ac504912b5569bd2fa35e426adca
90db764bf66857e0f52cc60f127611ab6de8c08a
describe
'6566' 'info:fdaE20081130_AAAAACfileF20081130_AAADWN' 'sip-files00092thm.jpg'
524fc2cecb78c6a92977dc812f982822
2e9eb6496fb007fac23cc62d58497811a1d0d9a8
describe
'969983' 'info:fdaE20081130_AAAAACfileF20081130_AAADWO' 'sip-files00093.jp2'
6bf5192ce3af8db6da926bd4be628455
92648726c93d671731a0cdda101d126efc710a27
describe
'81300' 'info:fdaE20081130_AAAAACfileF20081130_AAADWP' 'sip-files00093.jpg'
92bec50bbba303ea53e4ad6b0aabcc35
6d3fee2917301dad94870ffb194067ffd2f53199
describe
'41321' 'info:fdaE20081130_AAAAACfileF20081130_AAADWQ' 'sip-files00093.pro'
02f0ebf203da9f3f2bbe756fae6f6747
95ec900964d0a71ccb7a992b611c17db0b3dc965
describe
'27564' 'info:fdaE20081130_AAAAACfileF20081130_AAADWR' 'sip-files00093.QC.jpg'
fa6c2a73e5b8af9bf5523a7421549cc6
243f257364b4df062bdd6d96a6912fc5364c90b4
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADWS' 'sip-files00093.tif'
d157c3d4dd63c3a31e901d8178780e40
3ce39b2e5fe4649915f3bbb2cbd70a91f9a35156
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADWT' 'sip-files00093.txt'
53267d092f44af0fb57b834e3a871c8a
16d24917864b05190f7cc84777cc50f2bef5f639
describe
'6965' 'info:fdaE20081130_AAAAACfileF20081130_AAADWU' 'sip-files00093thm.jpg'
b1603e89a3b3d08faa01ed0f1567e7b2
c4657ee7ca2b1c6662cee6e72f25ccc0ed144f6b
describe
'1075758' 'info:fdaE20081130_AAAAACfileF20081130_AAADWV' 'sip-files00094.jp2'
e745c3f986a6bc8d021629c3d62730f2
f0cce720d44e6ced4719d0aa1478e2b4c6866f06
describe
'48490' 'info:fdaE20081130_AAAAACfileF20081130_AAADWW' 'sip-files00094.jpg'
b002a6bcd45a2854bdc44409883ed70e
0704fd8e3e75d88bb34d42052559e4d0204c83b9
describe
'6888' 'info:fdaE20081130_AAAAACfileF20081130_AAADWX' 'sip-files00094.pro'
608ec334688f429d1d1997f2c3d34231
787d0ed3b02d95ac45c7dd35044897114b022080
describe
'14940' 'info:fdaE20081130_AAAAACfileF20081130_AAADWY' 'sip-files00094.QC.jpg'
0ecc3db49eefc16697a02aa4a1d6c707
dcb251d9e030b8a51d22e596afbd3bcc6373a00d
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADWZ' 'sip-files00094.tif'
e0c5fe828903c68d63f5d6036dceb74a
2159e1881a340376f04fc128a3d4e42f5bdddacc
describe
'378' 'info:fdaE20081130_AAAAACfileF20081130_AAADXA' 'sip-files00094.txt'
2c5b517c087373877d44d8dcf7de1b58
d95cef993c313dcd67acf0931cbb485159444859
describe
'4405' 'info:fdaE20081130_AAAAACfileF20081130_AAADXB' 'sip-files00094thm.jpg'
6d899f8db1a845219d79d477c3964421
19a68a765955ed7125bdffe06d3e6ab0e99981aa
describe
'970007' 'info:fdaE20081130_AAAAACfileF20081130_AAADXC' 'sip-files00095.jp2'
a799b5668579ee2be1d28f92390decb0
80b759f54afd6ed99c4d9578bb97be0469c58200
describe
'73025' 'info:fdaE20081130_AAAAACfileF20081130_AAADXD' 'sip-files00095.jpg'
de841dd1ef874ab458a2be4f09fac48c
623b5a930206762c0403bf34982f41da8397e668
'2017-08-14T14:29:57-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADXE' 'sip-files00095.pro'
c8e9aabd60c32cb3a5c51a46632bc5b1
bab1635bfd1aa6444739de39dec59f41979c1262
'2017-08-14T14:33:19-04:00'
describe
'24777' 'info:fdaE20081130_AAAAACfileF20081130_AAADXF' 'sip-files00095.QC.jpg'
3cfaf7853f50ede850dee456c5c0af7e
85298f363ebe9b8da0bf9303760b737e3a2db379
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADXG' 'sip-files00095.tif'
b19352c696814a42f3ebbd80d770913e
191040fc0c5aeced39dbb7fe9bee625ca8e905dc
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADXH' 'sip-files00095.txt'
34170260a98fa2d57108d96f257617ac
ff973fb3866e86d8646b2ccf571b33856dba52f0
describe
'6668' 'info:fdaE20081130_AAAAACfileF20081130_AAADXI' 'sip-files00095thm.jpg'
99f37bcd10727ed05887d92410d54c01
602bc9aa7e74dada66f1dbb77e0e1d81a98cb5a7
'2017-08-14T14:29:35-04:00'
describe
'1051290' 'info:fdaE20081130_AAAAACfileF20081130_AAADXJ' 'sip-files00096.jp2'
147ec9f04d55050044ed4f8938ef7de1
6910da89372870190ad18cfa69e866279ea61972
describe
'41184' 'info:fdaE20081130_AAAAACfileF20081130_AAADXK' 'sip-files00096.jpg'
48895383dcdf6beae1e9693bfb60ecac
62095943e9e582844b6fbaa5d368af88747f29dd
describe
'4490' 'info:fdaE20081130_AAAAACfileF20081130_AAADXL' 'sip-files00096.pro'
679345c7911806b21fc0340a97a0dce1
2a98b3da11fad56c56f1b958929d4720e382fd41
describe
'13349' 'info:fdaE20081130_AAAAACfileF20081130_AAADXM' 'sip-files00096.QC.jpg'
be22ca4aa8b02922a348b35d9e4c3042
d03fb1ffe5a368d285d9f8dc8f49dcd041f09e5f
describe
'8426868' 'info:fdaE20081130_AAAAACfileF20081130_AAADXN' 'sip-files00096.tif'
b3d15721b7d14281d775cd94fae8cf69
7ade92f391abe7316d0089d781236b1f5f109ead
describe
'208' 'info:fdaE20081130_AAAAACfileF20081130_AAADXO' 'sip-files00096.txt'
4134aa229edde873c71151e5f41e119e
a4dbecc3c656290c29548436cceb91d698445469
describe
'4274' 'info:fdaE20081130_AAAAACfileF20081130_AAADXP' 'sip-files00096thm.jpg'
2eb9908ce4332785544c7ba925e2e50a
f26d18c3466000187ffb592ece316f7c6b4935d8
'2017-08-14T14:28:26-04:00'
describe
'1064977' 'info:fdaE20081130_AAAAACfileF20081130_AAADXQ' 'sip-files00097.jp2'
7707424357070773adb46e2b95708932
bf4f66982cdd4a2a5b91200e63f28716cb0b1054
describe
'48336' 'info:fdaE20081130_AAAAACfileF20081130_AAADXR' 'sip-files00097.jpg'
e09ff21abaa3f68fefc035e018da687f
6cdcb8213867d6804b7b6fbe1cc1eaaf2735cd84
describe
'9509' 'info:fdaE20081130_AAAAACfileF20081130_AAADXS' 'sip-files00097.pro'
412499c89fef735f750dd214e6d42c3b
ed22b8f2eb176979615ef68ddbaa08ede8145779
describe
'15342' 'info:fdaE20081130_AAAAACfileF20081130_AAADXT' 'sip-files00097.QC.jpg'
7c55d88b68554ce3dbc87e8912048539
d506604929c92df86760a1f7e4e31c1173f19d12
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADXU' 'sip-files00097.tif'
f2e9cf371511ba42ec4060c89f2d789e
c32646815cc9fc00e80d093b5e909454c16b4dff
'2017-08-14T14:28:39-04:00'
describe
'445' 'info:fdaE20081130_AAAAACfileF20081130_AAADXV' 'sip-files00097.txt'
08cd857fc7ea1b76a0ee98975befa474
3f49d80d957c3f7b98b372b7c353268faf65d73d
describe
Invalid character
Invalid character
'4584' 'info:fdaE20081130_AAAAACfileF20081130_AAADXW' 'sip-files00097thm.jpg'
20a3b8598b9ac5450b05662343677fc3
bc273cb34b1f9cbf2931cd2290540c713e01e806
describe
'1063092' 'info:fdaE20081130_AAAAACfileF20081130_AAADXX' 'sip-files00098.jp2'
a0b51e41b8b38369602d9b509c3e3a13
f94c5404cb2457adc4aec4f1acba386a24372c0b
describe
'45225' 'info:fdaE20081130_AAAAACfileF20081130_AAADXY' 'sip-files00098.jpg'
08045c248ab1fefa438dd7c9cbea33fb
f63c221d1acfea9ee71673133645bcb8003fc017
describe
'6658' 'info:fdaE20081130_AAAAACfileF20081130_AAADXZ' 'sip-files00098.pro'
b5c1dd51ff8198bf0a01ebbc799ca09b
c4f57f36e70f42eb21008ff07d97be0912035c0c
'2017-08-14T14:33:20-04:00'
describe
'14935' 'info:fdaE20081130_AAAAACfileF20081130_AAADYA' 'sip-files00098.QC.jpg'
1e6b432503019747d1a9fd2f77e3f969
574d21226dddfb83263a009b632a787d5b887439
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADYB' 'sip-files00098.tif'
c0d36add6dc44526fc152a045bf95b3a
