Western Michigan University ScholarWorks at WMU
Master's Theses Graduate College
8-1974
An Investigation of Photographic Phase Holograms
Dale Lance Markham
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Recommended Citation Markham, Dale Lance, "An Investigation of Photographic Phase Holograms" (1974). Master's Theses. 2607. https://scholarworks.wmich.edu/masters_theses/2607
This Masters Thesis-Open Access is brought to you for free and open access by the Graduate College at ScholarWorks at WMU. It has been accepted for inclusion in Master's Theses by an authorized administrator of ScholarWorks at WMU. For more information, please contact [email protected]. AS INVESTIGATION OP PHOTOGRAPHIC PHASE HOLOGRAMS
by
Dale Lance Markham
A Thesis Submitted to the Faculty of The Graduate College in partial fulfillment of the Degree of Master of Arts
Western Michigan University Kalamazoo, Michigan August, 1974
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. ACKNOWLEDGEMENTS
Gratitude is expressed to ray Thesis Committee Members
Professors Nathan L. Nichols and John E. Herman for their
constructive criticisms which benefited in the writing of
this thesis. Particular thanks goes to my Major Thesis
Advisor Professor Stanley K. Derby for his time, patience,
and guidance given to me during the many months of this
investigation.
Dale Lance Markham
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Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. M-6326 MASTERS THESIS MARKHAM, Dale Lance AN INVESTIGATION OF PHOTOGRAPHIC PHASE HOLOGRAMS. Western Michigan University, M.A., 1974 Physics, optics
Xerox University Microfilms ,Ann Arbor, Michigan 48106
THIS DISSERTATION HAS BEEN MICROFILMED EXACTLY AS RECEIVED.
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. TABLE OP CONTENTS
CHAPTER PAGE I THE PROBLEM AND ITS BACKGROUND...... q
II HOLOGRAPHY...... 3
III PROPERTIES OP PHASE HOLOGRAMS ...... n
IV EXPERIMENTAL ARRANGEMENT...... 17
Hologram Camera ...... q7
Transparency measurements ...... qa
V STUDIES IN BLEACHING PROCESSES ...... 22
Techniques for Producing Photographic Phase Holograms .... 22
The Modified Stanford Process ...... 24-
The Kodak Reversal Bleach System . . . 34
The Modified Developer Process .... 4 4
The Modified Reversal Bleach Process . 53
The Agfa P r o c e s s ...... 59
VI ATTEMPTS TO IMPROVE HOLOGRAPHIC IMAGES . . 66
Printout Resulting from Variable Light Intensities...... 55 Printout Resulting from Wavelength Variation of L i g h t ...... gg
Printout Resulting from Ultrasonic Agitation...... 7q
Ultrasonic Agitation Effect upon Wavelength Sensitivity ...... 72
Effects of Toners on Brightness and R e s o l u t i o n ...... 75
Liquid Gates and Holographic Resolution 76
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. TABLE OP CONTENTS (Cont.)
CHAPTEN PAGE
VII SELECTING AN OPTIMUM HOLOGRAPHIC PROCESS . 78
CONCLUSIONS ...... g5
APPENDICES
I PROCESSING STEPS POE THE MODIFIED STANFORD P R O C E S S ...... S8
II PROCESSING STEPS FOR THE KODAK REVERSAL BLEACH SYSTEM ...... 99
III PROCESSING STEPS FOR THE MODIFIED DEVELOPER PROCESS ...... 100
IV PROCESSING STEPS FOR THE MODIFIED REVERSAL BLEACH PROCESS .... 101
V PROCESSING STEPS FOR THE AGFA PROCESS . . 102
VI PROCESSING STEPS FOR THE DERBY PROCESS . . 103
VII PROCESSING STEPS FOR THE MARKHAM PROCESS . 104
VIII INFORMATION ABOUT UNUSUAL CHEMICALS USED IN THIS PAPER ...... 105
FOOTNOTES ...... 108
BIBLIOGRAPHY...... H A
iv
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. LIST 0? TABLES
TABLE PAGE
1. Categorization of the Five Processes Investigated in this P a p e r ...... 26
2. The Essential Processing Steps of The Modified Stanford Process ...... 28
3» Pinal Absolute and Normalized Transparencies of Holograms Processed with The Modified Stanford Process and Processed with the Pour Modifications Performed on The Modified Stanford Process ...... 29
4. The Essential Processing Steps of The Kodak Reversal Bleach S y s t e m ...... 35
5. Pinal Absolute and Normalized Transparencies of Holograms Processed with The Kodak Reversal Bleach System and Processed with the Five Modifications Performed on The Kodak Reversal Bleach System ...... 4-3
6 . The Essential Processing Steps of The Modified Developer Process ...... 48
7. Pinal Absolute and Normalized Transparencies of Holograms Processed with The Modified Developer Process and Processed with the Three Modifications Performed on The Modified Developer P r o c e s s ...... 52
8 . The Essential Processing Steps of The Modified Reversal Bleach Process . . . 54
9. Final Absolute and Normalized Transparencies of Holograms Processed with The Modified Reversal Bleach Process and Processed with the Three Modifications Performed on The Modified Reversal Bleach Process . . . 55
10. The Essential Processing Steps of The Agfa P r o c e s s ...... 60
11. Pinal Absolute and Normalized Transparencies of Holograms Processed with The Agfa Process and Processed with the Pour Modifications Performed on The Agfa Process 61
v
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. LIST OP TABLES (Cont.)
TABLE p a g e
12. Summary of The Western Michigan University Modifications ...... 80
13. Final Absolute and Normalized Transparencies of Holograms Processed with The Twelve Western Michigan University Modifications 87
14. The Essential Processing Steps of The Derby P r o c e s s...... 91
15. The Essential Processing Steps of The Markham P r o c e s s ...... 92
vi
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. LIST OF FIGURES
FIGURE P£G£
1. The Sand Box Unit ...... IS
2. Arrangement of Components in The Sand Box U n i t ...... 18
3. Arrangement of Transparency Measurement Zones on each H o l o g r a m...... is
4. Schematic of the Emulsion Cross Section for a Direct Bleach Process, a Negative Phase Image Process, and a Reversal Bleach Process ...... 25
5. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Modified Stanford Process (MSP) and processed without the prehardener in The Modified Stanford Process ...... 30
6. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Modified Stanford Process (MSP) and processed with D-76 substituted as the developer in The Modified Stanford Process 31
7. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Modified Stanford Process (MSP) and processed with potassium dichromate sub stituted as the bleaching agent in The Modified Stanford Process ...... 32
8. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Modified Stanford Process (MSP) and processed without the clearer in The Modified Stanford P r o c e s s ...... 33
9. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Kodak Reversal Bleach System (KRBS) and processed with D-19 substituted as the developer in The Kodak Reversal Bleach S y s t e m ...... 38
vii
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. LIST OF FIGURES (Gont.)
FIGURE PAGE 10. Time Variation of Absolute and normalized Transparency of Holograms processed with The Kodak Reversal Bleach System (KRB3) substituting D-19 and D-76 as developers 39
11. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Kodak Reversal Bleach System (KRBS) substituting D-19 as the developer and substituting D-19 as the developer along with removal of the stain remover . • . 40
12. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Kodak Reversal Bleach System (KRBS) substituting D-19 as the developer and substituting D-19 as the developer along with removal of the clearer ...... 41
13. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Kodak Reversal Bleach System (KRBS) substituting D-19 as the developer and: 1) processed without the stain remover, 2) processed without the clearer, 3) processed without either the stain remover or the clearer ...... 42
14. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Modified Developer Process (MDP) and processed with D-19 substituted as the developer in The Modified Developer Process 49
15. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Modified Developer Process (MDP) substituting D-19 and D-76 as developers . 50 16. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Modified Developer Process (MDP) substituting D-19 as the developer and substituting D-19 as the developer along with omission of potassium iodide from the bleach bath ...... 51
viii
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. LIST OF FIGURES (Cont.)
FIGURE PAGE
17. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Modified Reversal Bleach Process (MRBP) and processed with D-76 substituted as the developer in The Modified Reversal Bleach P r o c e s s ...... 55
18. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Modified Reversal Bleach Process (MRBP) and processed with Sodium Bisulfite as the clearer in The Modified Reversal Bleach P r o c e s s ...... 57
19. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Modified Reversal Bleach Process (MRBP) and processed without the clearer in The Modified Reversal Bleach Process . . . 58
20. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Agfa. Process (AP) and processed.with D-76 substituted as the developer in The Agfa Process ...... 62
21. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Agfa Process (AP) and processed without the clearer in The Agfa Pr o c e s s ...... 63
22. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Agfa Process (AP), processed without phenosafranine in the desensitizer of The Agfa Process, and processed without the desensitizer in The Agfa Process . . . 64-
23. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Modified Developer Process arranged at various distances from a printout inducing light source ...... 67
ix
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. LI S3? OP FIGURES (Cont.)
FIGURE PAGE
24. Tine Variation of Absolute and Normalized Transparency of Holograms processed with The Modified Reversal Bleach Process arranged at various distances from a printout inducing light source ...... 68
25. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Modified Reversal Bleach Process arranged with different filters placed in front of a printout inducing light . . 70
26. Time Variation of Absolute and Normalized Transparency of Holograms processed with different modifications after agitation of the unexposed film in an ultrasonic c l e a n e r ...... 73
27. Wavelength Variation of the Darknesses of Spectral Lines on a Kodak S.A.-3 Spectro- graphic Plate Agitated in an Ultrasonic Cleaner before Exposure divided by the Darknesses of Spectral Lines on an Unagitated S.A.-3 Plate ...... 75
28. Time Variation of Absolute and Normalized Transparency of Holograms processed with Western Michigan University Modifications One and T w o ...... 29. Time Variation of Absolute and Normalized Transparency of Holograms processed with Western Michigan University Modifications Two and Three ...... q 2
30. Time Variation of Absolute and Normalized Transparency of Holograms processed with Western Michigan University Modifications Three and P o u r ...... 83
31. Time Variation of Absolute and Normalized Transparency of Holograms processed with Western Michigan University Modifications Five, Six, and S e v e n ...... 84
x
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. W'
LIST OP PIGUBES (Cont.)
PIGUBE PAGE
32. Time Variation of Absolute and Normalized Transparency of Holograms processed with Western Michigan University Modifications Six, Seven, and E i g h t ...... 85 33. Time Variation of Absolute and Normalized Transparency of Holograms processed with Western Michigan University Modifications Nine, Ten, Eleven, and Twelve ...... 86
34-. Time Variation of Absolute and Normalized Transparency of Holograms processed with Western Michigan University Modifications 4A, 12A, and 12B ...... 90
33. Time Variation versus Absolute Transparency for a Typical Bleached Hologram ...... 96
xi
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. CHAPTER I
THE PROBLEM AND ITS BACKGROUND
Since the theory and research on holography was first 1 2 accomplished by Gabor , it was left to Leith and Upatnieks
to show that the idea of holography was more than just an
optical curiosity. The first holograms were recorded on
ultra fine grained photographic emulsions, processed with
just a development and a fixing stage. Cathey showed that
holograms could also be bleached resulting in an increased
brightness of the holographic image. Because a brightness
ratio of almost a factor of ten exists between bleached
and unbleached holograms, study proceeded in the direction
of developing better methods of producing bleached holo
grams. Other means of producing holograms such as recording
the hologram in dichromated gelatin or photoplastics have
been developed but because photographic emulsions are at
least 100 times faster than other materials and are sen
sitive to all wavelengths of visible light, most ventures
were turned towards photographic holography.
Along with the increase of brightness there are two
problems which must be solved before high quality bleached
holograms can be produced. The first problem concerns
the fact that a photographic emulsion, when bleached,
produces an excessive, amount of scattered light which
degrades the holographic image. A second problem concerns 1
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. the fact that the final "bleached product is generally left
in the form of a silver halide, which exhibits printout
darkening as a function of time. As the silver halide
reduces hack into metallic silver, the hologram darkens
and the holographic information is lost. The resultant
increase in darkening of the emulsion is known as the
printout effect.
It is the purpose of this investigation to attempt
to produce bleached holograms which have good resolution
and high resistance to printout darkening.
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. CHAPTER II
HOLOGRAPHY
Holography is a radically different concept in photo
graphic optics. The process, which can he called photog
raphy hy wavefront reconstruction, records the reflected
light waves from an object and not the image of the object,
being photographed, as with the normal photographic process
The photographic record, called a hologram, bears no
resemblance to the original object but contains in an
optical code all the information about the object that
would be contained in an ordinary photograph and much
additional information unrecordable by any other photo
graphic process. The hologram looks like a hodgepodge of
specks, blobs, and whorls upon the developed photographic
plate or film. The creation of an intelligible image from
the hologram is known as the reconstruction process, where
the waves optically recorded on the emulsion surface pro
ceed onward reconstructing an image of the original subject
oblivious to the time lapse in their history. These waves
are indistinguishable from the original waves and are
capable of all the phenomena that characterize the original
waves.
As in ordinary photography, the object is illuminated
and a photographic emulsion positioned to receive reflected
light from the object. However, no lens or other image 3
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. forming device is used in creating a hologram. Each point
on the emulsion receives light from the entire object;
conversely, each point on the object reflects light to
the entire photographic emulsion. The illuminating light
must be monochromatic and coherent, also different from
ordinary photography. Lastly, a mirror is used to direct
a portion of the coherent light directly to the plate,
bypassing the object. This beam is called the reference
beam, and it is the interference effect between it and
the reflected object light which creates the hologram.
The problem of wavefront reconstruction is to record
the exact form of the wave pattern reflected from an ex
tended and irregular object. To capture the wave pattern
completely both the amplitude and the phase of the waves
must be recorded at each point on the emulsion surface.
Ordinary photographic emulsions record wave amplitudes by
conversion of the amplitudes to corresponding variations
in the opacity of the emulsion. The emulsion, however,
is completely insensitive to phase relations. The technique
of interferometry is used in holography to preserve these
phase relations. It can be shown that relative phase infor
mation can be preserved in two-beam interference patterns.
The basic technique of hologram formation then is to divide
the coherent light coming from a laser into two beams; one
to illuminate the subject and one to act as a reference
beam. The reference beam usually has a spherical or planar
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. wavefront. The reference "beam is directed to intersect
the light reflected from the subject. Since these two
beams are coherent, an interference pattern will form in
the volume of space where the beams overlap. A photo
graphic emulsion placed in the overlap region thus records
the amplitude and phase relations from the reflected light
originating from the subject. After suitable processing
of the emulsion, the medium becomes the hologram.