1f7100c0b6c5009c85c6e308fc30fb8450f5fe9e
describe
'361' 'info:fdaE20081130_AAAAACfileF20081130_AAADYC' 'sip-files00098.txt'
87ed427b9fd314d8691e57070f7a0fc2
e7c92218b80b2746c0631e723c1ad4024c232dfa
describe
Invalid character
Invalid character
'4576' 'info:fdaE20081130_AAAAACfileF20081130_AAADYD' 'sip-files00098thm.jpg'
a0f95e8709fc70d24ffeb682e042e527
23e6c232a0f58304f3ebcbe00907e57960418790
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADYE' 'sip-files00099.jp2'
02a7b7c6d49d4bdfc264497335731f33
8bea4ebc21cb8703aef2bf6cc3af3aa7013b32c6
describe
'77424' 'info:fdaE20081130_AAAAACfileF20081130_AAADYF' 'sip-files00099.jpg'
99e7164c2560e848fd61a7677724a1cf
9a59db9ef8755a0d86fb4f524c3bba951cbd2e28
'2017-08-14T14:32:26-04:00'
describe
'39321' 'info:fdaE20081130_AAAAACfileF20081130_AAADYG' 'sip-files00099.pro'
194f1ebdd2e3bc7b9122c2ec098a1174
613ec9bcda3535d5da7caad92fd764a23abbb01c
describe
'26235' 'info:fdaE20081130_AAAAACfileF20081130_AAADYH' 'sip-files00099.QC.jpg'
e82a5eb3efbbaf4356c985d8bfc6f92f
3421826773bb177486c2c92babfe636f0c362bfb
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADYI' 'sip-files00099.tif'
52db2512a1d3c163ec50dac9a1c7d3b3
7b593fc0cb2317a4fb2cb94b0dfc5de76ee1e38f
'2017-08-14T14:28:54-04:00'
describe
'1606' 'info:fdaE20081130_AAAAACfileF20081130_AAADYJ' 'sip-files00099.txt'
3253809634e1a586a4fcde0b058b50e3
5a64ea628b5aa926e847d6f988411958ba18e9ab
describe
'6915' 'info:fdaE20081130_AAAAACfileF20081130_AAADYK' 'sip-files00099thm.jpg'
aa87aacb279bcfad329a627b10d80ac4
7ba0cd089ce7ca964eeaf60f3718bf0ce148abda
describe
'1051686' 'info:fdaE20081130_AAAAACfileF20081130_AAADYL' 'sip-files00100.jp2'
582e8250e1ee5922c838bbb71724e4f7
5f33a4890420771bd5c1ae2e33704635f0c12f76
describe
'28474' 'info:fdaE20081130_AAAAACfileF20081130_AAADYM' 'sip-files00100.jpg'
1e8292c7bedbec19c2f5527d9b48001e
dd7b5456be6b5ad7e3894304559383847bad4b8c
describe
'7429' 'info:fdaE20081130_AAAAACfileF20081130_AAADYN' 'sip-files00100.pro'
513813cf96a588b24a66c8027c91836f
24253e39705386e07b62b8e2bfb99fcfad67a585
'2017-08-14T14:28:35-04:00'
describe
'9794' 'info:fdaE20081130_AAAAACfileF20081130_AAADYO' 'sip-files00100.QC.jpg'
4d24e63cfa5b6339279e1992572d7ede
509c05da7afa22323e7f6c69bffccbaebf1b95f7
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADYP' 'sip-files00100.tif'
2484b2937d05cf8fc8f23e88f379a394
b7f9d44437e89042b082ecdba0dbf39d9842ea4b
'2017-08-14T14:30:46-04:00'
describe
'578' 'info:fdaE20081130_AAAAACfileF20081130_AAADYQ' 'sip-files00100.txt'
347419b8e53924e4eec228542d7e7f7d
c52b6ea1e0343f536211c43cb3066918273fa7d3
describe
'3442' 'info:fdaE20081130_AAAAACfileF20081130_AAADYR' 'sip-files00100thm.jpg'
2887b2a61fc746929776d75f503c8350
8a9ce877ffdddfd1119cc05c7026f59802528ad3
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADYS' 'sip-files00101.jp2'
5273974a3f77a64bba7bbccb7a4534c5
7ae36e137deb2b33aa0c39b8f6c71efd60bb55c0
describe
'79893' 'info:fdaE20081130_AAAAACfileF20081130_AAADYT' 'sip-files00101.jpg'
599ba75fa283ce7ad5144aa2a3f0f6be
291984054ac8ffb4beaebb0c660bb1393f30ffd2
'2017-08-14T14:28:14-04:00'
describe
'41211' 'info:fdaE20081130_AAAAACfileF20081130_AAADYU' 'sip-files00101.pro'
6fe347ecde7112a1ba06aa4b4570c841
3cf6e00aebdd4bb2fb605d0741aeb4095d4235c3
describe
'27335' 'info:fdaE20081130_AAAAACfileF20081130_AAADYV' 'sip-files00101.QC.jpg'
54b4bc30092cd1097bdb0634d013cc00
9954343a86eddf397197c3bcbb731d447e325628
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADYW' 'sip-files00101.tif'
71f7da36ec8963b9b57a0bd1fcb2a62b
32590dd87360c846bcb60a6a43b716e772e337c1
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADYX' 'sip-files00101.txt'
179ebdcb65e1e47254906d1fd462d9d7
9d3d144b7fe0bfd0c79ec0858c7b04315b729b6f
describe
'6874' 'info:fdaE20081130_AAAAACfileF20081130_AAADYY' 'sip-files00101thm.jpg'
c50ae5afa9d081fb1279dcee86e8fee9
b864cdd79c9436124de017635cfa5bb35c63b140
describe
'1053190' 'info:fdaE20081130_AAAAACfileF20081130_AAADYZ' 'sip-files00102.jp2'
94f5ed5783d37091397aee3af0e0da64
22aa7be48d4e69cbb78d654622edf435fc0c5d58
describe
'28470' 'info:fdaE20081130_AAAAACfileF20081130_AAADZA' 'sip-files00102.jpg'
0a9736d1f33a3f6039bf13a9880ab69b
20c109fc834541b79553728464464f4e412f9e9d
describe
'7343' 'info:fdaE20081130_AAAAACfileF20081130_AAADZB' 'sip-files00102.pro'
1c6098f1cb01c633fb72bf4f4500e16c
237969210459467a27a720cb7af32a8378a29530
describe
'10333' 'info:fdaE20081130_AAAAACfileF20081130_AAADZC' 'sip-files00102.QC.jpg'
5e08e0d39a6436311e68bd2e8bc14ad9
5249cd0029dba2139935fccc32a2398221f59e60
describe
'8442128' 'info:fdaE20081130_AAAAACfileF20081130_AAADZD' 'sip-files00102.tif'
c2d474695101436ff098d3d089b588d5
4c5315ee95a8c323b4ebbdf06ed6ae1c6dd7d5ed
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADZE' 'sip-files00102.txt'
0849d3d257344cafa2caef7c327c21ef
bfe966e35a923c8d3674e5773b5c699027ece4c0
describe
'3472' 'info:fdaE20081130_AAAAACfileF20081130_AAADZF' 'sip-files00102thm.jpg'
c98de55358c01ecb59fc6c09b7fd4e06
ad5ccb620ce69e2489cdb648065a94a843ef03db
describe
'969976' 'info:fdaE20081130_AAAAACfileF20081130_AAADZG' 'sip-files00103.jp2'
7fd6e1bbf35b9512b83c183a9bb95067
b21f93d5d4b8bce21d9f851314585ec640ae0dc0
describe
'79572' 'info:fdaE20081130_AAAAACfileF20081130_AAADZH' 'sip-files00103.jpg'
889b8e6aa2821fddbe547d5a97e5ab1b
5853630c2c4c39a8fd69278a15826b892005822b
describe
'39859' 'info:fdaE20081130_AAAAACfileF20081130_AAADZI' 'sip-files00103.pro'
b2a3da6d65e8bf88dba05cc578a36d19
eb9f0d9b6316db7cdf334a7d98a7d9b1d99c3c3b
describe
'26945' 'info:fdaE20081130_AAAAACfileF20081130_AAADZJ' 'sip-files00103.QC.jpg'
b47e02c3a5b089cedb0536c732b5821a
7a1d2a2360c7196936746f2b31a497b7565a2a79
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADZK' 'sip-files00103.tif'
e4e21ce6b136434d8f226d292821bed1
17f29190f948e7888e512bcd698211e2ca558729
describe
'1618' 'info:fdaE20081130_AAAAACfileF20081130_AAADZL' 'sip-files00103.txt'
8a38a08ff2e85953b323bd92f7f70b5c
7494485c861ffbf8ac5f150d399f87fcc2e7d521
describe
'6739' 'info:fdaE20081130_AAAAACfileF20081130_AAADZM' 'sip-files00103thm.jpg'
c61390f3fb9b7801b90962b40827fc90
59e658c953b23baac6c7bdda95cf2358b798d8a1
describe
'1051955' 'info:fdaE20081130_AAAAACfileF20081130_AAADZN' 'sip-files00104.jp2'
23b3a4055104976acf3cb23a3f229b68
3bfd6349540145d22f18dde00caffac789a8a083
describe
'43574' 'info:fdaE20081130_AAAAACfileF20081130_AAADZO' 'sip-files00104.jpg'
41f05d1e3879df0d22fee897a01bef3c
ce1a63c95dd985cdd5803834e663d1da23dfa1d6
describe
'5441' 'info:fdaE20081130_AAAAACfileF20081130_AAADZP' 'sip-files00104.pro'
4b7cffa999f7cb3d53921808cb0e787d
3d6c1096a9895f3963984df338cbbd464438a6f4
describe
'14427' 'info:fdaE20081130_AAAAACfileF20081130_AAADZQ' 'sip-files00104.QC.jpg'
d1f97fe7c45f1573719e6b01dbf83b95
955239371ccf8b4d44fa9436cad2300ff4e1e2fa
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADZR' 'sip-files00104.tif'
c7ccd44df1662b96fe144184110b7981
49fce6e54b720d6b6e14f04c6aa47dd77ba2ed15
describe
'251' 'info:fdaE20081130_AAAAACfileF20081130_AAADZS' 'sip-files00104.txt'
df4402592110df92c254d73beca894ba
dda06ae944aabe3c4ccfddc1fed69cc185735778
describe
'4505' 'info:fdaE20081130_AAAAACfileF20081130_AAADZT' 'sip-files00104thm.jpg'
ddf75794ec462cbb21ccfe14736aafb1
e37c467cda7c702a7d48398af0cb72cef5150aeb
describe
'970006' 'info:fdaE20081130_AAAAACfileF20081130_AAADZU' 'sip-files00105.jp2'
afd8e9b322e7f97488eb38b2bcdca626
58f128d4b919ef2d774f470e71568fa9d0f9b6c0
describe
'45419' 'info:fdaE20081130_AAAAACfileF20081130_AAADZV' 'sip-files00105.jpg'
09cb37dd164b992cf59959c8840ef428
6be538d49064c923b5e91fc1d876dc01f50b6501
describe
'6048' 'info:fdaE20081130_AAAAACfileF20081130_AAADZW' 'sip-files00105.pro'
4cce83f2e0b1689202198a299ff103a7
a27be13880b1ae6dbb77944ce96bf82aa0c5a213
describe
'14333' 'info:fdaE20081130_AAAAACfileF20081130_AAADZX' 'sip-files00105.QC.jpg'
d6997957ba8a5b65f956ae2365972ca1
c0822c36357502ece72cb71ce813fbbe2a8211cd
describe
'info:fdaE20081130_AAAAACfileF20081130_AAADZY' 'sip-files00105.tif'
e07aaf018a9f01b6ea83f84b4337eda5
e0dd7447d02b419479b7bc6f49c934314d915952
describe
'317' 'info:fdaE20081130_AAAAACfileF20081130_AAADZZ' 'sip-files00105.txt'
a3aa05a61ad02c0670b429b206d95de9
f857b672704837cea5ef163bafb459f0039c48bd
describe
'4352' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAA' 'sip-files00105thm.jpg'
e88467da0c10fa5516265741fd90e028
19108fa8bc9d1bf26b9c2ec943ada33ef52749ac
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEAB' 'sip-files00106.jp2'
cd969eccc58809cf4eea307f2c70335e
057f5e6d5a198d6500880c989e16e43d5b79b082
describe
'81377' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAC' 'sip-files00106.jpg'
ef5c0501c440c49e0a4bd10d4b1525fd
6682bc86bf90a6e37adb325cbd96b66d2e76cd88
describe
'42489' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAD' 'sip-files00106.pro'
639821db1619c487d341ca4049a88222
e8df003e1ccb4b2d273850a7f462e0e8c44a51ea
describe
'28001' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAE' 'sip-files00106.QC.jpg'
7d68ce1ae231a5087e8dfee44f917ec7
2fab20d57edb36c88e68a70f7eeffb8e12891b88
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEAF' 'sip-files00106.tif'
ae2cef5c064262c82e52b14fec651dd3
966e89511b3aa0c922268b290247977b0a6a9438
describe
'1701' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAG' 'sip-files00106.txt'
9b399c2a102e7cff425810f1397d8b40
5460e1f0984e623dc0fc34428587303a8d6c3524
describe
'7042' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAH' 'sip-files00106thm.jpg'
70fc6a080bb540bae63828bec7336857
ada89aefcd468cdb201177e98d42745a0709a052
'2017-08-14T14:34:12-04:00'
describe
'1053209' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAI' 'sip-files00107.jp2'
c2fb429e43cf16216098119b6a70d8a5
cd7a0c50b8445039bed45a767c7ca6b61571909a
describe
'34812' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAJ' 'sip-files00107.jpg'
49ee6d10ccfaec1fd8cd43fa780260c5
7b07b51e5e1e5a9d7b2966977f40713851b4cca6
describe
'11925' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAK' 'sip-files00107.pro'
1f80d20823630c0e8b7f24d4dd8e4a14
672883585f16bb9d92a09a9715dc8e6d939af415
'2017-08-14T14:29:22-04:00'
describe
'10983' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAL' 'sip-files00107.QC.jpg'
6aadccf3da0242dfba1288a8c085ab10
b62c95acbe77d5fc57321968369ed1d89565e4b8
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEAM' 'sip-files00107.tif'
a3e08f52092051322d86d3cfc70e446c
b9cbbc3e1162f3f7fa36f182a2862b35eb4ca28d
describe
'800' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAN' 'sip-files00107.txt'
7249bca970cd17659fe6eedf07708885
969e161a9568008f59dfe593e0bf6b38a8c699c4
describe
'3379' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAO' 'sip-files00107thm.jpg'
d5cbb45c46830be2af2be0e315cf029c
b72104fdcd6032bda1bd2634ddf452d3622962d9
describe
'1051207' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAP' 'sip-files00108.jp2'
13d922f41052364a0af940b056272ddf
f46d2eb5f85f40db3535ec4a258069d64ea02d06
describe
'34416' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAQ' 'sip-files00108.jpg'
6f56ebfd227b0757406ca316438eb195
4bdb0a2e1a067d4eaf0a73ebf87e815dc3264692
describe
'7512' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAR' 'sip-files00108.pro'
c7b7a9ddbf564a2e599222799c8f4d3c
740d516f7df712aca74672e7aa0efcf5e9cf6d54
describe
'11184' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAS' 'sip-files00108.QC.jpg'
0b84b2e82a929243e226c2bae0863565
add0f7cb8af37ebe19ef6e439f996c94c49949da
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEAT' 'sip-files00108.tif'
82e2f21d857e11aef537e6ff25bf7fcd
e900b05b5efcb6bb6e410dd53459b618e6c1f207
'2017-08-14T14:28:42-04:00'
describe
'325' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAU' 'sip-files00108.txt'
3bf9f014c66016b601e57ad1ee7da1eb
053b26568030f10fd2023cb3e10b21f36217d9ab
describe
'4088' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAV' 'sip-files00108thm.jpg'
da6388ba9ec970bbddb2aa2544249fc5
677c6b0cdfde38d19e44a00bb886cb3323372f4a
describe
'1063870' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAW' 'sip-files00109.jp2'
5a4064142380e8d9294ac19ef6746743
4c12fec312b883df9318c3991985b38d667fbf99
describe
'45116' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAX' 'sip-files00109.jpg'
5d7e3e16caa1ca29d241bbf423c72f9e
e6042d7de8109bb568147ab4c84a42aed2543c22
'2017-08-14T14:29:50-04:00'
describe
'13338' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAY' 'sip-files00109.pro'
61d48672bdb432e58ceebf4716d31c0a
c42ee659e843446fd7b96683c73c7a6ceb05bd15
describe
'14831' 'info:fdaE20081130_AAAAACfileF20081130_AAAEAZ' 'sip-files00109.QC.jpg'
97742dfe63d446b09ae39e4f295ec9d5
b44cefc16abf5de94572c6c9f090ee0d2ef6903a
'2017-08-14T14:33:21-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEBA' 'sip-files00109.tif'
7cdbcf36d00f68149c9f6f23ac501e9e
ce948935f8838cffca0a08bd800a26993999e415
describe
'1015' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBB' 'sip-files00109.txt'
48fa4fe020f4adc2731c00765bbedd23
9962dbbd9f57689201e561365da811e187a227a2
describe
'4546' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBC' 'sip-files00109thm.jpg'
f100fbdc1e71d98a1718d014493fe1c5
301a43f06008e99a97a7830bcdffa2913ef34371
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEBD' 'sip-files00110.jp2'
8c0fa277163209d79a733bbd4e7162dd
2120fb6d4b68e19803ad51907c69d25482088ef4
describe
'76488' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBE' 'sip-files00110.jpg'
64eb1499649faef707116f7c9fbbc80c
24475a6cca16579662a6316f2a43362a34b54904
'2017-08-14T14:33:24-04:00'
describe