The intensity of the interference pattern can be
regarded as a three-dimensional contour map. If the
photographic emulsion in the overlap region is very thin,
it will record line traces of the maximum intensity contour
surfaces. Such holograms are called plane holograms and
these holograms have properties similar to those of plane
diffraction gratings. If the photographic emulsion is
relatively thick, the contour surfaces themselves are
recorded. Such holograms are called volume holograms and
these take on properties of volume diffraction gratings.
A hologram made in the manner just described has many of
the properties of a grating made by a ruling engine; how
ever, such a grating has precise uniformity whereas a
hologram has complete nonuniformity. The inadvertently
produced irregularities in an imperfectly ruled grating
produces false spectral lines called ghosts, while the
deliberately induced irregularities in a hologram give
rise in the reconstruction process to a complete well
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. defined image.
The lines of developed silver on plane holograms and
the surfaces of developed silver on volume holograms are
very closely spaced and therefore diffract light signif
icantly. When the hologram is illuminated by the original
reference beam, part of the light diffracted out of the
reference beam is directed and shaped by the hologram into
a re-creation of the light wavefronts originally coming
from the subject. A reconstructed wave train proceeds
out from the hologram exactly as did the original subject
wave. An observer viewing a wave identical with the orig
inal subject wave perceives it to diverge from a virtual
image of the subject located precisely at the original
subject position. If the reference beam is accurately
positioned so that all rays of the reflected beam are
opposite to the original reference beam, then a real image
of the subject at the original subject location is produced.
Because the light converges to the image it can be directly
detected with a photographic emulsion without need for a
lens. In summary, a hologram acts as a combination rec
ording and projection system which provides an image of
the original subject when illuminated by the reference and
does so without the need for additional lenses.
Holograms and the images they produce have many cu
rious and fascinating properties. The pertinent infor
mation recorded on the hologram can be seen only under
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 7 magnification and consists of highly irregular fringes
which hear no apparent relation to the subject. A hologram
can he broken into small fragments and each fragment will
produce a complete image. However, as the pieces get
smaller, the image resolution is lost. The hologram is
itself a positive, not a negative. Normally one would
consider a hologram as a negative, but the image it pro
duces is a positive. The photographic emulsion containing
the hologram registers only two levels of density; trans
parent and opaque. However, the tonal qualities of the
image do not suffer. Several images can be superimposed
on a single emulsion with successive exposures, and each
image can be recovered without being affected by the other
images. The virtual image is seen by looking through the
hologram as if it were a window-. The image appears in
complete three-dimensional form. As the observer changes
his viewing position the perspective of the picture changes,
just as if the observer were viewing the original scene.
Parallax effects are evident between near and far objects.
If an object in the foreground lies in front of something
else, the observer can move his head and look around the
obstructing object to see the previously hidden object.
One must refocus his eyes when the observation is changed
from a near to a far object. In short, there are no visual
tests one can make to differentiate the image from the
real object. The real image will hang in space between
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. the observer and the hologram also having all of the above
mentioned features; however, this real image is much more
difficult to view.
The light used to illuminate the object must be both
coherent and monochromatic. If the spectrum of the light
was broad, each wavelength component would produce its own
separate pattern and the resultant of all these components
would average out the fringes and produce a smooth dis
tribution. Thus the requirement for a monochromatic source.
If the source is non-coherent, then each source element
produces interference fringes displaced from those of other
elements; thus, the sum of many such sets of fringes aver
ages to some very nearly uniform value, thus losing the
desired fringe pattern.
Holography was intended as a tool for electron micros
copy. It occurred to Gabor in 194S that the aberrated
image produced by an electron lens still preserves all of
the subject information but in a somewhat coded form. If
the aberrated image could somehow be decoded, the reso
lution limit of the electron microscope perhaps could be
increased by a factor of ten. Gabor dispensed with the
microscope altogether and performed a decoding operation
on a photographic record of unfocused electron waves
diffracted from the subject. He theorized that this wave
record could be decoded by illuminating it with coherent
visible light; thus, waves arising out of the diffraction
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. yield the optical equivalent of the unfocused electron
waves* These waves should yield a highly magnified optical
image, the magnification being given by the ratio of the
light wavelength to that of the electron wavelength. The
light beam must be an accurately scaled imitation of the
electron waves. Gabor formed the first hologram with
visible light to test his theory. At that time, and even
now, it is not possible to obtain the required beam coher
ence in an electron wave and difficulties also exist in
high resolution recording at very short wavelengths.
Before the invention of the laser, the concept de
rived by Gabor seemed to be doomed to a class of optical
curiosities. Due to the many obstacles, little progress
was made and the concept abandoned for nearly a decade.
However, in the early 1960's Leith and TJpatnieks^ bright
ened prospects in holography, by employing the newly
developed laser which provided a very intense, monochro
matic, coherent light source. By 1964 they had convincing
proof that holography was indeed practical. This was a
long step from Gabor's idea of wavefront reconstruction.
Several imaginative applications seem to rest in the
balance if holography can be improved. One specific appli
cation seems to lie in the areas of electron or x-ray
holography as first proposed by Gabor. Holograms recorded
in these electromagnetic frequencies may theoretically be
reconstructed in visible light. The most sensational
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 10
future application of holography undoubtedly lies in the
field of producing three-dimensional television and motion
pictures; however, technical problems must be surmounted
before these forms of entertainment become a reality.
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. CHAPTER III
PROPERTIES OP PHASE HOLOGRAMS
In optical holography a photographic emulsion is used
to record the sum of the wavefronts from the object and
from a reference beam, the reference beam making possible
the recording of both the amplitude and the phase of the
object wavefront. The amplitude of the object wavefront
is represented by the intensity of a fringe pattern re
corded by the density of developed silver sites while the
phase of the object wavefront produces variations in the
position of the fringes. The resulting holographic image
is due in part to the different amplitudes of metallic
silver developed on the photographic emulsion. Such a
hologram is sometimes called an amplitude hologram, since
in reconstruction of the image, the photographic emulsion
spatially amplitude modulates the wavefront of the illumi
nating beam in a way to reconstruct the original wavefront
from the object.
Analogous to a modulated carrier in electrical commu- 5 nications, Cathey first developed the idea that spatial
phase modulation could replace spatial amplitude modulation
in reconstruction of the holographic image. If an amplitude
hologram is bleached, so as to convert the metallic silver
to a transparent compound whose index of refraction differs
from that of the gelatin, then the holographic record is 11
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 12 written in the resulting localized changes in the index
of refraction of the emulsion. Such a hologram is some
times called a phase hologram, because the holographic
information is now due to a spatially phase modulated
wavefront•
Since Cathey^ first bleached a photographic plate
and showed that phase holograms add more flexibility to
the wavefront reconstruction process, other methods of
producing pure phase holograms have been developed.
Materials other than bleached photographic emulsions for
producing phase holograms include: dichromated gelatin^”11)
photopolymer thick thermoplastics^^*1^ , photo
resist (-*-9-24), iron o x i d e ^ * 2^ , photoplastics^2^-2^ .
Two terms are useful in describing properties of
holograms: these are diffraction efficiency and signal to
noise ratio. These terms may be applied equally well to
either amplitude or phase holograms. The brightness of
a holographic image can be described by the term diffrac
tion efficiency which is defined as the amount of light
diffracted by the hologram into making the holographic
image, divided by the incident light upon the hologram.
Diffraction efficiency is usually expressed as a percentage.
The resolution of a holographic image can be described by
the term signal to noise ratio, which is defined as the
ratio of the intensity of the diffracted light originating
from the object as compared to the intensity of the scat—
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 13 tered light originating from the background.
Holograms suitably processed in dichromated gelatin^
have diffraction efficiencies of as high as 90% and signal
to noise ratios of 230 to 1. These holograms have good
environmental stability but their spectral sensitivity
is limited to the short wavelengths. Holograms suitably
processed in photopolymer materials^ have diffraction
efficiencies of as high as 80% and signal to noise ratios
of 200 to 1 but the environmental stability of photopolymer
materials must be improved. Holograms suitably processed 32 in thick thermoplastics have diffraction efficiencies of
25% and signal to noise ratios of 70 to 1 but the material
distorts at high temperature and humidity and is not very
sensitive at long wavelengths. Holograms suitably processed
in photoresist materials^ have diffraction efficiencies
of 80% and signal to noise ratios of 250 to 1 but humidity
causes fine cracks to form in the photoresist material. 34- Holograms suitably processed in iron oxide materials have
excellent stability against all environmental parameters
but the maximum diffraction efficiencies are 20% and signal
to noise ratios 15 to 1. Holograms suitably processed in
photoplastics^ have good environmental stability and
sensitivity at long wavelengths but diffraction efficiencies
of only 10% and signal to noise ratios of 45 to 1 have been
reported. Burckhardt^ has shown that theoretically it is
possible to produce bleached photographic holograms with
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 14
1 0 0 % diffraction efficiency, whereas the maximum possible
diffraction efficiency of unbleached photographic holograms
is about 4%. Latta^, and Upatnieks and Leonard^ 8 have
produced bleached photographic holograms with diffraction
efficiencies of about 60%.
Because of their high sensitivity to light, especially
at long wavelengths, photographic emulsions are still
preferred for recording holograms. When a photographic
emulsion is developed, fixed, and then bleached, the plate
or film is rendered almost transparent. Because of reduced
attenuation of light, spatial phase modulation methods are
capable of producing a brighter image than spatial ampli
tude modulations.
The phase modifications to the incident beam can be
caused by an index of refraction variation in the emulsion
or by relief images on the emulsion surface. Variation of
the index of refraction is proportional to the mass of
silver originally exposed, thus the more silver sites
originally exposed and converted to a transparent material,
the greater the change in the index of refraction. Since
the mass of silver is proportional to the silver density,
holograms which demonstrate high diffraction efficiencies
when bleached have high original densities. Variation in
the relief image height is also proportional to the orig
inal silver density as well as dependent on the tanning
action produced on the gelatin by the developer and the
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 15 ■bleach. Tanning is the result of a higher than normal
degree of cross linking of the gelatin molecules due to
chemical treatment of the emulsion. Tanning causes the
gelatin layer to become insoluble in water. Upon drying,
that area of the gelatin receiving a greater degree of
tanning becomes thicker than the less tanned area because
the amount of water absorption, and hence the volume
expansion, decreases with increased tanning.
Unfortunately, while bleached photographic holograms
have high diffraction efficiencies, the improved efficiency
is accompanied by an increase in scattered light reducing
the image resolution. Also, the materials remaining in
the emulsion are very prone to convert back into metallic
silver (printout effect), rendering the hologram darker
and the holographic image of lesser quality. Several
reasons have been proposed for the poor resolution quality
of a bleached holographic image: local changes in emulsion
thickness on development due to release of stress intro
duced by factory drying, tanning of the emulsion by the
developer and bleach, stress formation during the drying
of the emulsion, silver being extruded from geometrically
regular positions to filamentary tangles in developing,
scattering by the large silver halide grains, optical
irregularities or phase errors within the volume of the
emulsion, localized lateral distortions that vary according
to the grain pattern of the signal beam.
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 16
All of the above factors are contributors to the
scattering of light in bleached holograms which is clas
sified as optical noise. Methods of controlling the
printout effect as well as lowering the optical noise
in photographic phase holograms must be found before an
optimum process can be reported.
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. CHAPTER IV
EXPERIMENTAL ARRANGEMENT
Hologram Camera
The holograms were exposed in a hologram camera known
as a "sand "box unit". The unit is so named because the
laser and the lenses and mirrors which diverge and reflect
the laser beams are simply placed into a box full of sand.
The box is a table turned upside down which has a retaining
wall of six inch depth which is filled with sand. The box
is placed upon a truck tire inner tube which is not fully
inflated. The tube in turn lies on another table which
isolates the system from the floor and walls. The tube
is not fully inflated to better act as a vibration damper.
The box is isolated from the floor and walls to prevent
vibrations from entering the system. The laser, lenses,
and mirrors are placed in the sand as a further precaution
against vibration (figure 1 ).
The components of the hologram camera were arranged
as in figure 2. The laser was a Bausch and Lomb He-Ne
Gas L aser^ which produced a beam of 0.6 milliwatts full
intensity at 6328 angstroms. A black box was positioned
over the laser with only a hole to let the beam out in
order to cut out the background glare produced by the laser.
The reference beam to stage illumination ratio was 1.5 to
1, and the angle between these beams was 60 degrees. The 17
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. Components
/1 \ Inverted ‘ Table Sand'
Retaining Wall 2^ Inner Tube — T 7 \ -Table
Figure 1. The Sand Box Unit
Plane ^ \ ^ Plane Mirror Mirror Microscope Lenses \L
Beam Splitter
Film ^Platform
Figure 2. Arrangement of Components in The Sand Box Unit
One-Eighth Hologram Inch Circles
Figure 3. Arrangement of Transparency Measurement Zones on each Hologram
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 19
stage consisted of a series of spikes for estimating
signal to noise ratio of the holographic image as well
as the backside of a Kennedy half dollar for determining
the resolution properties of the image.
The hologram box was placed in a photographic darkroom
where no light or air currents could enter. To expose a
hologram a black piece of cardboard was placed in front
of the laser beam, the unexposed film was positioned by
means of clips onto the film platform, the system was
allowed to rest for thirty seconds so that vibrations
were damped out, then the cardboard was carefully raised
to allow the beam to enter the system. After the proper
exposure time the cardboard was lowered blocking off the
beam and ending the exposure. The hologram was then proc
essed immediately in a separate darkroom.
Transparency Measurements
The method of determining the transparency of holo
grams was straightforward and simple. After the hologram
was processed, five circles one-eighth inch in diameter
were drawn on the non-gelatin side of the hologram (fig
ure 3). Each small circle of the hologram was then 40 oriented in turn in a Bausch and Lomb Microphotometer
and the transparency of the small circular area was
measured. The working value for each hologram transpar
ency was taken as the average of the five values recorded
for the five circular areas. The holograms were then
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 20 placed on a light box of diffused fluorescent light
(intensity 145 foot-candles) for twenty-four hours a day.
Any evidence of printout darkening could be detected if
after a given period of time a further check of the
holographic transparency showed changes, the assumption
being that the changing transparency of the hologram is
directly related to the phenomenon of printout darkening.
Duplicate holograms were generated for each modi
fication of the various parameters of developing, bleaching,
clearing, and desensitization. Each duplicate hologram
pair resulted in printout versus time curves that were
very similar. Because of this similarity, the duplicate
measurements for each pair were averaged and plotted as
a single curve.