'39158' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBF' 'sip-files00110.pro'
e488e5e6903b0019c420a167c9a9a7dd
d11b9b665bb5e83275a804075abc23e1aac9c7ef
describe
'25974' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBG' 'sip-files00110.QC.jpg'
70a69c12b88e01c934e64dd38b3032e2
9c2a1564a70fd29a14947cbaceb841c8f7019230
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEBH' 'sip-files00110.tif'
63e5c5a8a4f134ba85e122db53d31089
5201bb9c55041fb7bab548f6b1e2244ecc76081f
'2017-08-14T14:31:46-04:00'
describe
'1614' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBI' 'sip-files00110.txt'
a844d6ef8444c0f2f9df9c71ed48a522
7659aada3a8ed3f9d48776fd00d6262a4300a1d2
describe
'6650' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBJ' 'sip-files00110thm.jpg'
8a01699ccc7a0fc248438c5261c77987
fc6821029e2f48d76f54ec553e5b7846832833dc
describe
'1076358' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBK' 'sip-files00111.jp2'
7bf4e099663bade7d096743fee0e1d6e
8b6e6b7863346a3b93ad1877e807c8e908257d18
describe
'44752' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBL' 'sip-files00111.jpg'
132e3db9bff1c7d03917f43e1aa09791
45856f0445684b6e810a7e677431fd389eddf7bb
describe
'4992' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBM' 'sip-files00111.pro'
5b5663aa328efc8db897f3b496a0f025
1a8a61dd2cb6cb420beddbb1279c115cba2beeba
'2017-08-14T14:31:58-04:00'
describe
'15198' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBN' 'sip-files00111.QC.jpg'
cd6d1f74ba31548cbcd10a4a49e8652e
4b24ce592f58c0a783060555301262315dde0324
describe
'8628448' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBO' 'sip-files00111.tif'
ae2da103ea187a6b92c7a172f9d75cf7
3b734235b6fd720d714332a9f494f47f7f2d1629
'2017-08-14T14:31:27-04:00'
describe
'213' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBP' 'sip-files00111.txt'
d3eb83b81a755f8822a12cb627aed804
2d40dcc947eee99d10644a3b08313c4cfcf91bef
describe
'4761' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBQ' 'sip-files00111thm.jpg'
9a8b45195c36bb74501628c943990b98
1cbd87da516accdbcbd9a64fdab2da8a487e0a7f
describe
'1063226' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBR' 'sip-files00112.jp2'
4f4b312f9d5cc1f1a25db87b75dec982
3dd4e2c148d442e52d3b4a4ec7c25133c52eddf4
describe
'40001' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBS' 'sip-files00112.jpg'
18bc9ee44c5ba4218ffb7a4406bbdb29
d082e274c1850b78c9aeaf14d6a3cfc93bb30536
describe
'3734' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBT' 'sip-files00112.pro'
dac0658a026305554b4b57f71d6cb12b
1eaccc74e8c0e09f7900d90132ab620e02e20ee9
describe
'13889' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBU' 'sip-files00112.QC.jpg'
76c705304cc1b8db25c36a9a4c9d0df1
f33547b92855eabb2e4345be81af719f96c010ef
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEBV' 'sip-files00112.tif'
883c58f499bc6c9f1f67e4a279a3ef01
513627adea811158bbf227898fcf3d2f0ebd6aa6
'2017-08-14T14:33:15-04:00'
describe
'263' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBW' 'sip-files00112.txt'
0cee3c044d1fec248861958947b6fdf9
590cfa2b81341a555e51bd51a0609543aca96065
describe
Invalid character
Invalid character
'4436' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBX' 'sip-files00112thm.jpg'
6661e625e04d104b56d60b4edb70462d
e0bca39da8901737abcffadda7b917e7f091d674
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEBY' 'sip-files00113.jp2'
453850027af169e724cce05a28a2e119
02b8ec719af57882668a413314ff3f46789ef2b3
describe
'75699' 'info:fdaE20081130_AAAAACfileF20081130_AAAEBZ' 'sip-files00113.jpg'
c596f48d96ec7482ebf5a03127d52028
2c317ccecbd4ae1518da341b92938b76c2735cf1
'2017-08-14T14:28:19-04:00'
describe
'38262' 'info:fdaE20081130_AAAAACfileF20081130_AAAECA' 'sip-files00113.pro'
6749b2cb79fd4264e13cd9af06669e97
eb61b20d7fedb651f8a650f272b84d6541ffcab4
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAECB' 'sip-files00113.QC.jpg'
a0002db99acbf231c7893fe69ed13f2f
a54964b55a1522c7a059880581fc07058b41b6b1
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAECC' 'sip-files00113.tif'
b1109b6a8598eb84197ced0f7c2daf1d
eb5cbb3b68add99bc4635205fab1fa583eb6715a
'2017-08-14T14:34:17-04:00'
describe
'1559' 'info:fdaE20081130_AAAAACfileF20081130_AAAECD' 'sip-files00113.txt'
ce23f104b4dcb4b436015054f57bb9c6
59d5415a244300a6060f29123bee013b6e72e77e
describe
'6621' 'info:fdaE20081130_AAAAACfileF20081130_AAAECE' 'sip-files00113thm.jpg'
9e1b65a988c7e4f123dcf648d0f127f4
3116ba82b16820cf04e7d251c58f5901a0656f8a
describe
'1062596' 'info:fdaE20081130_AAAAACfileF20081130_AAAECF' 'sip-files00114.jp2'
b0c14583666ef400bbc2ce39ee5c437c
c8a861ad72c4f81607e236dc9dbdfab4e3af6d18
describe
'44135' 'info:fdaE20081130_AAAAACfileF20081130_AAAECG' 'sip-files00114.jpg'
fbe4d49f1786bd842ef925f4c3533f66
dfdb4ebe711043156c843c07c508dde883133ad9
'2017-08-14T14:28:04-04:00'
describe
'7243' 'info:fdaE20081130_AAAAACfileF20081130_AAAECH' 'sip-files00114.pro'
a095ff8d4ff8f04d15cd21500435789d
ecce164b8433679b3ec9d5b043a4f4f897b5be97
describe
'14761' 'info:fdaE20081130_AAAAACfileF20081130_AAAECI' 'sip-files00114.QC.jpg'
d79013d54c895bda433b02ad8b4f8fac
0674b084c5dd665afc330dc83b433e49f2f08006
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAECJ' 'sip-files00114.tif'
4275622619f2953a89ae4eb86f4ee42d
07fef1473b1b292fbd1f8886af7e2d2e52a03ae6
describe
'331' 'info:fdaE20081130_AAAAACfileF20081130_AAAECK' 'sip-files00114.txt'
41cf71d5f32bd472e3c27009d2e038a9
fbe494757b8eeef15b5a0d1e3d34770abeb3df8e
describe
'4726' 'info:fdaE20081130_AAAAACfileF20081130_AAAECL' 'sip-files00114thm.jpg'
44cec80cc8fbb56bc363da1fc21dd21e
977b5f4830c19c52a710cdfb321d906c849c96b7
describe
'1063824' 'info:fdaE20081130_AAAAACfileF20081130_AAAECM' 'sip-files00115.jp2'
9499b166f83464fc2a2543c9696ba1c5
464fcfcd45e4299de5c46cfbc8f3ad127d59a0a2
describe
'32482' 'info:fdaE20081130_AAAAACfileF20081130_AAAECN' 'sip-files00115.jpg'
c451758e8b9559fa2cd70722bd206beb
52339306e468b0afe8f6f8f4f20d5bb4f3f7a94b
describe
'4038' 'info:fdaE20081130_AAAAACfileF20081130_AAAECO' 'sip-files00115.pro'
01ef2667a03758a74cf4297cd61a9294
8871034804b219e0efd0a5b17ded2f85c804c28e
'2017-08-14T14:29:47-04:00'
describe
'11015' 'info:fdaE20081130_AAAAACfileF20081130_AAAECP' 'sip-files00115.QC.jpg'
662f1067d22964b139d780d42651b718
2b8f19433955182b3627d1b8ec674b8920e4dd8e
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAECQ' 'sip-files00115.tif'
0d8e00b5e1c2b083c1fb24f08ed4bd4a
00f5bd4fcd11e7f86930e1d8ec1cb444cb510a4c
describe
'381' 'info:fdaE20081130_AAAAACfileF20081130_AAAECR' 'sip-files00115.txt'
cd9fe1b70857a64ac7d126f742e40f55
dbfdbcedd20db44a4652b9dc45bedfbdf7df9679
describe
Invalid character
Invalid character
'3574' 'info:fdaE20081130_AAAAACfileF20081130_AAAECS' 'sip-files00115thm.jpg'
544202a6afc113d9c8d8b89b155c6cfd
c07a9663c588984f5bb354a53da1f0a8b80675b0
describe
'1063809' 'info:fdaE20081130_AAAAACfileF20081130_AAAECT' 'sip-files00116.jp2'
441c0b8dca83d992f59774a9b8cdc07a
6008c3794c42b563ba64c00bd1301174405cafe1
describe
'34314' 'info:fdaE20081130_AAAAACfileF20081130_AAAECU' 'sip-files00116.jpg'
b78799cc9edfd6fe6d73a519ebffa930
2f65ef157277422f98bb12e84d5a83db0449ee12
describe
'8753' 'info:fdaE20081130_AAAAACfileF20081130_AAAECV' 'sip-files00116.pro'
b1e8b0cfef678d26c67da8b383cefc88
ef9e62e897b9182903965215e2b7c6fb3a8ce5b4
describe
'11420' 'info:fdaE20081130_AAAAACfileF20081130_AAAECW' 'sip-files00116.QC.jpg'
91fece9f8208718cd9ef349d001c5f3e
fc117ea9f50b76b61a970d1212d30afedd7825ab
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAECX' 'sip-files00116.tif'
f96bc654e0e7acc1bcd297a4fa686ff5
bfd3e284a834f238f42b134a18b5bae325570fb5
describe
'618' 'info:fdaE20081130_AAAAACfileF20081130_AAAECY' 'sip-files00116.txt'
f741f40c473894f52aa452bb019efb01
0b99fcbd394e92ad0d82a45b42312261edb971f8
describe
'3723' 'info:fdaE20081130_AAAAACfileF20081130_AAAECZ' 'sip-files00116thm.jpg'
88be66f9fa52e20c257862d0dde17d1f
2cc4a9019bf3473de4f2e82880bb40fb3378ddd6
describe
'1063690' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDA' 'sip-files00117.jp2'
788d76d5d8407cc78444f0a17f547871
614c1088e1f9c6d20b7508e01edc0fdb0cc8a153
describe
'45938' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDB' 'sip-files00117.jpg'
92b45e8d7f20a7787b9c170af28f52da
a6f8d78245db829e0912854949fed1fcadc843fa
describe
'7810' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDC' 'sip-files00117.pro'
55cc1fb4ca418de0d353c94aef412713
5f282482d5b0165970caa2c3a2cbf7fd79eae831
describe
'14782' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDD' 'sip-files00117.QC.jpg'
9c938f81eca712990aa9ad2f2cd6b84b
e5a0c3431e5029447e0145197869c0eab743891e
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEDE' 'sip-files00117.tif'
a76f7ae162c4141134bbb16c1286f3d2
41f18d5bdab52724a3921b3b4d7f59b4432dd9d0
describe
'352' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDF' 'sip-files00117.txt'
01184d45c3a8f08a7c7a026a164a0c85
673358bb6a01abb0e4cbba7d71a86e7a0a171314
describe
'4451' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDG' 'sip-files00117thm.jpg'
4c70e184ea37abed983f99d09e94f3aa
c4716e022e173a0c296ef098fda03a10a6a83ae4
describe
'969801' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDH' 'sip-files00118.jp2'
bc48c7e57aa88da5ad62619c93c5d1d1
57169d7764c2258c9016f2e7c139e94ff3fa8bb2
describe
'65100' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDI' 'sip-files00118.jpg'
7b9e404f15a9d72c870d3338c7275d69
d8a5d3fb386ed1aa41d1153ddd0a50f58869cea7
describe
'32253' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDJ' 'sip-files00118.pro'
dcc8647ca50bdb86c944e3ef14d9dde8
c03a2a7943ea0769ef7d861ca7edac581a0e60b4
describe
'21913' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDK' 'sip-files00118.QC.jpg'
827ac2a3afd0799f9061993e79c75225
8ee40b972fa31c716d431f5d748718ab6ab6c460
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEDL' 'sip-files00118.tif'
a4b35e8c2fc3cddbdb8a545049cb741f
165ff585734e9164508ccca42730dedc12495877
describe
'1323' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDM' 'sip-files00118.txt'
37a00642602dbab5e5c4d40fb32cd9e2
1a98276c8a7dcc85c1d9745c7e7d4bae3a136d93
describe
'5455' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDN' 'sip-files00118thm.jpg'
4ff77254f7b692f8c6b045b0abfc4b31
d8b1f9dd3fd5620d273623130cbd0723573526ba
describe
'1062567' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDO' 'sip-files00119.jp2'
4f89afdd8cee4403a1c9cae2fbd55d6b
1e5e2afba2795627c1cfb72010be4d1f6df76fb9
describe
'35256' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDP' 'sip-files00119.jpg'
c55ba96b5747e81bb8123761d3efedad
c535ef6efa9c80c2f442431cb6d0766d1f930bea
'2017-08-14T14:27:21-04:00'
describe
'6826' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDQ' 'sip-files00119.pro'
3df91996ca0a057a4f127ed2fd06bf1e
6c184ac529f0ffe5c33aff79e15e483b8f07254b
describe
'11698' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDR' 'sip-files00119.QC.jpg'
3bf4446044307d13819533aee4bf9cd7
c5d9233ccc8912fb8cab8c68e018ab51aa9c3955
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEDS' 'sip-files00119.tif'
8e0a7d7c1f67dbeb1e86ffb5077e1b7e
12fbcb534cb97a627106a33463fec3bd6030c0e9
describe
'281' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDT' 'sip-files00119.txt'
aeee529d70389e5bad57989ec3680cd8
b564ce81c9bbbefedc77e90e67359cd5b7931c09
describe
'3799' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDU' 'sip-files00119thm.jpg'
232af09445a323493d47c33fad0d08bf
5a8fe478b8742bf5594218eb072c309ddb024b3f
describe
'1063856' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDV' 'sip-files00120.jp2'
cb94f56a3d4c1cfe951217db545ab20f
871993b0e5b5e8bf35bf3f07dbf2f27295b212f4
describe
'36263' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDW' 'sip-files00120.jpg'
f53a3f503c11ed9e666fdd2ee4e3f818
77653733cb0163db67db9fb36998ecaf1a5724d4
describe
'7375' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDX' 'sip-files00120.pro'
1ecfd998e3fc3f7970f267db3f021de8
b1a4da73563c87758a1a7126f7b7fd6ee4eadc24
describe
'12157' 'info:fdaE20081130_AAAAACfileF20081130_AAAEDY' 'sip-files00120.QC.jpg'
3c4e7fe312dbf84b0d378fb8d832a598
f45a11dfc8b0e885aa807d69cfabaf73b8e8f600
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEDZ' 'sip-files00120.tif'
faad0e1efcbe9176a7ae1e5ca6f8f24d
9497d9e3ddc89e212fced8239b16f913d434a2fe
describe
'474' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEA' 'sip-files00120.txt'
5152c006cef27cc0d38af75dd9691e3e
df25fa55fc66420b55c28a96b1a78d239e346041
describe
'4105' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEB' 'sip-files00120thm.jpg'
b4b41ad3f14412a20b24b653ccd34809
f6d3fba74c74b4d05e22c8fe82baf42260b6cbf5
describe
'969796' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEC' 'sip-files00121.jp2'
32c2f64964f29608665c50a36de9144d
a58032d6e81a42337a31c6e462581f78fa3a1907
describe
'59862' 'info:fdaE20081130_AAAAACfileF20081130_AAAEED' 'sip-files00121.jpg'
a8fc9abc8d2030e4ea44b779e324ab9c
05c29fc208ff93458164559add735588e333719a
describe
'29601' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEE' 'sip-files00121.pro'
c60e4940d135dbe2d82b5377e3cb92e5
c1249701e2413b6a8f1fcf734a4740b5fde38e34
describe
'19763' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEF' 'sip-files00121.QC.jpg'
5e5c2e000d9f67cbf053d022fea904d0
bc8edb1bf1fdf1963c293e4c7d5ef21927ffa518
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEEG' 'sip-files00121.tif'
e23f4fb67402c60e777946581f74c214
075b114c3741986246537a02974323ad639d66e6
'2017-08-14T14:33:36-04:00'
describe
'1310' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEH' 'sip-files00121.txt'