The absolute percentage of transmitted light was
plotted as a function of time to determine the transparency
variation of each modification. The higher the transpar
ency of the modification, the more likely it is for the
hologram to have a high diffraction efficiency. The
normalized percentage of transmitted light was plotted to
determine the printout variation of each modification as
a function of time. The lower the printout resistance
of the modification, the more likely it is for the holo
graphic image to suffer a degradation. The absolute
percentage of transmitted light is read directly from the
microphotometer. The normalized percentage of transmitted
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 21
light is found by dividing the holographic transparency
as a function of time by the initial holographic trans
parency .
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. CHAPTER Y
STUDIES IN BLEACHING PROCESSES
Techniques for Producing Photographic Phase Holograms
A search was made in the literature for ways of
producing high quality photographic phase holograms. It
was found that several groups had evolved their own
particular means of processing. Of these processes, each
can be placed into one of three categories for production
of photographic phase holograms. These categories are:
1 ) direct bleaching process, 2 ) negative phase image
process, 3 ) reversal bleaching process.
In a typical direct bleaching process the emulsion
is developed and fixed, then bleached in a solution that
converts the metallic silver into a transparent, insoluble
salt having a refractive index significantly higher than
that of the gelatin. When the emulsion dries, a relief
image is formed where the developer converts the silver
halide into metallic silver. The tanning tends to be
fairly localized within the emulsion and as a result the
emulsion pulls together. Por a direct bleaching process
the variations of optical path length from the relief image
and those from index variations within the emulsion are
additive, consequently excessive optical noise is produced
upon the reconstructed image. 22
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 23 In a typical negative phase image process, the exposed
emulsion is developed but not fixed so that silver halide
remains in the unexposed regions. The emulsion is then
bleached in a suitable bleach bath which converts the
metallic silver to a soluble salt and removes it from the
emulsion. Because the remaining silver halide appears as
a negative for a direct process, this is referred to as a
negative phase image process. In a direct bleach process
the formed relief image enhances scattered light. However,
the negative phase image process keeps the relief image
path length variation of light to a minimum. This dras
tically reduces the optical noise in the holographic image.
Maximum tanning occurs in regions of maximum development
and thus there is a tendency for a relief image to be
formed at the position of the silver sites. However, the
bulk of the silver halide tends to counteract this effect
and for commonly used developers this bulking seems to be
the stronger effect.
In a typical reversal bleach process the exposure
and development of the hologram are carried out to form
a normal silver image. The hologram is then re-exposed
to a uniform source of white light making developable the
silver halide grains not protected by the previously
formed silver image. The hologram is bleached after the
second development, thus the metallic silver formed in
either development is removed leaving a phase image formed
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. only from the residual silver halide. If the second
exposure is controlled, almost the entire "background of
silver halide grains can be eliminated leaving a phase
image consisting of the silver halide grains shielded by
the silver formed from the first exposure. It is intu
itively obvious that reduction of this background would
reduce the scattered light inherent in a bleached holo
graphic image. Figure 4 shows schematically the three
previously described processes.
Of the processes described in the literature five
were selected for investigation in this paper because of
the claims that each processed holograms of high diffrac
tion efficiencies, high signal to noise ratios, and high
resistance to printout. These processes were: 1) The hi Modified Stanford Process , 2) The Kodak Reversal Bleach
System^2, 3) The Modified Developer Process^, 4) The 44 \ 45 Modified Reversal Bleach Process , 5) The Agfa Process •
The following experimental work is directed towards exam
ining each process in detail and combining the good fea
tures of these five methods into an optimum process for
creating photographic phase holograms. Table I categorizes
each process investigated in this paper.
The Modified Stanford Process
The Modified Stanford Process is a result of modifi
cations on The Stanford Process. The Stanford Process was
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission.
VJ1
remove Ag light uniformwhite 5) 5) Bleach to 3) 3) Re-expose with 2) 2) Develop 4) 4) Redevelop 1) 1) Expose
AgBr yigBr I I Base I Ag
AgBr AgB
remove Ag represent emulsion movement) 2) 2) Develop 3) No Fix 1) 1) Expose 5) 5) Dry (Arrows 4) 4) Bleach to I- Baae I I- LBase I c w i AgBr-^ AgBr AgBr
to a silver convert Ag emulsion represent halide movement) a Negative Phase Image Prooess, and a Reversal Bleach Process 1) 1) Expose 2) 2) Develop 3) 3) Fix 5) 5) Dry (Arrows 4) 4) Bleach to _ Baas I Figure 4. Schematic of the Emulsion Cross Section for a Direct Bleach Process, I BaseI I L,., Direct Bleach Process Negative Phase Image Process Reversal Bleach Process ;— :Br— V Ag^CDD AgBr Ag- Ag- AgBr' Silver Silver Halide Halide
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 26 Table I
Categorization of the Five Processes Investigated in this Paper
Modified Stanford - Direct Bleach Process
Kodak Reversal Bleach - Negative Phase Image Process
Modified Developer - Negative Phase Image Process
Modified Reversal Bleach - Reversal Bleach Process
Agfa - Negative Phase Image Process
46 developed by Lehmann, Lauer, and Goodman at Stanford
University. To negate the effects of the relief image
formation in a direct bleaching process they introduced a
prehardening step immediately after exposure and before 47 development. Lehmann, Lauer, and Goodman report that
the speed of Agfa films decreases in proportion to the
prehardening time. However, as the prehardening time
increases the diffraction efficiency and signal to noise 48 ratio both decrease. Upatnieks and Leonard report that
Kodak Prehardener SH—5 reduces the relief pattern and
localized distortions on Kodak 649-F plates giving better
diffraction efficiency and signal to noise ratio. The
Stanford Process utilizes cupric bromide as a bleaching
agent. Lehmann, Lauer, and Goodman^ theorize that the
bleach first converts the metallic silver to silver bromide
leaving insoluble cuprous bromide in the emulsion. A
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 27
clearing bath consisting of a mixture of potassium perman
ganate and potassium bromide then converts the cuprous
bromide back into soluble cupric bromide and also removes
the sensitizing impurities from the emulsion leaving a
transparent silver bromide medium of refractive index 2 . 2 5
in the emulsion. In regard to printout behavior, Lehmann, 50 lauer, and Goodman only reported that holograms exposed
to rooms lighted by fluorescent lights, sunlight filtered
through Venetian blinds, and scanned by a He-Ne and Argon
lasers yielded after seventy days no appreciable evidence
of printout. Since the final emulsion product is silver
bromide, one would expect that a printout would occur
fairly rapidly as a function of time, as reported by 51 McMahon and Maloney .
The Stanford Process was modified by Colburn, Zech,
and Ralston^ 2 in two ways: 1) an amount of ferric chloride
equal to that of the cupric bromide was added to the bleach,
2 ) a two step drying process of 5 0 % methanol then 1 0 0 %
methanol was instituted to insure a more uniform and quicker
drying procedure as well as helping clear the emulsion
surface of sensitizing impurities. This modified process
they named The Modified Stanford Process. The essential
processing steps of The Modified Stanford Process are given
in Table II. Holograms processed by The Modified Stanford Process
gave brighter holographic images than with any other process
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. Table II
The Essential Processing Steps of The Modified Stanford Process
Step 1 ...... Preharden in Kodak SH-5
Step... 2 ...... Develop in Kodak D-19
Step 3 ...... Fix in Kodak fiapid Fixer
Step 4 ...... Bleach in Ferric Chloride and Cupric Bromide
Step 5 ...... Clear and Desensitize in Potassium Permanganate and Potassium Bromide
tried in this paper. However, image resolution was not
as good as with most of the processes, indicating much
scattering of light in the emulsion due either to the
"bleaching process or to the relief image formed by such
a direct bleaching process. No qualitative data were
taken on diffraction efficiency or signal to noise ratio.
The printout effect was studied in a much more qual
itative manner. The Modified Stanford Process was further
altered in this investigation by the omission or substi
tution of a certain processing step to better understand
how each step changes the printout resistance of the
emulsion. The first variation of The Modified Stanford
Process involved omission of the prehardening step. The
second change was the replacement of D-19 with D-76 as
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. the developer. The third change was the substitution of
potassium dichromate as the bleaching agent. Variation
number four was the omission of the clearing bath.
Figures 5-8 illustrate the transparency response of
the bleached emulsions to the alterations of The Modified
Stanford Process while Table III gives the final absolute
and normalized transparencies of these alterations.
Table III
Final Absolute and Normalized Transparencies of Holograms Processed with The Modified Stanford Process and Processed with the Four Modifications Performed on The Modified Stanford Process
Absolute Normalized Transparency Transparency
Modified Stanford Process 45% 1 1 0 %
Without Prehardener 52% 105%
Developed with D-76 52% 96%
Bleached with Potassium Dichromate 8 6 % 99%
Without Clearer 33% 89%
Figures 5-8 show that although printout is extreme
in all modifications within the first week, each modifi
cation recovered as time progressed. Although all proc
esses leveled off to a constant transparency after a ten
week period, some of the modifications have final trans
parencies above those of the initial readings. Processing
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 3 0
50 +» axi kDkO 45 ca-H •p^ n ©*o o © 40 Ft+> © 43 O Reference, (MSP) B © © 35 •P C Processed without 3 gj A H the prehardener Ofrt © 30 ,0«H ■< O 25 10 Time in Weeks
120
■Or) © a N © § 80
O S5 O
10 Time in Weeks
Figure 5. Time Variation-of Absolute and normalized Transparency of Holograms processed with The Modified Stanford Process (MSP) and processed without the prehardener in The Modified Stanford Process
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 55
O Reference, (MSP) A Developed with D-76
10 Time in Weeks
12CT
k T3 O © Ph -P +> TJ *h © S 63 © 8C
2 4 6 8 10 Time in Weeks
Figure 6. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Modified Stanford Process (MSP) and processed with D-76 substituted as the developer in The Modified Stanford Process
Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 32
80 O Reference, (MSP) A Bleached with potassium dichromate ® 'O o © h+» o) -p & -H s © ®
iH OH 40 10 Time in Weeks 110 £h xf © © p-t -p •O -H 8 0 ® e ea m Jh § 70 3$ a 64 S o 60 10 Time in Weeks Figure 7• Time Variation of Absolute and normalized Transparency of Holograms processed with The Modified Stanford Process (MSP) and processed with potassium dichromate sub stituted as the bleaching agent in The Modified Stanford Process Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 45 O Reference, (MSP) -p © X A Processed without ce-H 40 ■p-3 the clearer c © ■© o © ft -P 35 © -P P4 -H S © © ■P c 30 3 0} «—I F( o c-t m & 110 n © w-p djg 100 -p *0 C-rt © (-3 O 90 h T3 © © PU-P -P T3 -H 80 © S N © -H C r-t © OS Sh 70 S E-* o a o 60 50 1 _L JL 4 5 6 8 10 Time in Weeks Figure 8. Time Variation of Absolute and Formalized Transparency of Holograms processed with The Modified Stanford Process (MSP) and processed without the clearer in The Modified Stanford Process Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 34 without the prehardener yields a higher transparency than processing with the prehardener; however, probably with decreased diffraction efficiency and signal to noise ratio although no measurements were taken. Developing in D-76 yields holograms which are more transparent but more apt to printout than holograms developed in D-19. Holograms bleached with potassium dichromate are almost completely transparent; however, the holographic image is very faint indicating perhaps that potassium dichromate is not a suitable agent for holograms processed with a direct bleach process. Holograms processed without being cleared were very low in both transparency and printout resistance indicating that the potassium permanganate and potassium bromide in the clearer increase the holographic trans parency as well as desensitize the hologram to printout. The shape of the curves in Figures 5-8 would seem to indicate that the recovery rates of the curves are inde pendent of any change made in this investigation. Perhaps the sudden printout and gradual recovery is normal to a direct bleach process. Further investigations will be made in this paper to attempt to better understand the behavior of this transparency response. The Kodak Reversal Bleach System The. Kodak Reversal Bleach System which was developed by Lamberts and Kurtz*^ utilizes a special developer which produces sufficient tanning action to keep the relief image Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 35 path length variation to a minimum, which is the primary function of a negative phase image process. The essential processing steps of The Kodak Reversal Bleach System are given in Table IV. Table IV The Essential Processing Steps of the Kodak Reversal Bleach System Step 1 . , Step 2 . . Potassium Dichromate Step 3 . . Potassium Permanganate Step 4 . . Sodium Bisulfite The active constituent of Kodak Special Developer 5 h. SD-48 is pyrocatechol , which provides a strong tanning action with its high value of pH. The relief image is formed because of the strong local tanning action of the special developer on the gelatin in regions where devel opment to metallic silver takes place. This tanning action causes the gelatin to pull together when drying, increasing the thickness of the emulsion layer relative to other areas. The refractive index variation of the gelatin occurs because the developed silver is removed from the gelatin by the bleach which results in a higher Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. concentration of the original high index silver halide crystals in regions that received less exposure, and thus, an increase in the refractive index of the emulsion layer. Lamberts and Kurtz^ reported a diffraction effi ciency of 46% and a signal to noise ratio of 17 when the process was used on Kodak 649-? plates. No mention was made of possible printout darkening. Pyrocatechol is a hazardous material and when using the developer caution is needed. Rubber gloves seemed unsuitable since several gloves developed leaks after contact with the developer; however, plastic gloves worked very well. The developing stage of this