498c968815d5574eb157948aebcc5bbd
0c2c48b038c7b9a865947dfeaec9a151d25e5310
describe
'5252' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEI' 'sip-files00121thm.jpg'
67a931dc4db10a6a60624cbf7c5d3e29
a903b77592b360378a634a3c3350c607ac710a88
'2017-08-14T14:34:38-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEEJ' 'sip-files00122.jp2'
77e56c10e247fd654e72918deefc1173
9df13ba4ada0cbab1fac4f60366415ca2bd69f2d
describe
'75705' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEK' 'sip-files00122.jpg'
3fc1bd24d78ab1cfdb076ef1265e0a9a
9ddb599a99de1f4dcddd022196b14f159218e004
describe
'37735' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEL' 'sip-files00122.pro'
f9af5ad2ca8996f35d5a7126e2b2cf6f
8253a5485b75cd6a5a7c64146b73c2da5bc25cc6
'2017-08-14T14:28:55-04:00'
describe
'25149' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEM' 'sip-files00122.QC.jpg'
726ff339176ea4edf227fca18c3a4b2e
2b2a0eb0f8e9cebcf2fb2344666c07ec7b90f860
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEEN' 'sip-files00122.tif'
11be52a9dd9a5352afad733d96648798
34e1a8e151a60648af611faf53d5e32c66a38eb7
'2017-08-14T14:28:22-04:00'
describe
'1568' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEO' 'sip-files00122.txt'
1673d20a852e341a52698075bc4eb8c3
b7bb2e02dc5559a08aced9b8e56b7ca2c29d3af2
describe
'6541' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEP' 'sip-files00122thm.jpg'
99bceda6960d57aa230762a45425082b
952ca5838e3379202d09c995eaea9bd084122c30
describe
'970008' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEQ' 'sip-files00123.jp2'
5d52684a78dc95f77e4162df80ef4560
11542aa8b51993348eb87c96c3b44c44f2618f08
describe
'75361' 'info:fdaE20081130_AAAAACfileF20081130_AAAEER' 'sip-files00123.jpg'
bb5ba1bc61f742d3d0e6c1c200086239
7eea3e413e29f334acb5ae68077a55d25314370f
describe
'39303' 'info:fdaE20081130_AAAAACfileF20081130_AAAEES' 'sip-files00123.pro'
de06fd5dbe6a2c831c77d41539759c15
ea30bbe219b9840dd8b75dce21b7ff4de0507f5d
describe
'26364' 'info:fdaE20081130_AAAAACfileF20081130_AAAEET' 'sip-files00123.QC.jpg'
2a93e53efeefa3b1662b2273f3bd9ca0
4d53db23f20664f9f983424b61d11cffc7b2bee0
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEEU' 'sip-files00123.tif'
669433d15f32de8164c608965de77a7f
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describe
'1610' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEV' 'sip-files00123.txt'
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describe
'6581' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEW' 'sip-files00123thm.jpg'
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'2017-08-14T14:32:24-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEEX' 'sip-files00124.jp2'
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describe
'64512' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEY' 'sip-files00124.jpg'
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describe
'31828' 'info:fdaE20081130_AAAAACfileF20081130_AAAEEZ' 'sip-files00124.pro'
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describe
'21820' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFA' 'sip-files00124.QC.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEFB' 'sip-files00124.tif'
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'2017-08-14T14:29:36-04:00'
describe
'1372' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFC' 'sip-files00124.txt'
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describe
'5817' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFD' 'sip-files00124thm.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEFE' 'sip-files00125.jp2'
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describe
'33286' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFF' 'sip-files00125.jpg'
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describe
'14019' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFG' 'sip-files00125.pro'
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describe
'10790' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFH' 'sip-files00125.QC.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEFI' 'sip-files00125.tif'
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describe
'580' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFJ' 'sip-files00125.txt'
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describe
'2977' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFK' 'sip-files00125thm.jpg'
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'2017-08-14T14:28:17-04:00'
describe
'969996' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFL' 'sip-files00126.jp2'
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describe
'54379' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFM' 'sip-files00126.jpg'
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describe
'25442' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFN' 'sip-files00126.pro'
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describe
'17610' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFO' 'sip-files00126.QC.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEFP' 'sip-files00126.tif'
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describe
'1058' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFQ' 'sip-files00126.txt'
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describe
'4582' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFR' 'sip-files00126thm.jpg'
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describe
'1051902' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFS' 'sip-files00127.jp2'
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describe
'34470' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFT' 'sip-files00127.jpg'
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describe
'11606' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFU' 'sip-files00127.pro'
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describe
'11306' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFV' 'sip-files00127.QC.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEFW' 'sip-files00127.tif'
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describe
'900' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFX' 'sip-files00127.txt'
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describe
'3810' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFY' 'sip-files00127thm.jpg'
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describe
'1051936' 'info:fdaE20081130_AAAAACfileF20081130_AAAEFZ' 'sip-files00128.jp2'
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describe
'39995' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGA' 'sip-files00128.jpg'
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describe