process was very difficult to control. With the Agfa 10E70^^ film a devel opment time of two minutes was found to give optimum results as to the holographic image. The images obtained were not of particularly high efficiency but the reso lution of the images was good. One would expect a high tanning developer such as pyrocatechol to have less of a relief image forming effect on a thin emulsion such as Agfa 10E70 film (about 5 microns) than on a thick emulsion such as Kodak 649-F^ plates (about 18 microns). Thus a smaller diffraction efficiency and smaller signal to noise ratio might be expected with Agfa 10E70 film, although no qualitative data were taken. The printout effect was studied in a much more qual itative manner. The Kodak Reversal Bleach System was Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 37 further modified in this investigation by the omission or substitution of a certain processing step to better under stand how each step changes the printout resistance and transparency of the emulsion. The first variation of The Kodak Reversal Bleach System was the replacement of the special developer with D-19. The second variation was the replacement of the special developer with D-76. The third variation was the omission of the stain remover. The fourth variation was the omission of the clearer. The fifth variation was the omission of both the stain remover and the clearer. Figures 9-13 illustrate the transparency response of the bleached emulsions to the alterations of The Kodak Reversal Bleach System while Table V gives the final absolute and normalized transparencies of these alter ations. Developing the hologram with the special developer, with D-19» or with D-76 produces transparency and print out behavior responses which are almost indistinguishable. Holograms processed without the stain remover were un changed in transparency from holograms processed utilizing the stain remover; however, the printout was noticeably less extreme indicating that the potassium permanganate which is the working agent in the stain remover tends to speed printout darkening in the emulsion. Holograms processed without the clearer were much less transparent Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. without prohibited reproduction Further owner. copyright the of permission with Reproduced Normalized Percentage Absolute Percentage Figure 9- Time Variation of Absolute and ofand Normalized Absolute TimeVariation 9-Figure of Transmitted Light of Transmitted Light 40 80 65 60 90 r 90 n 0 1 0 and and (KBBS) System TheBleach Kodak Reversal with processed of Transparency Holograms developer in The Kodak Reversal Bleach System Bleach Reversal developer Kodak Thein 1 processed with D—19 substituted as the assubstituted D—19 processedwith 2 2 3 3 A O Reference, D-19 developed D-19 Reference, O Time inWeeks Time Time in Timein Weeks 4 oa eeslBec System Bleach Reversal Kodak 5 5 6 6 (KKBS) 7 7 8 8 9 9 10 10 O Reference, Developed in D-19 A Developed in D-76 40 0 1 4 62 8 10 Time in Weeks 90 0) W-P 85 aJ si -p *0 C -H o o 80 © © Ph -P -P 'O -H 75 © S N © - h q H 0$ 70 <3 U g * O V t a o 65 60 XX X 4 5 6 8 10 Time in Weeks Figure 10, Time Variation of Absolute and Formalized Transparency of Holograms processed with The Kodak Reversal Bleach System (KRBS) substituting D-19 and D-76 as developers Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 65 i-, •p © J2 ui u - _ _ 40 0 4 5 6 8 10 Time in Weeks 90 © W-P 85 aS jS - p W C - H © o 80 Ft *a © © P4-P -p TJ -H 75 © g N © £ 70 as h S eh u o 60 _L ± ± 4 5 6 8 10 Time in Weeks Figure 11. Time Variation of Absolute and normalized Transparency of Holograms processed with The Kodak Reversal Bleach System (KRBS) substituting D-19 as the developer and substituting D-19 as the developer along with removal of the stain remover Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 4 1 7 0 1- O Reference, Developed in D-19 +» ® x i low aJ-H 60 A Developed in D-19 and processed 4* Id without the clearer © T3 o © 50 - Jh -P © + » P4-H a © © -p c 40 “ 2 gS rH fl O £4 © .0*4 30 < O 20 XX X X 0 4 5 6 7 8 10 Time in Weeks 100 © W-P 90 CSX! - P W d -H © id o 80 © © 034 +» -P 'O t4 70 © a n m § as d 60 g * o *4 55 o 50 40 _L X X X 4 5 6 7 8 10 Time in Weeks Figure 12. Time Variation of Absolute and Normalized Transparency of Holograms processed with The Kodak Reversal Bleach System (KRBS) substituting D-19 as the developer and substituting D-19 as the developer along with removal of the clearer Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. if S ^ ^ 7 ! V ■’ J ^ 1'- . ^ ,•■*-■'' '''-** \T- ■, ’ <(”??, '■ J - »*L '' ■ .* ■■-'■■ .. . ,- _ •■■_. . ,\~ *-S : , - : C ■ ■ .‘"T1'. ' ,'^v^V ■*■..■ V '- ■ .■ *. '■*<_ . ‘‘t- ,-■' 42 60 O Ho stain remover ■p OSS V k O 50 A Ho c le a re r aS *H •Pt-3 C © T3 lO Ho stain remover or clearer O © Ft -P 40 © -P P*-H S © 03 30 •P C 3 aJ rl F» O ^ © 2 0 <: o 10 XXX 0 4 - 5 6 8 10 Time in Weeks 1 0 0 i—, © W-P 90 as - P w ©C -H»-3 O 80 Ft >© © © Ph +> -P 'CJ -H 70 © S 63 © ■H £ i—i as as Ft 60 I 51 O VH S5 o 50 40 X I ^ -3 4 5 6 8 10 Time in Weeks Figure 13. Time Variation of Absolute and normalized Transparency of Holograms processed with. The Kodak Reversal Bleach System (KBBS) substituting D-19 as the developer and: 1) processed without the stain remover, 2) processed without the clearer, 3) processed without either the stain remover or the clearer Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 43 Table V Final Absolute and Normalized Transparencies of Holograms Processed with The Kodak Reversal Bleach System and Processed with the Five Modifications Performed on The Kodak Reversal Bleach System Absolute Normalized Transparency Transparency Kodak Reversal Bleach System 40% 66 % Developed with D-19 42% 65% Developed with D-76 38% 64% Without Stain Remover 39% 74% Without Clearer 28%------47%---- Without either Stain Remover or Clearer 32% 67% and much more susceptible to printout than holograms processed utilizing the clearer. This indicates that sodium bisulfite which is the working agent in the clearer is an important chemical in retaining high transparency and high resistance to printout in The Kodak Reversal Bleach System. Transparency and printout are moderate with holograms processed without either the clearer or the stain remover. This is reasonable since processing without the clearer yields holograms very susceptible to printout and low transparency while processing without the stain remover yields holograms which have the opposite qualities as those just mentioned. The quality of the Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 4 4 holographic images was not noticeably different with any of the above mentioned alterations, although no qualitative data were taken. The Kodak Reversal Bleach System is not particularly impressive as far as printout behavior is concerned. Since Agfa 10E70 emulsions are thinner than Kodak 649-F plates, the tanning action of the developer used in this process probably is not as effective as could be hoped for with thicker emulsions. Although the process shows a 31% decrease in transparency over a period of ten weeks indi cating that the printout effect is a problem in this process, it was found that sodium bisulfite is a useful chemical in curtailment of the printout effect. The Modified Developer Process The third process studied was that of Hariharan, 58 Kaushik, and Hamanathan . This process, which has as its special property a modified developer, will be called in this paper The Modified Developer Process. This process is a result of modifications of The Kodak R-10 Bleach 5Q Process which was first used by Altman*^* and later by Russo and Sottini6®, McMahon and Franklin63*, TJpatnieks and Leonard6^, and McMahon and Maloney6^. The initial R-10 Bleach Process utilized sodium chloride to change the final developed silver image into a silver chloride com- plex; however, McMahon and Franklin as well as TJpatnieks and Leonard6 *5 reported that R-10 Bleaches belong to a class Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. of printout enhancing materials- It was left to McMahon 66 and Maloney to show with qualitative data that the stability against printout is essentially determined by the silver halide of which the image is formed, silver chloride being the poorest, silver bromide being somewhat better, silver iodide being the best, exhibiting a high 67 resistance to printout darkening- McMahon and Maloney thus modified The Kodak R-10 Bleach Process to incor porate a potassium iodide solution in order to change the final image into a silver iodide. The modified process worked fine with thin emulsion Agfa materials but poor results as far as image formation was concerned were obtained when the process was used on go thicker Kodak 649-F plates. Hariharan and Eamanathan theorized that since silver iodide has a relatively high solubility in solutions of potassium iodide the solvent action of potassium iodide could result in etching of the halide image and loss of the high spatial frequency inter ference pattern inherent in the hologram. By lowering the concentration of potassium iodide in the bleach bath, the etching should be reduced. The Kodak R-10 Bleach was modified so that 2 grams potassium iodide per 12 liters of water were used instead of 128 grams potassium iodide per 1 2 liters of water, resulting in better holo graphic images and negligible levels of staining as compared to the higher concentration of potassium iodide. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 46 Up to this point the process had teen a direct bleaching process; the emulsion being developed, fixed, and then bleached. By accident, Eariharan, Ramanathan, go and Kaushik ^ treated an unfixed hologram in a dichronate bleach containing potassium iodide and obtained a remark ably good holographic image. Such a treatment should convert the developed silver grains into sites of silver iodide and result in a very weak phase image because of the small refractive index difference between silver bromide (n = 2.25) and silver iodide (n = 2.21). Reasons cited for this phenomenon include dissolution of the unexposed silver halide grains by the bleach bath as well as oxidation of the silver image by the bleach to Ag+ resulting in the unexposed emulsion grains growing slight ly larger forming an intensified phase image. They tried different concentrations of potassium iodide in the bleach bath and found 2 grams of potassium iodide per 20 liters water gave optimum results in diffraction efficiency and signal to noise ratio of the holographic image. In the same paper it was reported that the bleach of ammonium dichromate used in The Kodak R-10 Bleach Process yielded poorer overall results than using potassium dichromate as the bleaching agent. Although no qualitative data were given, they reported that the stability against printout was almost as good as silver iodide phase holo grams produced by bleaching a silver image by conventional Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 4-7 means and much better than silver bromide phase holograms. Further work was done by Eariharan, Kaushik, and Hamanathan*^ where they pointed out that the scattered optical noise inherent in bleached holograms is proportional to the square of the volume of the transparent grains representing the image and also learned experimentally that the maximum values of diffraction efficiency are obtained when only a small fraction of the available silver halide in the emulsion is used. Combination of these facts means that a controlled etching of the emulsion grains in a solution of a suitable silver halide solvent to reduce their size will yield a hologram with very low optical noise and a very high diffraction efficiency. After extensive testing the same group added 0. 5 grams of sodium thiosulfate to the developer to act as the etching agent. The holographic images were reported to have a significant increase in signal to noise ratio (roughly 60 to 1 which is comparable to unbleached holograms), without a decrease in the diffraction efficiency. To date this is the final modification, and this process can be described as a simple negative phase image process capable of producing holo graphic images of reported high diffraction efficiency and low optical noise. The essential processing steps of The Modified Developer Process are given in Table 71. The Modified Developer Process was by far the simplest process of the ones investigated in this paper. The Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 4 8 Table 71 The Essential Processing Steps of The Modified Developer Process Step 1 ...... Sodium Thiosulfate Step 2 ...... Potassium Dichromate and Potassium Iodide brightness and resolution of the holographic image were both very good, although no qualitative data were taken. The effects of printout darkening were studied in a much more qualitative manner. The Modified Developer process was further modified in this investigation by the omission or substitution of a certain processing step to better understand how each step changes the printout resistance of the emulsion. The first variation of The Modified Developer Process was the replacement of the modified developer with D-19. The second variation was the replacement of the modified developer with D-76. The third variation was the omission of potassium iodide from the bleach bath solution. Pigures 14-16 illustrate the transparency response of the bleached emulsions to the alterations of The Modified Developer Process while Table 711 gives the final absolute ana normalized transparencies of these alterations. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. O Reference, Developed in D-19 A The Modified Developer Process WU bO (MDP) <3 -h -p>-3 o o 60 ^ -p o -P P4 -H -P C 3 efl & «H <$ O 40 0 1 2 3 4 6 7 8 95 10 Time in Weeks 85 a> M-P 80 «3;C -P V C-H XXX 55 0 4 5 6 8 10 Time in Weeks Figure .14. Time Variation of Absolute and normalized Transparency of Holograms processed with The Modified Developer Process (MDP) and processed with D-19 substituted as the developer in The Modified Developer Process Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. without prohibited reproduction Further owner. copyright the of permission with Reproduced Figure 15. Time Variation of Absolute and Normalized and Absolute of Variation Time 15. Figure Normalized Percentage Absolute Pe:fcentage of Transmitted Light °f Transmitted Light 65 85 80 r 2 1 0 Transparency of Holograms processed with processed Holograms of Transparency h oiidDvlprPoes (MDP) Process Developer Modified The substituting D-19 and D-76 as developers as D-76 and D-19 substituting 3^5678 9 3^5678 10 A Developed in in Developed A O Reference, Developed in D-19 in Developed Reference, O Time in Weeks in Time Weeks in Time H-76 10 50 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. without prohibited reproduction Further owner. copyright the of permission with Reproduced Normalized Percentage Absolute Percentage of Transmitted Light of Transmitted Light Figure 16. Time Variation of Absolute and Normalized and Absolute of Variation Time 16. Figure 60 0 - 80 40 45 r 0 7 50 65 55 60 0 1 with omission of potassium iodide from iodide potassium of omission with h oiidDvlprPoes (MDP) Process Developer with Modified processed The Holograms of Transparency the bleach bath bleach the substituting D-19 as the developer along developer the as D-19 and developer substituting the as D-19 substituting 2 3 A Developed in D-19 and processed and D-19 in Developed A O Reference, Developed in D-19 in Developed Reference, O Time in Weeks in Time without potassium iodide potassium without Time in Weeks in Time 4 5 6 7 8 9 10 10 52 Table VII Pinal Absolute and Normalized Transparencies of Holograms Processed with The Modified Developer Process and Processed with the Three Modifications Performed on The Modified Developer Process Absolute Normalized Transparency Transparency Modified Developer Process 54% 72% Developed with D-19 41% 63% Developed with D-76 43% 70% Without Potassium Iodide 44% 6 6 % The absolute and normalized transparency of holograms processed with The Modified Developer Process were higher than those of any of the alterations. Developing with D-76 yields holograms which are slightly more transparent and more resistive to printout than holograms developed with D-19. Printout was less severe when potassium iodide was omitted, which is a fact difficult to explain. Per haps the small concentration of potassium iodide in the bleach bath does not work as effectively on Agfa emulsions* since The Modified Developer Process was developed to use on Kodak 649-P emulsions which are several times thicker. Although holograms processed with The Modified Developer Process had transparencies and printout resistance supe rior to any of the alterations made in this investigation, Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 53 the printout "behavior of this process is still quite a problem. The quality of the holographic images was slight ly superior when processed using The Modified Developer Process in comparison to any of the alterations, although no qualitative data were taken. The Modified Reversal Bleach Process The fourth process investigated was The Modified 71 Reversal Bleach Process initiated by Hariharan and 72 finalized by Hariharan and Ramanathan . This process can be described as a true reversal bleach system. Hariharan and Ramanathan‘ further explored methods of converting silver bromide phase holograms to silver iodide phase holograms. The problem was to introduce the iodide ion in a form which would not result in for mation of soluble complexes in the emulsion. Since quaternary ammonium iodides behave like strong electro lytes when in solution, Ag+ would be readily converted to silver iodide and the solubility of silver iodide in the solution would be small. They concluded that holo grams treated in a 0 .2% solution of tetramethylammonium iodide^ resulted in excellent holograms with low optical noise, high diffraction efficiency, and good resistance to printout. The essential processing steps of The Modified Reversal Bleach Process are given in Table VIII. The Modified Reversal Bleach Process produced holo- Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 54 Tat>le 7III The Essential Processing Steps of The Modified Reversal Bleach Process Step 1 ...... Develop in Kodak D-19 Step 2 ...... Re-expose uniformly to White Light Step 3 ...... Redevelop in Kodak D-19 Step 4 ...... Bleach in Potassium Dichromate Step 5 ...... Clear in Tetramethylammonium Iodide grams with optical noise lower than any other process tested in this paper and diffraction efficiencies as good as with any process tested, although no qualitative data were taken. The re-exposure to uniform light was found to he quite critical as to exposure intensity and time. With Agfa 10E70 film the re-exposure was done by a 25 watt light bulb at a distance of 4 feet for a duration of 0 . 5 seconds. The effects of printout were studied in a much more qualitative manner. The Modified Reversal Bleach Process was further altered in this investigation by the omission or substitution of a certain processing step to better understand how each step changes the printout resistance of the emulsion. The first variation of The Modified Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 55 Reversal Bleach Process was the replacement of D- 1 9 with 3>-76 as the developer. The second variation was the substitution of sodium bisulfite for tetramethylammonium iodide as the clearer. The third modification was the omission of the clearer. Figures 17-19 illustrate the transparency response of the bleached emulsions to the alterations of The Modi fied Reversal Bleach Process while Table IX gives the final absolute and normalized transparencies of these alterations. Table IX Pinal Absolute and Normalized Transparencies of Holograms Processed with The Modified Reversal Bleach Process and Processed with the Three Modifications Performed on The Modified Reversal Bleach Process Absolute Normalized Transparency Transparency Modified Reversal Bleach Process 46% 82% Developed with D-76 45% 84% Cleared with Sodium Bisulfite 49% 74% Without Clearer 43% 71% The Modified Reversal Bleach Process yields holograms which hold 82% of their initial transparencies which clas sifies this process as the best yet investigated for permission of the copyrightowner. Further reproduction prohibited without permission Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. without prohibited reproduction Further owner. copyright the of permission with Reproduced Normalized Percentage Absolute Percentage of Transmitted Light of Transmitted Light Figure 17 • Time Variation of Absolute and Normalized and Absolute of Variation Time 17 •Figure 100 80 - 80 70 40 40 - 60 0 0 1 1 Process and processed with with processed and developer in The Modified Reversal Bleach Reversal Modified The in developer h oiidRvra lahPoes (MRBP) Process Bleach Reversal with Modified processed The Holograms of Transparency 2 2 3 3 A Developed in D-76 in Developed A eeec, (MRBP) Reference, O Time in Weeks in Time Time in Weeks in Time 4 4 7 5 5 D-76 6 6 substituted as the as substituted 7 8 8 9 10 9 10 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. without prohibited reproduction Further owner. copyright the of permission with Reproduced Normalized Percentage Absolute Percentage of Transmitted Light of Transmitted Light 0 r 70 80 Figure 18. Time Variation of Absolute and Normalized and Absolute of Variation Time 18. Figure clearer in The Modified Reversal Bleach Process Reversal Modified The in clearer and processed with Sodium Bisulfite as the as Bisulfite Sodium (BRBP) with Process processed and Bleach Reversal with Bodified The processed Holograms of Transparency Time in Weeks in Time Time in Weeks in Time eeec, (MRBP) Reference, Processed with Sodium Eisulfite Sodium with Processed as the clearer the as Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. without prohibited reproduction Further owner. copyright the of permission with Reproduced Normalized Percentage Absolute Percentage Figure 19* Time Variation of Absolute and Normalized and of Absolute Variation Time 19* Figure of Transmitted Light of Transmitted Light 80 60 40 1 0 The Modified Reversal Bleach Process Bleach Reversal Modified The in clearer the without processed and h oiidRvra lahPoes (MBBP) Process Bleach Reversal Modified The with processed Holograms of Transparency 2 3 A A O O Time in Weeks in Time Time in Weeks in Time Processed without the clearer the without Processed eeec, (MRBP) Reference, 5 6 7 8 9 10 10 59 resisting printout. Substituting D-76 as the developer changed the transparency response very little. Clearing with sodium "bisulfite produced holograms which were more transparent yet more susceptible to printout than holograms cleared in tetramethylammonium iodide. Processed holograms which were not cleared were slightly less transparent and severely more susceptible to printout than holograms cleared either with sodium bisulfite or tetramethyl ammonium iodide. Uo significant differences could be seen in the holographic images processed by the different alterations although no qualitative data were taken. The Agfa Process The final process investigated was that recommended by Agfa-Gevaert*^ to produce phase holograms. The bleach utilized is potassium dichromate, the same used by three of the processes investigated in this paper. The unusual thing about The Agfa Process is that the 76 desensitization bath incorporates phenosafranine as the active material. Phenosafranine is a well known red dye and was found to be a powerful photographic desensitizer by Luppo—Cramer*^ who showed that adding it to a developer in one part per twenty thousand enabled the photographic plate to be examined in a bright light after only a one minute development and also that adding it to a prebath enabled development to be carried out in the presence of Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 60 a considerable amount of light, Chang and George*^8 reported soaking plates in a solution of safranine aconc, a material similar in structure to phenosaf ranine, and reported that plates turned darker at a slower rate when treated with this material. They conjecture that such dyes cause the gelatin to absorb strongly in the blue acting as a blue filter blocking light off from the silver halide grains. The essential processing steps of The Agfa Process are given in Table X. Table X The Essential Processing Steps of The Agfa Process Step 1 ...... Develop in Xodak D-19 Step 2 ...... Bleach in Potassium Dichromate Step 3 ...... Clear in Sodium Sulfite and Sodium Hydroxide Step 4 ...... Desensitize in Phenosaf ranine The Agfa Process produced holograms which yielded holographic images which were good as far as brightness and resolution are concerned although no qualitative data were taken. The effects of printout darkening were studied in a much more qualitative manner. The Agfa Process was fur Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 61 ther modified in this investigation by the omission or substitution of a certain processing step to better understand how each step changes the printout resistance of the emulsion. The first variation of The Agfa Process was the replacement of D-76 for D-19 as the developer. The second variation was the omission of phenoseXranine from the desensitization bath. The third variation was the omission of the entire desensitization bath. The fourth variation was the omission of the clearer. Figures 20-22 illustrate the transparency response of the bleached emulsions to the alterations of The Agfa Process while Table XI gives the final absolute and normalized transparencies of these alterations. Table XI Final Absolute and Normalized Transparencies of Holograms Processed with The Agfa Process and Processed with the Four Modifications Performed on The Agfa Process Absolute Normalized Transparency Transparency Agfa Process 53% 32% Developed with D-76 57% 92% Without Phenosafranine in the Desensitizer 45% 67% Without De sensitizer 46% 70% Without Clearer 55% 90% Reproduced with permission of the copyright owner. Further reproduction prohibited without permission 70 ■p O Beference, (AP) *o w © -h A Developed in D-76 ■PhI S3 © •© o © Sh - P 60 © -P P* -H a 0) CQ ■P S3 55 © «J rH St O £-1 CO S> Vi 50 < o 0 1 2 3 56 7 8 9 10 Time in Weeks 100 fcO-P 05 Si -p V S3-H © 1-3 o Sn © © Pl-P -P ©N 8© 05nr - h a iH © © u 80 O «H » o 10 Time in Weeks Figure 20. Time Variation of Absolute and normalized Transparency of Holograms processed with The Agfa Process (AP) and processed with D-76 substituted as the developer in The Agfa Process Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. without prohibited reproduction Further owner. copyright the of permission with Reproduced Normalized Percentage Absolute Percentage of Transmitted Light of Transmitted Light Figure 21. Time Variation of Absolute and Normalized and Absolute of Variation Time 21. Figure 100 70 60 80 r 'O 1 0 The Agfa Process (AP) and processed without processed (AP) and Process Agfa The with processed Holograms of Transparency the clearer in The Agfa Process Agfa The in clearer the 2 3 A Processed without the clearer the without Processed A eeec, (AP) Beference, O Time in Weeks in Time Weeks in Time 4- 5 6 7 8 9 10 10 6 4 70,- O Reference, (AP) O Processed without the desensitizer -p 65 ©.S3tcbd ca-H A Processed without phenosafranine - P p ! in the desensitizer c 60 © o © Ft -p © -p Ph -H S 55 © © -p S3 3 aJ «—) ^ 50 O =H © C O 45 40 ± _L _L 4 5 6 8 10 Time in Weeks 90 r I S3 -H 10 Time in Weeks Figure 22. Time Variation of Absolute and normalized Transparency of Holograms processed with The Agfa Process (AP;, processed without phenosafranine in the desensitizer of The Agfa Process, and processed without the desensitizer in The Agfa Process Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 65 Holograms developed in D-76 had suprisingly higher transparencies and higher resistance to printout than holograms developed in D-19. Holograms processed without phenosafranine in the desensitization hath exhibited the lowest transparency levels and lowest resistance to print out of any alteration indicating that phenosafranine is a very powerful substance in producing holograms which have high transparency and high resistance to printout. Holograms processed without the desensitization bath have transparency responses quite similar to holograms proc essed without just phenosafranine. These curves therefore justify the statement that phenosafranine is the only active chemical in the desensitization bath optimizing holographic transparency responses. Holograms processed without the clearer were more transparent and less sus ceptible to printout than holograms processed with The Agfa Process, indicating that the chemicals sodium hy droxide and sodium sulfite in the clearer do little clearing, but do sensitize the emulsion slightly to printout darkening. No significant differences could be seen in the holographic images processed by the different alterations, although no qualitative data were taken. Removal of the clearing bath, developing in D-76, and using phenosafranine as a desensitizer yields holograms which hold about 9 0% of their initial transparency, by far the best process investigated for resisting printout. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. CHAPTER YI ATTEMPTS TO IMPROVE HOLOGRAPHIC IMAGES In addition to testing the five processes described previously, other attempts were made to develop bleached holographic images of better quality as well as trying to understand more fully the printout phenomenon. Printout Resulting from Variable Light Intensities The first experiment designed was to try to correlate the printout effect as a function of light intensity incident upon the processed hologram. Five holograms were processed using The Modified Developer Process and five processed using The Modified Reversal Eleach Process. A hologram from each process was placed at distances of 8, 4, 2, 1, and 0.5 feet from a 75 watt incandescent light bulb. The holograms were illuminated twenty-four hours a day and monitored on the Bausch and Lomb micro- photometer every three days in the same manner as de scribed previously. Pigures 23 and 2-‘: show the trans parency and printout behavior of each hologram as a function of time. Por The Modified Developer Process the final trans parency levels are as follows; 8 feet, 82%; 4 feet, 80%; 2 feet, 76%; 1 foot, 64%; 0.5 feet, 63%. The same values for The Modified Reversal Bleach Process are as follows: 8 feet, 89%; 4 feet, 85%; 2 feet, 79%; 1 foot, 65%; 0.5 66 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. without prohibited reproduction Further owner. copyright the of permission with Reproduced Figure 23* Time Variation of Absolute and normalized and Absolute of Variation Time 23* Figure Absolute Percentage of Transmitted Light 35 50 55 65 60 inducing light source light printout inducing a from distances various at The Modified Developer Process arranged Process Developer Modified The Transparency of Holograms processed with processed Holograms of Transparency Time in Days in Time 2 5 8 21 18 15 12 . foot 0.5 4 feet 4 1 foot 1 8 feet 8 2 feet 2 67 60 70 80 omlzd ecnae f rnmte Light Transmitted of Percentage Normalized V 8 f e e t 6 8 4 feet 6 5 r 2 feet 100 ■p 95 § s i I •© 90 £ Q> © -P P* -P *ri ►d e © CD c 85 g cS Ft © e* c f © 12 15 18 Time in Days Figure 24. Time Variation of Absolute and normalized Transparency of Holograms processed with The Modified Reversal Bleach Process arranged at various distances from a printout inducing light source Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 69 feet, 70%. Although the relationship is not simple, it does appear that the printout effect is more severe as the light intensity increases. Printout Resulting from Wavelength Variation of Light The second experiment was designed to study the printout effect as a function of the wavelength of light striking the emulsion. Six holograms were processed using The Modified Reversal Bleach Process and each was placed behind a filter which allowed only monochromatic light to strike it. The light source was an incandescent light bulb and the filters were arranged so that equal inten sities of monochromatic light struck each hologram. The transparency of each hologram was monitored by the Bausch and Lonb microphotometer as described previously. Figure 25 shows the transparency and printout behavior of each hologram as a function of time. After a thirty day period of time the following transparency percentages of the original transparency were recorded: yellow filter, 73%; green filter, 79%; blue filter, 80%; blue-green filter, 84%; opaque filter (no light striking the emulsion), 92%; red filter, 95%. Although the results are inconclusive as far as finding a working correlation between wavelength and printout darkening, they do show a couple of notable features: 1) holograms tend to darken even in the dark, Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. without prohibited reproduction Further owner. copyright the of permission with Reproduced Figure 25* Time Variation of Absolute and Normalized and Absolute of Variation Time 25* Figure Absolute Percentage of Transmitted Light 60 0 3 in front of a printout inducing light inducing printout a of placed front filters in different with Process Bleach arranged Reversal Hodified The Transparency of Holograms processed with processed Holograms of Transparency 6 1 1 1 2 2 2 30 27 24 21 18 15 12 9 Time in Bays in Time Black □ Blue-Green Blue Yellow Green 100 80 omlzd ecnae f rnmte Light Transmitted of Percentage Normalized 71 2) putting holograms in an environment where only red filters are used for illumination will insure a long life for holograms with respect to printout darkening. Printout Hesuiting from Ultrasonic Agitation In attempting to develop bleached holographic images of better resolution and brightness, the idea of trying to produce finer grained emulsions was explored. The reason for producing an emulsion with smaller grain size would be an increased probability in higher resolution of the holographic image. In a typical ultrasonic cleaner a drop of mercury after a short period of time will be completely disso ciated throughout the containing bath of water. If an unexposed photographic emulsion was placed in an ultra sonic cleaner, it might be reasonable to expect that the emulsion grains would be broken down into smaller par ticles. Unexposed Agfa 10E70 film was processed in a Bendix Sonic Energy Cleaner*^ for a five minute period of time. The film was then allowed to air dry for three days. Holograms were then processed in one of three ways: 1) developed in D-19, then bleached in potassium di- chromate; 2) developed in D-19, bleached in potassium dichromate, then desensitized in phenosafranine; 5) developed in D-19» re—exposed to uniform light, re developed in D-19 (reversal bleached), then desensitized Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 72 in phenosafranine. Figure 26 shows the transparency and printout behavior of each modification as a function of time. Holograms processed by methods two and three produced very weak holographic images while the images produced in method number one were only fair. The transparency of holograms processed v/ith the ultrasonic unit went from 42% to 52%. Holograms processed by method number one held only 63% of their initial transparency after a thirty day period of time while method number two holograms eventu ally held 98% of the initial transparency after recovery from 83% after three days and method number three holo grams eventually held 94% of the initial transparency after recovery from 81% after a three day period. Al though holograms processed using the ultrasonic unit have images which range from fair to poor, their printout resistance is very high when suitably processed. Ultrasonic Agitation Effect upon Wavelength Sensitivity The Bendix Sonic Energy Cleaner was also used in 80 studying the effects of processing Kodak S.A.-3 spectro- graphic plates through the cleaner with regard to possible increased resolution of spectral lines. An S.A.-3 plate was placed in the ultrasonic cleaner for five minutes, let dry for five days, and then positioned in a Hilger Medium Quartz Spectrograph®^. A rotating step sector was Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. to r 73. O Developed and bleached 4* 9Sl 65 - O Developed, bleached, and desensitized 00 M 05 *H +» p! A Developed, reversal bleached, C 9 * 0 60 “ and desensitized O 40 12 15 18 21 24 27 30 Time in Days 100 95 a> to*> a si 90 -p u> a> pi o Fh 85 © < D f4-P •P •O -H ® 8 80 - n m ■H pH OS Fh 75 g * O 5 5 O 70 65 X ± 12 15 18 h Si 2*7-- 3^ Time in Days Figure 26* Time Variation of Absolute and Normalized Transparency of Holograms processed with different modifications after agitation of the unexposed film in an ultrasonic cleaner Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 74 positioned in front of the spectroscopic slit and twin iron electrodes were "burned "by an arc source for a forty second duration. She plate was then developed in D-19 for five minutes, put in a stop "bath for fifteen seconds, and finally fixed for three minutes in Kodak Eapid Fixer. Another S.A.-3 plate was processed in the exact same manner except that this plate was not agitated in the ultrasonic cleaner. After comparison of the dried plates no resolution difference could "be seen in spectral lines; however, the ultrasonically agitated plate appeared to have slightly darker spectral lines. An H & D curve was plotted from the unagitated plate and the darknesses of spectral lines were compared at intervals of about 250 angstroms. The ultrasonically agitated plate had spectral lines consistently darker than those on the unagitated plate, running from equal intensities to 1.4 times as dark. The significant point about the study is the fact that in the region of 4750 angstroms to 5300 angstroms the spectral lines were 1.3 to 1.4 times darker on the ultrasonically agitated plate, a fact hard to explain away by processing chemical changes, slight differences in spectroscopic processing, or initial differences between the plates. Figure 27 shows the ratio of spectral line darknesses as a function of wavelength. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 75 Pigure 27. Wavelength. Variation of the Darknesses of Spectral Lines on a Kodak S.A.-3 Spectro- graphic Plate Agitated in an Ultrasonic Cleaner before Exposure divided by the Darknesses of Spectral Lines on an Unagit&ted S.A.-3 Plate Effect of Toners on Brightness and Resolution A study of toners was also made in the hope that out of this branch of photographic processing a method could be found to produce holographic images of superior quality. Normally processed amplitude holograms were toned in one of four toner solutions: 1) Hypo Alum Toner (Agfa 222), 2) Iron Blue Toner (Agfa 241), 3) Sulfide Toner (Kodak T- 10), 4) Uranium Toner (Kodak T-9). Although no quali tative data were taken, the holographic image brightness and resolution were not improved with any of the toners but actually decreased in cases. A conclusion must be reached that toning of a hologram produces no improvement of the holographic image. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. Liquid Gates and Holographic Resolution Several articles in the literature(82“88) have mentioned using liquid gates to try to improve the reso lution of holographic images. Ideally this liquid gate would match the index of refraction of the gelatin and fill in any scattering centers produced by the formation of a relief image on the emulsion surface or by pock marks in the emulsion where metallic silver sites have been vacated by bleaching. Seven materials were investigated as to their ability to increase holographic image resolution when used as liquid gates on holograms produced on Agfa 10E70 films. The materials are as follows: 1) Xylene8^, 2) methyl Benzoate^8, 3) Chlorobenzene^, 4) Bromoethane^, 5) p-Chlorotoulene^, 6) 1,2-Dibromopropane^., 7) 1,3- Dibromopropane^. All of these materials have refractive index of approximately 1.50, the same as photographic gelatin. The liquid gates were formed by gluing with rubber cement a round washer made of bone onto the emulsion surface, filling the washer with the material, then cementing a thin glass slide onto the top of the washer. Although no qualitative data were taken, holographic image resolution did not change with any of the materials tested except xylene, where the image resolution was severely decreased. The probable formation of very small . \ .1 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 77 relief images on the relatively thin Agfa 10E70 emulsion might he one possibility as to why there is no resolution improvement. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. CHAPTER VII SELECTING AH OPTIMUM HOLOGRAPHIC PROCESS After the investigations were performed on the five processes described previously in Chapter IV, it was noted that combining the good aspects of some processes could possibly result in a general all around better process for producing phase holograms. Holograms were processed in one of the following twelve ways: 1) developed, then bleached; 2) developed, bleached, then processed in tetra- methylammonium iodide; 3) developed, bleached, processed in tetramethylammonium iodide, then processed in pheno safranine; 4) prehardened, developed, bleached, processed in tetramethylammonium iodide, then processed in pheno safranine; 5) developed, then reversal bleached; 6) de veloped, reversal bleached, then processed in phenosaf ranine; 7) developed, reversal bleached, then processed in tetramethylammonium iodide; 8) developed, reversal bleached, processed in tetramethylammonium iodide, then processed in phenosafranine; 9) developed in D-19, then bleached with The Modified Stanford Process bleach; 10) developed in D-19, fixed, then bleached with The Modified Stanford Process bleach; 11) developed in D-19, bleached with The Modified Stanford Process bleach, then processed in phenosafranine; 12) developed in D-19, fixed, bleached with The Modified Stanford Process bleach, then processed 78 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 79 in phenosafranine. Unless otherwise indicated, the de- - veloper used was the modified developer investigated in The Modified Developer Process and unless otherwise indi cated the bleaching agent was potassium dichromate. These twelve modifications are summarized in Table XII. Figures 28-33 illustrate the transparency response of the bleached emulsions to the alterations described previously while Table XIII gives the final absolute and normalized transparencies of these alterations. Holograms processed by methods number one and two both yielded final transparency levels of 4-2%, which was 75% of the initial transparency for method number one as compared to 79% of the initial transparency for method number two holograms. This indicates that processing in tetramethylammonium iodide does help in resisting printout by about 4% without changing the opacity of the hologram. The final transparency of method number three holograms was 44%, which was 90% of the original transparency. This shows that phenosafranine increased the normalized trans parency by 11% over holograms processed without it, even increasing the final transparency in doing so. The final transparency of method number four holograms was 47%, which was 87% of the initial transparency. It seems that pre hardening increases the transparency somewhat but also lowers the printout resistance slightly. The final trans parency of method number five holograms was 46%, which was Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 8 0 Table H I Summary o f The Western Michigan University Modifications MODIFICATION DESCRIPTION 1 ...... Developed, then bleached 2 ...... Developed, bleached, then cleared 3 ...... Developed, bleached, cleared, then desensitized 4- ...... Prehardened, developed, bleached, cleared, then desensitized 5 ...... Developed, then reversal bleached 6 ...... Developed, reversal bleached, then desensitized 7 ...... Developed, reversal bleached, then cleared 8 ...... Developed, reversal bleached, cleared, then desensitized 9 ...... Developed with D-19, then bleached with CuBr2 + PeCl^ 1 0 ...... Developed with D-19, fixed, then bleached with CuBr2 +■■■ PeCl^ 1 1 ...... Developed with D-19, bleached with CuBr2 + PeCl^, then desensitized 1 2 ...... Developed with D-19* fixed, bleached with CuBr2 + PeCl^, then desensitized Unless otherwise indicated the developer used was The Mod ified Developer investigated in chapter 17, and the bleach ing agent was potassium dichromate. The clearer refers to tetramethylammonium iodide and the desensitizer refers to phenosafranine. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 60 p ox! 55 O WMU Modification Number 1 «0 <30 9) P P P A WMU Modification Number 2 c © T J 50 O © -P © - P P* Pc 45 © © - P f j 3 30 XXX 12 15 18 21 24 27 30 Time in Days 90 © 85 w p « JS P V C-H © P 80 O f-i •© © © P * P P 75 T3 P © N 6© P s «-» «a 70 05 ft n * o Vi S3 o 65 60 X XX 12 15 18 21 24 27 30 Time in Days Figure 28. Time 'Variation of Absolute and Normalized Transparency of Holograms processed with Western Michigan University Modifications One and Two Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. without prohibited reproduction Further owner. copyright the of permission with Reproduced Normalized Percentage Absolute Percentage of Transmitted Light of Transmitted Light Figure 29. Time Variation of Absolute and Normalized and Absolute of Variation Time 29. Figure 40 80 0 3 Western Michigan University Modifications University Michigan Western Two and Three and Two processed, Holograms of with Transparency 6 A A O O 1 1 1 2 2 2 30 27 24 21 18 15 12 9 WMU Modification Number 2 Number Modification WMU WMU Modification Number Number Modification WMU Time in Days in Time Days in Time 2 5 18 15 12 21 3 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. without prohibited reproduction Further owner. copyright the of permission with Reproduced Normalized Percentage Absolute Percentage of Transmitted Light of Transmitted Light lOOp Figure 30. Time Variation of Absolute and Normalized and Absolute of Variation Time 30. Figure 80 J 3 9 2 5 8 1 4 7 30 27 24 21 18 15 12 9 6 3 0 ---- 1 --- Western Michigan University Modifications University Michigan Western Three and Four and Three Transparency of Holograms processed with processed Holograms of Transparency 1 ---- A O 1 ---- Time in Lays in Time Time in Lays in Time WMU Modification Number 4 Number Modification WMU 3 Number Modification WMU 1 __ I ____ I ____ I____I ___ I 1 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. without prohibited reproduction Further owner. copyright the of permission with Reproduced Normalized Percentage Absolute Percentage Figure 31. Time Variation of Absolute and Normalized and Absolute of Variation Time 31. Figure of Transmitted Light of Transmitted Light 100 70 65 50 60 55 0 0 3 3 Five, Six, and Seven and Six, Five, Modifications University Michigan Western Transparency of Holograms processed with processed Holograms of Transparency 6 6 1 1 1 2 2 2 30 27 24 21 18 15 12 9 Q O O A O O Time in Lays in Time WMU Modification Number Modification WMU WMU Modification Number Modification WMU WMU Modification Number Modification WMU 2 5 8 1 4 7 30 27 24 21 18 15 12 Time in Lays in Time 84 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. without prohibited reproduction Further owner. copyright the of permission with Reproduced Normalized Percentage Absolute Percentage of Transmitted Light of Transmitted Light 100 110 105 0rA r 70 Figure 32. Time Variation of Absolute and Normalized and of Absolute Variation Time 32. Figure - Western Michigan University Modifications University Michigan Western Six, Seven, and Bight and Seven, Six, Transparency of Holograms processed with processed Holograms of Transparency O WMU Modification Number 6 Number Modification WMU O WMU Modification Humber 7 Humber Modification WMU WMU Modification Number 8 Number Modification WMU Time in Days in Time 2 5 8 1 24 21 18 15 12 ie n Days in Time 12 18 24 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. without prohibited reproduction Further owner. copyright the of permission with Reproduced Normalized Feroentage Absolute Percentage of Transmitted Light of Transmitted Light 110 100 120 45 40 80 Figure 33. Time Variation of Absolute and Normalized and Absolute of Variation Time 33. Figure 70 „ 70 35 60 65 50 55 0 3 Nine, Ten, Eleven, and Twelve and Eleven, Ten, Nine, Western Michigan University Modifications University Michigan Western Transparency of Holograms processed with processed Holograms of Transparency 6 1 1 1 2 2 2 30 27 24 21 18 15 12 9 A O O Q HOT 0 Time in Lays in Time Lays in Time HOT HOT WMU 11 Number Modification oiiainnme 9 number Modification Modification Number 10 Number Modification Modification Number Number 12 Modification 4 7 30 27 24 ^ — - A Table XIII Pinal Absolute and Normalized Transparencies of Holograms Processed with The Twelve Western Michigan University Modifications Absolute Normalized Transparency Transparency Modification Number 1 42% 75%' Modification Number 2 42% 79% Modification Number 3 44% 90% Modification Number 4 47% 87% Modification Number 5 46% 71% Modification Number 6 63% 90% Modification Number 7 63% 101% Modification Number 8 62% 105% Modification Number 9 52% 91% Modification Number 10 66% 96% Modification Number 11 53% 114% Modification Number 12 69% 107% only 71% of the initial transparency. The final trans parency of method number six holograms was 63%» which was 90% of the initial transparency, indicating that pheno safranine increased transparency by 17% and printout resistance by 19%. The final transparency of method number seven holograms was 63%» which was 101% of the initial transparency • The transparency level dropped to 96% of Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. r- 88 the original after three days but quickly recovered to the final value. Tetramethylammonium iodide thus in creased the transparency by 16% and the resistance to printout by 30%. The final transparency of method number eight holograms was 62% which was 105% of the initial transparency, this level never dropping to less than 100% and never going above 106%. It appears that with reversal bleached holograms tetramethylammonium iodide has a greater resistance to printout than does pheno- safranine, just the opposite of what occurs with holograms processed with a negative phase image process. The final transparency of method number nine holograms was 52%, which was 91% of the original transparency. However, this normalized value was only 66% after three days, re covering slowly as time progressed. The final transparency of method number ten holograms was 66%, which was 96% of the original transparency. This normalized value dropped to 89% after three days but slowly recovered to the present value. Since this recovery phenomenon occurs both with fixed and unfixed holograms, the recovery must be linked with the bleach bath used in The Modified Stanford Process. The final transparency of method number eleven holograms was 53%» which was 114% of the initial value, the lowest normalized value being 99% after three days. The final transparency of method number twelve holograms was 69%, which was 107% of the initial value, the lowest normalized Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 89 value "being 99% after six days. It appears that pheno- safranine staves off the initial severe degradation inherent to holograms "bleached with The Modified Stanford Process "bleach and then they recover above "the initial transparency "by some mechanism still unclear, "but very possibly connected to the materials used in the bleach bath. Holograms processed with methods number eight and twelve were the only ones which showed excellent resis tance to printout, high transparency, and good emulsion stability. Therefore, further trials were done on holo grams bleached in one of three manners: 1) developed in The Modified Developer Process developer, reversal bleached in potassium dichromate, cleared in tetramethyl ammonium iodide, then desensitized in phenosafranine; 2) developed in D-19» fixed, bleached in ferric chloride and cupric bromide, then cleared in tetramethylammonium iodide; 3) developed in 3)-19» fixed, bleached in ferric chloride and cupric bromide, then desensitized in pheno safranine. Figure 34 shows the transparency and printout behavior of each modification as a function of time. The above modifications are identified in Figure 34 as 4A, 12A, and 12B respectively. The final transparency of modification 4A holograms was 66%, which was 103% of the initial transparency. Never did this normalized value go below 100% or above Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 65 •p ©.S3 t>0 taO Cfl t 1 60 - P F 3 C © o ® WMU Modification Number 4A h +> 55 © -p PM -H WMU Modification Number 12A S © © 50 WMU Modification Number 12B s § ri Pi O E -t Q /3«tH 45 <5 O 40 12 15 18 Time in Bays 125 r Sk.120 ©.£3 • P JO ®^115 Pi T3 © © Pi -P «T3 £-pi 110 9 E 6) m H §105 CD H g * £ olOO 95 ± JL _L 12 15 18 21 24 27 50 Time in Bays Figure 34. Time Variation of Absolute and Normalized Transparency of Holograms processed with Western Michigan University Modifications 4A, 12A, and 12B Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 91 104%. Shis indicates that processing with this modifi cation produces holograms which have very stable compounds residing in the emulsion. The final transparency of modifications 12A and 12B was 47% and 61% respectively which was 123% and 117% of their initial transparency. This recovery is representative of holograms bleached in cupric bromide and ferric chloride. One may question if this drastic recovery of holographic transparency degrades the image; however, no significant change could be observed visually in the holographic images which were processed in this fashion. Western Michigan University Modifications Humber 12A and 12B will be described as The Derby Process and western Michigan university Modification Humber 4A will be described as The Markham Process in Tables XIV and XY and appendices VI and VII respectively. Table XIV The Essential Processing Steps of The Derby Process Step 1 ...... Develop in Kodak D-19 Step 2 ...... Fix in Kodak Sapid Fixer Step 3 ...... Bleach in Cupric Bromide and Ferric Chloride Step 4 ...... Desensitize in Phenosafranine and/or Clear in Tetramethylammonium Iodide Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. Table XV The Essential Processing Steps of The Markham Process Step 1 ...... Develop in Kodak D-19 and Sodium Thiosulfate Step2...... Ee-expose uniformly to white light Step 3 . . . ..Eedevelop in Kodak D-19 and Sodium Thiosulfate Step 4- ...... Clear in Tetramethylammonium Iodide Step 5 ...... Desensitize in Phenosafranine Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. CONCLUSIONS A process has been developed which produces photo graphic phase holograms of high diffraction efficiency, low noise, and high resistance to printout darkening. The process was developed by combining the best qualities of some of the latest processes reported in the literature. The first innovation was the use of a modified developer which consists of a very small amount of sodium thic- sulfate added to Kodak D-19. This developer slightly etches the undeveloped silver bromide particles in the emulsion making then smaller and as a result they scatter less light giving increased resolution to the holographic image. The second innovation utilizes the concept of reversal bleaching. After the initial development the entire hologram is then re-exposed to uniform white light and after a second development and bleaching of the emul sion only the grains of silver bromide shielded by the metallic silver produced by the first development remain in the emulsion. These remaining grains, called the reversed image, contain all of the information which was recorded on the emulsion prior to the first development. Due to this reversal bleaching process, the scattering of the emulsion has been cut significantly because most of the original silver bromide particles have been proc essed away. The third innovation was the use of tetra- 93 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 94 methylammonium iodide to convert the silver bromide par ticles remaining in the emulsion into silver iodide. Silver iodide resists printout darkening much more than does silver bromide, and tetramethylammonium iodide being a strong electrolyte in solution converts very satis factorily the grains into silver iodide without the etching of these grains which does occur with other processes. The fourth innovation was the use of pheno- safranine to desensitize the emulsion from printout darkening. Phenosafranine is a red dye which is thought to cause the gelatin to absorb short wavelength light. This absorption thus removes the high energy photons which apparently are more active in causing printout. A direct bleach process using cupric bromide and ferric chloride as the bleaching agent, followed by processing in tetramethylammonium iodide and/or pheno safranine, produces holograms which resist printout darkening but have slightly less resolution of the images than the process described previously. The advantage of this process is that it is very simple and only one of two exotic chemicals need be obtained. The process described previously involves many steps including a re—exposure which is somewhat difficult to control. Other methods of trying to improve photographic phase holograms did not produce as good results. Holograms were toned in the hopes that higher diffraction efficien— Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 95 cies could be observed. Holograms were immersed in index of refraction matching liquids in the hopes that lower . optical noise levels could be produced. Holographic film was agitated in an ultrasonic cleaner in the hopes of creating smaller grain sizes in the emulsion and gaining resolution of the holographic images. In all cases the results turned out disappointing. After twenty seven days of constant exposure by an incandescent lamp, holograms situated at different dis tances from the lamp recovered significantly in trans parency after the lamp was found to have burned out between twenty seven and thirty days of constant exposure. This indicated that after exposure to light, holograms recover some of their initial transparency if they are placed in darkness. A further study is suggested to determine the effects of pulsed light of different fre quencies on the printout stability of bleached holograms. Although using the ultrasonic cleaner for improving holographic image quality failed, a Kodak S.A.-3 plate agitated in the device produced slightly darker spectral lines than a plate not agitated. The lines were almost 1.5 times as dark on the red end of the spectrum. A fur ther study is suggested to determine if agitating certain emulsions in an ultrasonic cleaner produces increased sensitivity at certain wavelengths. In the bleached holograms of this investigation, the Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. phenomena of printout and subsequent partial recovery are thought to he related to the solarization processes in ordinary photography. The response of the bleached holo grams to prolonged illumination is characterized by the various experimental curves shown in this paper. These curves all have similar shapes and most display a region of decreasing transparency followed by a region of in creasing transparency, although the different curves show these effects in varying degrees. This transparency decline and partial recovery is represented by the typical curve of figure 35. Percent a Transparency | Time — ^ Figure 35. Time Variation versus Absolute Transparency for a Typical Bleached Hologram The printout region AB illustrates a period of time during which the sustained illumination on the hologram is causing an emulsion darkening. The increased density of the emulsion is thought to be caused by the photolytic generation of atomic metallic silver both within the silver Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 97 halide crystals and on their surfaces. The progressive darkening continues until it "bottoms out (at B) due to a competing re-brominization process. The transparency recovery region BC may be explained by the gradual decrease in the ratio of the printout silver on the halide grain surface compared to printout silver in the grain interior. The halogen is usually liberated at the grain surface where it can unite with the surface silver, while the grain itself (via hole transport mechanism) tends to protect the internal print out silver. The decrease of printout silver from the grain surface and the increase of interior printout silver results in an overall effect of increased transparency of the hologram. The decrease in absorption is related to an effective decrease in the absorbing area of the printout silver. The research of this paper has generated two sig nificant modifications on photographic phase hologram processing. These have been identified in Tables XIV and XV and described in detail in appendices VI and VII as The Derby Process and The Markham Process respectively. These processes are particularly valuable in producing photographic phase holograms with high transparency levels which experience less printout than by any other known method. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. APPENDIX I PROCESSING STEPS FOR THE MODIFIED STANFORD PROCESS 3 Min. 1) Preharden in Kodak Prehardener SH-5 5 Min. 2) Develop in Kodak D-19 15 Sec. 3) Stop Bath 3 Min. 4) Fix in Kodak Rapid Fixer 10 Min. 5) Rinse in Distilled Water 7 Min. 6) Bleach 30 Sec. 7) Rinse in Distilled Water 1 Min. 8) Clear and Desensitize 10 Min. 9) Rinse in Distilled Water 5 Min. 10) Dry in 50% Methanol 3 Min. 11) Dry in 100% Methanol 12) Dry Slowly at Room Temperature BLEACH Ferrous Chloride 25 grams Cuprous Bromide ...... • • 25 grams Concentrated Sulfuric Acid « . • 15 milliliters Distilled Water ...... 500 milliliters C L E A R and DESENSITIZE Solution A Potassium Permanganate • . . • • 5 grams Distilled Water ...... 1 liter Solution B Potassium Bromide • ••...• 50 grams Concentrated Sulfuric Acid • . • 10 milliliters Distilled Water ...... 1 liter ( 1 part of A to 10 parts of B ) 98 permission of the copyright owner. Further reproduction prohibited without permission. APPENDIX II PROCESSING STEPS FOR THE KODAK REVERSAL BLEACH SYSTEM 5 Min. 1) Develop in Kodak Special Developer SD-48 15 Sec. 2) Stop Bath 1 Min. 3) Rinse in Running Water 3 Min. 4) Bleach 5 Min. 5) Rinse in Running Water 1 Min. 6) Stain Remover 1 Min. 7) Clearer 8 Min. 8) Rinse in Running Water 5 Min. 9) Dry in 50% Methanol 10) Wash Twice in Isopropyl Alcohol KODAK SPECIAL DEVELOPER SD-48 Solution A Sodium Sulfite ...... 8 grams Pyrocatechol...... 40 grams Sodium Sulfate 100 grams Distilled Water ...... 