'14698' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGB' 'sip-files00128.pro'
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describe
'13141' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGC' 'sip-files00128.QC.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEGD' 'sip-files00128.tif'
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describe
'1040' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGE' 'sip-files00128.txt'
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describe
'4301' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGF' 'sip-files00128thm.jpg'
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describe
'1051838' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGG' 'sip-files00129.jp2'
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describe
'25544' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGH' 'sip-files00129.jpg'
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describe
'1781' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGI' 'sip-files00129.pro'
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describe
'8587' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGJ' 'sip-files00129.QC.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEGK' 'sip-files00129.tif'
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describe
'82' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGL' 'sip-files00129.txt'
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describe
'3065' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGM' 'sip-files00129thm.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEGN' 'sip-files00130.jp2'
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describe
'87713' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGO' 'sip-files00130.jpg'
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describe
'47349' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGP' 'sip-files00130.pro'
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describe
'25405' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGQ' 'sip-files00130.QC.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEGR' 'sip-files00130.tif'
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describe
'1921' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGS' 'sip-files00130.txt'
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describe
'6412' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGT' 'sip-files00130thm.jpg'
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describe
'970036' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGU' 'sip-files00131.jp2'
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describe
'94862' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGV' 'sip-files00131.jpg'
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describe
'50900' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGW' 'sip-files00131.pro'
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describe
'27937' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGX' 'sip-files00131.QC.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEGY' 'sip-files00131.tif'
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describe
'2071' 'info:fdaE20081130_AAAAACfileF20081130_AAAEGZ' 'sip-files00131.txt'
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describe
'7327' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHA' 'sip-files00131thm.jpg'
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'2017-08-14T14:27:58-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEHB' 'sip-files00132.jp2'
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describe
'97701' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHC' 'sip-files00132.jpg'
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describe
'53856' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHD' 'sip-files00132.pro'
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describe
'28082' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHE' 'sip-files00132.QC.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEHF' 'sip-files00132.tif'
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describe
'2189' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHG' 'sip-files00132.txt'
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describe
'7142' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHH' 'sip-files00132thm.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEHI' 'sip-files00133.jp2'
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'2017-08-14T14:32:28-04:00'
describe
'95015' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHJ' 'sip-files00133.jpg'
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describe
'52214' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHK' 'sip-files00133.pro'
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describe
'27675' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHL' 'sip-files00133.QC.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEHM' 'sip-files00133.tif'
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describe
'2130' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHN' 'sip-files00133.txt'
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describe
'6952' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHO' 'sip-files00133thm.jpg'
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'2017-08-14T14:29:28-04:00'
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEHP' 'sip-files00134.jp2'
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describe
'97514' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHQ' 'sip-files00134.jpg'
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describe
'53703' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHR' 'sip-files00134.pro'
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describe
'28106' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHS' 'sip-files00134.QC.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEHT' 'sip-files00134.tif'
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describe
'2195' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHU' 'sip-files00134.txt'
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describe
'7298' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHV' 'sip-files00134thm.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEHW' 'sip-files00135.jp2'
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describe
'91634' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHX' 'sip-files00135.jpg'
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describe
'49518' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHY' 'sip-files00135.pro'
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describe