1 liter Solution B Sodium H ydro x i d e...... 20 grams Sodium Sulfate ...... 100 grams Distilled Water 1 liter ( 1 part of A to 1 part of B just before using ) BLEACH Potassium Bichromate ...... 9.5 grams Concentrated Sulfuric Acid . . . 12 milliliters Distilled Water ...... 1 liter STAIN REMOVER Potassium Permanganate • • • • • 2.5 grams Concentrated Sulfuric Acid . . . 8 milliliters Distilled Water ...... 1 liter CLEARER Sodium Bisulfite ...... 10 grams Distilled Water ...... 1 liter 99 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. APPENDIX III PEOCESSING STEPS POE THE MODIPIED DEVELOPEE PEOCESS 5 Min. 1) Develop in The Modified Developer 3 Min. 2) Einse in Distilled Water 5 Min. 3) Bleach 6 In. 4) Einse in Distilled Water THE MODI PIED DEVELOPEE Kodak D - 1 9 ...... 1 liter Sodium Thiosulphate 0.5 gram BLEACH Solution A Potassium Dichromate...... 8 grams Concentrated Sulfuric Acid . . . 10 milliliters Distilled W a t e r ...... 1 liter Solution B Potassium Iodide ...... 2 grams Distilled W a t e r ...... 1 liter ( 1 part of A to 1 part of B to 8 parts of distilled water just Before using ) 100 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. APPENDIX IT PROCESSING STEPS POR THE MODI PIED REVERSAL “BLEACH PROCESS 5 Min. 1) Develop in Kodak D-19 90 Sec. 2) Rinse in Distilled Water 3) Re-expose Uniformly to White Light (Approximately 15 sec. to a 15-W bulb at 1 meter for Kodak 649-P plates and approximately .5 sec. to a 25-W bulb at 4 feet for Agfa-Gevaert 103570 film) 5 Min. 4) Redevelop in Kodak D-19 3 Min. 5) Rinse in Distilled Water 12 Min. 6) Bleach 3 Min. 7) Rinse in Distilled Water 5 Min. 8) Clear 9 Min. 9) Rinse in Distilled Water BLEACH Potassium Dichromate...... 0.4 gram Concentrated Sulfuric Acid . . .0.5 milliliter Distilled W a t e r ...... 1 liter CT.TgATTER Tetramethylammonium Iodide . . . 2 grams Distilled Water . • ...... 1 liter 101 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. APPENDIX V PROCESSING STEPS POR THE AGPA PROCESS 5 Min. 1) Develop in Kodak D-19 2 Min. 2) Stop Bath 5 Min. 3) Rinse in Distilled Water 2 Min. 4) Bleach 5 Min. 5) Rinse in Distilled Water 1 Min. 6) Clear 5 Min. 7) Rinse in Distilled Water 10 Min. 8) Desensitize 9) Rinse Briefly in Ethyl Alcohol and Air Dry BLEACH Potassium Bichromate...... 5 grams Concentrated Sulfuric Acid . . . 5 milliliters Distilled W a t e r ...... 1 liter CLEARER Sodium Sulphite ...... 50 grams Sodium Hydroxide 1 gram Distilled Water ...... 1 liter DE SENSITIZER Ethyl Alcohol ...... 88 percent Distilled Water ...... 10 percent Glycerol 2 percent Potassium Bromide.....•• 120 milligrams/liter Phenosafranine...... 200 milligrams/liter 102 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. APPENDIX VI PROCESSING STEPS FOR THE DEEBY PROCESS 5 Min. 1) Develop in Kodak D-19 15 Sec. 2) Stop Bath 3 Min. 3) Fix in Kodak Rapid Fixer 5 Min. 4) Rinse in Distilled Water 7 Min. 5) Bleach 5 Min. 6) Rinse in Distilled Water 5 Min. 7) Clear 5 Min. 8) Rinse in Distilled Water 10 Min. 9) Desensitize 5 Sec. 10) Rinse in Ethyl Alcohol 11) Dry Slowly at Room Temperature BLEACH Ferrous Chloride...... 25 grams Cuprous Bromide ...... 25 grams Concentrated Sulfuric Acid .. . 15 milliliters Distilled Water 500 milliliters CLEARER Tetramethylammonium Iodide . . . 2 grams Distilled W a t e r ...... 1 liter DESENSITIZER Ethyl Alcohol ...... 0.9 liter Distilled W a t e r ...... 0.1 liter Phenosafranine • 200 milligrams ( The process can he modified to delete steps 7 and 8 or step 9 without detrimental effects to the processed holograms ) 103 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. APPENDIX YII PROCESSING STEPS FOR THE MARKHAM PROCESS 5 Min. 1) Develop in The Modified Developer 5 Min. 2) Rinse in Distilled Water 3) Re-expose Uniformly to White Light (Approximately 15 sec. to a 15-W hulh at 1 meter for Kodak 64-9-F plates and approximately .5 sec. to a 25-W bulh at 4 feet for Agfa-Gevaert 10E70 film) 5 Min. 4) Redevelop in The Modified Developer 5 Min. 5) Rinse in Distilled Water 5 Min. 6) Bleach 5 I n . 7) Rinse in Distilled Water 5 Min. 8) Clear 5 Min. 9) Rinse in Distilled Water 10 Min. 10) Desensitize 5 Sec. 11) Rinse in Ethyl Alcohol 12) Dry Slowly at Room Temperature THE MODIFIED DEVELOPER Kodak D - 1 9 ...... 1 liter Sodium T h i o s u l p h a t e 0.5 gram BLEACH Potassium Bichromate...... 8 grams Concentrated Sulfuric Acid . . . 10 milliliters Distilled Water 1 liter CLEARER Tetramethylammonium Iodide . . . 2 grams Distilled Water • 1 liter DESENSITIZER Ethyl Alcohol ...... 0.9 liter Distilled Water 0.1 liter Phenosafranine ...... 200 milligrams 10A Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. APPENDIX VIII INFORMATION ABOUT UNUSUAL CHEMICALS USED IN THIS PAPER Phenosafranine (3,7-diamino-5-phenylphenazinium chloride) M.W. 322.80 3-NH2C6H5N:C6H3-7-KH2:N-5-C6H5Cl Phenosaf ranine is a red dye used mostly for "biological staining 5 Tetramethylammonium Iodide M.W. 201.05 (CH3)4NI Tetramethylammonium is a strong electrolyte in solution oAh U a. ctt3-iN/-cH3 | ______0 ^ 3 ______Pyrocatechol (Catechol), (1,2-benzenediol) M.W. 110.11 CgH^-1,2-(OH)2 Pyrocatechol provides a strong tanning action on photographic gelatin due to its high value of pH. &-OH Xylene (1,2-dimethyl-benzene) or (1,3-dimethy1-benzene) or (1,4-dimethy1-benzene) M.W. 106.17 CgH^(CH3)2 “d :u5027 5°' .ob ob i . « t o (.) X X nD 1.4954 (p) ^ U* Co) C*0 (p)c*-b Xylene is used as a solvent as well as a starter for other organic compounds 105 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 106 APPENDIX YIII (Cont.) Methyl Benzoate (Niobia Oil) M.W. 136.15 (C6H5C02CH5) nD 1.5162 QT Methyl Benzoate is used as a solvent, a starter for other organic compounds, and also used in perfumery Chiorobenzene M.W. 112.56 C6H5C1 nD 1.5236 U* Chlorobenzene is used as a solvent as well as a starter for other organic compounds 1.2—Dibromopropane (propylene dibromide) M.W. 201.90 CH,CHBrCH0Br rt H H ? d t \ l „ nD 1.5190 H-C-C-C-Br H Br « 1.2-Dibromopropane is used as a solvent as well as a starter for other organic compounds 1 .3—Dibromopropane . ^ M.W. 201.90 Br(CH9),Br *1 V i 25 Br-C-C-C-Br n D 1 • 5214 H H H 1.3-Dibromopropane is used as a solvent as well as a starter for other organic compounds Bromoethane (Ethyl Bromide) ^ ^ M.W. 108.97 C^Br «-U-8r nD 1.9236 H-j|. Bromoethane is used as a solvent as well as a starter for other organic compounds . -j, 1 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission.' ' 107 APPENDIX VIII (Cont.) C*3 p-Chlorotoulene M.W. 126.59 CH5C6H4C1 £ 0 nD 1.5150 p-Chlorotoulene is used as a solvent as well as a starter for other organic compounds Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. FOOTNOTES 1. Gabor, D., “A New Microscopic Principle." Nature, CLXI, (19^8), 777-778. 2. Leith, Emmett N., and Upatnieks, Juris, "Wavefront Reconstruction with Diffused Illumination and Three- Dimensional Objects." Journal of the Optical Society of America. LIY, lo. ll'; OTovember, 1'9U), 1295-1301. 3. Cathey, Jr., W.T., "Three-Dimensional Wavefront Recon struction Using a Fhase Hologram." Journal of the Optical Society of America, LV, No. 4, (April, 1965), 55TI 4. Leith and Upatnieks, 9p. cit. 5. Cathey, op. cit. 6. ibid. 7. Colburn, W.S., Zech, R.G. , rjiO Ralston, L.M., "Holo graphic Optical Elements." Government Technical Re port, No. AFAL-TR-72-409, Harris Electro-Optics Cen ter of Radiation, Ann Arbor, Michigan, (November, 1972), 44—61. 8. Shanhoff, T.A., "Phase Holograms in Dichromated Gel atin." Applied Optics, YII, No. 10, (October, 1968), 2101-21U5. 9. Lin, L.H., "Hologram Formation in Hardened Dichroma ted Gelatin Films." Applied Optics, VIII, No. 5, (May, 1969), 963-9667^ 10. Curran, R.K., and Shankoff, T.A., "The Mechanism of Hologram Formation in Dichromated Gelatin." Applied Optics, XI, No. 7, (July, 1970), 1651-1657. 11. Chang, Milton, "Dichromated Gelatin of Improved Opt ical Quality." Applied Optics, X, No. 11, (November, 1971), 2550-2551T 12. Colburn, Zech, and Ralston, op. cit., p. 61-78. 13. Close, D.H., Jacobson, A.D., Margerum, J.D., Brault, R.G., and McClung, F.J., "Hologram Recordings on Photopolymer Materials." Applied Physics Letters, XIV, No. 5, (1971), 2550-o 5T7 14. Jenney, J.A., "Holographic Recording with Photopoly mer." Journal of the Optical Society of America, LX, No. 9, (September, 197& j , n Z Y - T K T . ------15. Wopschall, R.H., "Dry Photopolymer Film for Record ing Holograms." Journal of the Optical Society of America, LXI, No. 5, IMay, 1971), b4-9. 108 Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 109 16. Colburn, W.S., and Haines, X.A., "Volume Hologram Formation in Photopolymer Materials." Applied Optics, X, No. 7, (July, 1971), 1636-1641. 17. Colburn, Zech, and Ralston, op. cit., p. 78-95. 18. Tomlinson, W.J., Kaminow, I.P., Chandross, E.A., Pork, H.L., and Silvast, J., "Photoinduced Refracti ve Index Increase in Poly(Methyl Methacrylate) and its Applications." Applied Physics Letters, XVI, No. 12, (June, 1970), 486-489. 19. Colburn, Zech, and Ralston, op. cit., p. 95-108. 20. Sheridan, N.X., "Production of blazed Holograms." Applied Physics Letters, XII, No. 9, (May, 1968), 316-318. 21. Eartolini, R., Hannan, W., Xarlsons, P., and Lurie, M., "Embossed Hologram Motion Pictures for Televis ion Playback." Applied Optics, IX, No. 10, (October, 1970), 2283-229^7 22. Beesley, M.J., and Castledine, J.G., "The Use of Pho toresist as a Holographic Recording Medium." Applied Optics, IX, No. 12, (December, 1970), 2720-2724. 23 Bartolini, Robert A., "Improved Development for Hol ograms Recorded in Photoresist." Journal of the Opt- ical Society of America, XI, No. 5, (iMay, 1972), 24. Bartolini, Robert A., "Recording of Relief-Phase hol ograms in Photoresist." Journal of the Optical Socie ty of America, LXII, No. 11, ^November, 1972), 1397. 25. Colburn, Zech, and Ralston, op. cit., p. 109-126. 26. Sinclair, Yf.R., Sullivan, M.V., and Pastnacht, R.A., "DC Sputtered Films." Journal of the Electrochemical Society, CXVIII, (1971), 341. 27. Colburn, Zech, and Ralston, op. cit., p. 126-141. 28. Urbach, John C., and Meier, Reinhard W., "Thermoplas tic Xerographic Holography." Applied Optics, V, No. 4, (April, 1966), 666-667. 29. Lin, L.H., and Beauchamp, M.L., "Write-Read-Erase in Situ Optical Memory Using Thermoplastic Holograms." Applied Optics, IX, No. 9, (September, 1970), 2088- 30. Colburn, Zech, and Ralston, op. cit., p. 44-61. 31. loc. cit., p. 61-78. 32. loc. cit., p. 78-95. 33. loc. cit., p. 95-108. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. 34. loc. cit., p. 109-126. 35. loc. cit., p. 126-141. 36. Burekhardt, C.B., “Efficiency of a Dielectric Grat ing. " Journal of the Optical Society of America. LVII, So. 3 7 " ® y 7 l9 6 7 ), 661-603. ------' 37. Latta, John H . , “The Bleaching of Holographic Diffr action Gratings for Maximum Efficiency." Applied Op tics, 711, No. 12, (December, 1968), 2409-24T6'. 38. Upatnieks, Juris, and Leonard, Carl, "Diffraction Efficiency of Bleached Photographically Recorded Interference Patterns." Applied Optics, VIII, No. 1, (January, 1969), 85-89. 39. Cenco Model No. 87288, Central Scientific Company, 2600 South Kostner Avenue, Chicago, Illinois, 60623. 40. Jarrell-Ash Company Scientific Instruments, no. L451.309/57550, Newtonville 60, Massachusetts. 41. Colburn, Zech, and Ralston, op. cit., p. 12-44. 42. Lamberts, R.L., and Kurtz, C.N., “Reversal Bleaching for Low Plare Light in Holograms." Applied Optics, X, No. 6, (June, 1971), 1342-1347. 43. Hariharan, P., Kaushik, G.S., and Ramanathan, C.S., "Simplified, Low Noise Processing Technique for Photographic Phase Holograms." Optics Coanunications VI, No. 1, (September, 1972), 75-76. 44. Hariharan, P., and Ramanathan, C.S., "Supression of Printout Effect in Photographic Phase Holograms." Applied Optics, X, No. 9, (September, 1971), 2197- 45. Processing technique for producing phase holograms, Agfa-Gevaert, Inc., 275 North Street, Teterboro, New Jersey. 46. Lehmann, M., Lauer, J.P., and Goodman, J.W., "High Efficiency, Low Noise, and Suppression of Photochr- omic Effects in Bleached Silver Halide Photography." Applied Optics, IX, No. 8, (August, 1970), 1948-1949 47. loc. cit., p. 1948. 48. Upatnieks, Juris, and Leonard, Carl, "Efficiency and Image Contrast of Dielectric Holograms." Journal of the Optical Society of America, LX, No. 3, (March, 1970), 305. 49. Lehmann, Lauer, and Goodman, op. cit., p. 1948. 50. ibid. Reproduced with permission of the copyright owner. Further reproduction prohibited without permission. I l l 5 1 . McMahon, D.H., and Mai one j, W.F., "Measurements of the Stability of Bleached Photographic Phase Holo grams." Applied Optics, IX, No. 6, (June, 1970), 1363-1365. 52. Colburn, Zech, and Balston, op. cit., p. 12-44. 53. Lamberts and Kurtz, op. cit. 54. , Eastman Organic Chemicals Catalog No. 47, Kodak Publication No. JJ-1, Eastman Kodak Company! Eastman Organic Chemicals, Rochester, New York, 14650, (May 31, 1974), 187. Catalog chemical No. P604, Price: 100 g - S3.90; 500 g - $9.50. 55. Lamberts and Kurtz, op. cit., p. 1347. 56. Agfa-Gevaert, Inc., 275 North Street, Teterboro, New Jersey. 57. , Kodak Plates and Fijjns for Science and Industry, 1st, ea., Kodak Pamphlet No. P-9> Eastman Kodak Company, Rochester, New York, 14650, (1967), 4d, lOd. 58. Hariharan, P., Kaushik, G.S., and Ramanathan, C.S., op. cit. 59. Altman, J.H., "Pure Relief Images on Type 649-F Pla tes." Applied Optics, V, No. 10, (October, 1966), 1689-15901 60. Russo, V., and Sottini, S., "Bleached Holograms." Applied Optics, VII, No. 1, (January, 1968), 202. 61. McMahon, D.H., and Franklin, A.R., "Efficient, High Quality R-10 Bleached Holographic Diffraction Grat ings." Applied Optics. VIII, No. 9, (September, 1969)» 1927-1929. 62. 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No. 12, (December, 1968), 2409-24157^------Lehmann, M. , Lauer, J.P., and Goodman, J.W., "High Effic iency, Low Noise, and Supression of Photochromic Effects in Bleached Silver Halide Photography." Applied Optics. IX, No. 8, (August, 1970), 1948-1949. ------Leith, Emmett N., and Upatnieks, Juris, "Photography by Laser." Scientific American, CCXII, No. 6, (June.'1965). 24-35. Leith, Emmett.N., and Upatnieks, Juris, "’wavefront Recon struction with Diffused Illumination and Three-Dimensional Objects." Journal of the Optical Society of America, LIV. No. 11, (November,' Y964), 1295-1301. Lin, L.H., "Hologram Formation in Hardened Dichromated Gelatin Films." Applied Optics, VIII, No. 5, (May, 1969). 963-966. Lin, L.H., and Beauchamp, M.L., "Write-Eead-Erase in Situ Optical Memory Using Thermoplastic Holograms." Applied Optics, IX, No. 9, (September, 1970), 2088-2092. McMahon, D.H., and Franklin, A.R., "Efficient, High Qual ity R-10 Bleached Holographic Diffraction Gratings." 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Further reproduction prohibited without permission. 117 Periodicals (Cont.): Upatnieks, Juris, and Leonard, Carl, "Diffraction Effic iency of Bleached Photographically Recorded Interference Patterns." Applied Optics. VIII, Ho. 1, (January, 1969), 85-89. Upatnieks, Juris, and Leonard, Carl, "Efficiency and Image Contrast of Dielectric Holograms." Journal of the Optical Society of America, LX, No. 3, (March, 1970), 297-305. Upatnieks, Juris, and Leonard, Carl, "Signal and Noise in Bleached Holograms." Journal of the Optical Society of America, LIX, No. 4, (April, 1969), 481-482. Urhach, John C., and Meier, Reinhard W., "thermoplastic Xerographic Holography." Applied Optics, V, No. 4, (April, 1966), 666-667. Wopschall, R.H., "Dry Photopolymer Film for Recording Holograms." Journal of the Optical Society of America, LXI, No. 5, (May, 1971), 649: ------Young, M . , and KLttridge, F.H., "Amplitude and Phase Hol ograms Exposed on Agfa-Gevaert 10E75 Plates." 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