'26744' 'info:fdaE20081130_AAAAACfileF20081130_AAAEHZ' 'sip-files00135.QC.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEIA' 'sip-files00135.tif'
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describe
'2002' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIB' 'sip-files00135.txt'
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describe
'6408' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIC' 'sip-files00135thm.jpg'
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describe
'1051874' 'info:fdaE20081130_AAAAACfileF20081130_AAAEID' 'sip-files00136.jp2'
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describe
'39907' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIE' 'sip-files00136.jpg'
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describe
'18652' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIF' 'sip-files00136.pro'
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describe
'13644' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIG' 'sip-files00136.QC.jpg'
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describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEIH' 'sip-files00136.tif'
7183e0bc9a22ef9383cf7f6ca6790010
ec98c3b82deebd655ec43e6ef91f0a54ea9ee17a
describe
'796' 'info:fdaE20081130_AAAAACfileF20081130_AAAEII' 'sip-files00136.txt'
f3a0da1e9068b273bad318a6d6fc4f25
536829143903a7e03397b22901cfbb3c13b96b7a
describe
'3857' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIJ' 'sip-files00136thm.jpg'
e096f4b4aecab44add72fa7ae789c9fa
0e06683f343cb5cea324f0a53383414127989e51
describe
'1060384' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIK' 'sip-files00137.jp2'
bac819f497bae3ff09f6360aee429845
ee42cb2940adf9a0a4556459959e620e75c181dc
describe
'64782' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIL' 'sip-files00137.jpg'
fbd77fab1e41a13151ffe3709f4d0032
9ae4c5759e8e285ed1c0c6e489d5487c4e5cbc75
describe
'31170' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIM' 'sip-files00137.pro'
461aaccbee7f8322933fc968fa8ac622
0db925624060f0fde3baf9a84404ce8c154f9a10
describe
'17694' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIN' 'sip-files00137.QC.jpg'
8233f98ea2e4e08bfeb7b597bdc8aaca
746a243efa84577482716ec549b929f47e08c752
describe
'8499768' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIO' 'sip-files00137.tif'
2195ef29058e91981ba7d36e1d7afa07
a9d8b91b6cd7810a4798c83e94f5543ded8ca39f
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEIP' 'sip-files00137.txt'
1151db2f3bb9a64c0f4405b25811af7c
8236c16b1496e4282bf81caf8fe0c06c2db888b8
describe
Invalid character
Invalid character
'4527' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIQ' 'sip-files00137thm.jpg'
f2008e51411a9766a903b2428022b614
4bdaf4cfa1d27d28c65db2beaa49e0a0481743fc
describe
'1052518' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIR' 'sip-files00138.jp2'
b36e661a1250e07b30b1144328806a19
9f122320e47ed4b9dd6569612d6280323e963ec9
describe
'39260' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIS' 'sip-files00138.jpg'
c7623540c6eb7d07c17c69a21e18dc80
4e9b154c0c4f1ff20371b5a281f261454487a510
describe
'16388' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIT' 'sip-files00138.pro'
254b047f7fc6934ac65ee9748e2b91ef
a8b4058701fad275ca77a41bdb9c3295087ab1b3
describe
'10861' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIU' 'sip-files00138.QC.jpg'
dca2df283c7290eb61b75f1067e24f12
db97b565ee409f511ad3e9d09da8faf7c5d21c18
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEIV' 'sip-files00138.tif'
0a139bb7c7e18be3a7b2d3989221ce2e
7b25dad610109b623e4891722cbb641d734a51ad
'2017-08-14T14:33:46-04:00'
describe
'845' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIW' 'sip-files00138.txt'
d9bdd9293c25f86fc3656ff903a456c5
2a3be309833ed2311950d59156b79c6be3dc3ee7
describe
'3149' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIX' 'sip-files00138thm.jpg'
d402c848f868a08a0f5b05b4234bbb84
629af97be6182f9dbfc2bd052de13be239304721
describe
'981713' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIY' 'sip-filesCopyright.jp2'
40df5108d3a701f13574165de6ffc576
9bd788444c9f34dc136d9fd450305a887b8b7f99
describe
'68370' 'info:fdaE20081130_AAAAACfileF20081130_AAAEIZ' 'sip-filesCopyright.jpg'
c784a904ef6f0083f498ecd3d6845e59
c739454a5ad9aeeab6d5dc610f22274d162abfbb
describe
'44622' 'info:fdaE20081130_AAAAACfileF20081130_AAAEJA' 'sip-filesCopyright.pro'
0524770e7b0753ae16e6170dad284f2b
793d4df3a4d60e0f09eb97a071301aa21a7a3ef0
describe
'19561' 'info:fdaE20081130_AAAAACfileF20081130_AAAEJB' 'sip-filesCopyright.QC.jpg'
df68ff0b243177fb425796a1abb42225
976312a714620919f399edca840a0d723244d901
describe
'7870156' 'info:fdaE20081130_AAAAACfileF20081130_AAAEJC' 'sip-filesCopyright.tif'
355a96fd5e8f2a9c273a28e2c3acee95
105cf305fd344718d2c3e4e312d24b28a44cb21d
describe
'2080' 'info:fdaE20081130_AAAAACfileF20081130_AAAEJD' 'sip-filesCopyright.txt'
f1e59f58a9abe4dec4ffa9a0ab410160
e3b7f18b6f2bba74c59a4fbed16c86fa9bbd1a6b
describe
Invalid character
Invalid character
'4893' 'info:fdaE20081130_AAAAACfileF20081130_AAAEJE' 'sip-filesCopyrightthm.jpg'
a83241dbcaeacd45e3237b27cbb1abcd
c727bea0b368748ae93149e727a9b96a8176f16a
describe
'47378' 'info:fdaE20081130_AAAAACfileF20081130_AAAEJF' 'sip-filesCopyright_Archive.pro'
386faac9a5449e337c13d55de48af638
84f8838917fb30e34032d05b817bd7343cc80e5a
describe
'8467580' 'info:fdaE20081130_AAAAACfileF20081130_AAAEJG' 'sip-filesCopyright_Archive.tif'
8229beec991fe3bbba025d2f026c630f
546799101ec30f42c1c26082f64b34fd0108a021
describe
'info:fdaE20081130_AAAAACfileF20081130_AAAEJH' 'sip-filesCopyright_Archive.txt'
71c32892fc06730b3de4481451e68b41
fcd6a17a43f16bd0e8d04b7f47662808f101b771
describe
Invalid character
Invalid character
'233683' 'info:fdaE20081130_AAAAACfileF20081130_AAAEJI' 'sip-filesUF00082179_00001.mets'
3947672034663d2d20e34c6a4162ab06
b700e0d82018abbf6525a77fda1c3b79f5e25248
describe
TargetNamespace.1: Expecting namespace 'http://www.uflib.ufl.edu/digital/metadata/ufdc2/', but the target namespace of the schema document is 'http://digital.uflib.ufl.edu/metadata/ufdc2/'.
'2017-08-14T14:35:36-04:00' 'mixed'
xml resolution
http://www.loc.gov/standards/xlink.xsd
BROKEN_LINK schema http://www.loc.gov/standards/xlink.xsd
TargetNamespace.1: Expecting namespace 'http://www.uflib.ufl.edu/digital/metadata/ufdc2/', but the target namespace of the schema document is 'http://digital.uflib.ufl.edu/metadata/ufdc2/'.
'301118' 'info:fdaE20081130_AAAAACfileF20081130_AAAEJL' 'sip-filesUF00082179_00001.xml'
cfd709f91f4c19b68097314fe7b791e9
b2595c7ebcf2baac1e0664093cc2a100b4ba084d
describe
'2017-08-14T14:35:37-04:00'
xml resolution
http://www.loc.gov/standards/xlink.xsd
http://www.loc.gov/standards/xlink.xsd



PAGE 1

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