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Achromatized transmission-type holographic screen for a multiview stereoscopic image system

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The main drawback of the use of transmission-type holographic screens is poor color reproduction caused by their high spectral dispersion. For overcoming this drawback, a long, narrow diffusing slit is used as an object when recording the screen. The necessary size and position of the slit relative to the photoplate and to the recording and reconstruction beams are determined by the phase relations of the beams. By use of the slit, holographic screens of 30 cm × 40 cm are recorded with a diverging reference beam and are used to display a multiview full-color stereoscopic image. The images displayed on the screen show no sign of color separation except near the edges of the screen. The image brightness on the screen is high enough that it can be watched in a normally illuminated room.
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Achromatized transmission-type holographic
screen for a multiview stereoscopic image system
Seon-Ho Hwang, V. I. Bobrinev, Jung-Young Son, S. A. Shestak,
and Hyung-Wook Jeon
The main drawback of the use of transmission-type holographic screens is poor color reproduction caused
by their high spectral dispersion. For overcoming this drawback, a long, narrow diffusing slit is used as
an object when recording the screen. The necessary size and position of the slit relative to the photoplate
and to the recording and reconstruction beams are determined by the phase relations of the beams. By
use of the slit, holographic screens of 30 cm 340 cm are recorded with a diverging reference beam and
are used to display a multiview full-color stereoscopic image. The images displayed on the screen show
no sign of color separation except near the edges of the screen. The image brightness on the screen is
high enough that it can be watched in a normally illuminated room. © 1997 Optical Society of America
Key words: Transmission-type holographic screen, multiview full-color stereoscopic image, optical
diffuser.
1. Introduction
In most stereoscopic imaging systems, binocular dis-
parity is adopted for stereoscopic image generation.
1
In these systems, images representing views from both
the left and the right eye are projected in time sequen-
tially or in parallel, respectively, on the viewing screen,
and viewers see the images through a special plate or
a special pair of glasses. When viewers wear the spe-
cial glasses, the optical properties of the images for
each eye should match those of the glasses to direct
each image to the corresponding eye. There are many
stereoscopic viewing glasses of different types. Color
~red or green!filter, polarization ~horizontal or verti-
cal!, optical density ~high or low!, and time sequential
gating with liquid-crystal-display shutters are exam-
ples of stereoscopic viewing glasses.
2
Stereoscopic viewing plates are a more advanced
form of stereoscopic viewing media that do not re-
quire special glasses for viewing. Lenticulars, par-
allax barriers, microlens arrays, and holographic
screens are examples of such plates. These plates
can be classified into three distinct groups on the
basis of their operating roles: ~1!directing left- and
right-side images that are displayed under them to
the viewer’s corresponding eye, e.g., lenticular and
parallax-barrier plates, ~2!forming three-dimensional
images, e.g., a microlens-array plate, and ~3!directing
and displaying images, e.g., a holographic screen.
Among these plates, the lenticular plate is the most
developed stereoscopic viewing plate at present; how-
ever, its viewing zones and depth are limited.
3
The
parallax-barrier plate has low image brightness,
4
and
the microlens-array plate has so far had no form of
manufacture developed.
3
The holographic screen is a kind of holographic
optical element that can work like a mirror,
5
a lens, a
diffuser, or a lens plus diffuser.
6,7
A holographic
screen with mirror or diffuser properties also has an
image-forming capability. The screen directs lights
from the images projected on it to the viewing zone.
The viewing zone is defined as the images of the exit
pupil of the projection lens formed by the screen, and
the positions of the images relative to the holographic
screen are defined by the beam projection angle to the
screen.
The holographic screen has high light efficiency,
multiview properties, and an easy fabrication process
compared with other types of plates. However, as
S.-H. Hwang is with the Electronics and Telecommunications
Research Institute of Korea, Taejeon 305-350, Korea. When this
study was done V. I. Bobrinev and S. A. Shestak were with the
Research and Development Institute of Radio-optics, 34 Ku-
tuzovsky Prospekt, Moscow 121293, Russia. J.-Y. Son and H.-Y.
Jeon were with the Korean Institute of Science and Technology,
P.O. Box 131, Seoul 130-650, Korea. V. I. Bobrinev and S. A.
Shestak are now with the Korea Institute of Science and Technol-
ogy.
Received 9 April 1997.
0003-6935y97y266605-06$10.00y0
© 1997 Optical Society of America
10 September 1997 yVol. 36, No. 26 yAPPLIED OPTICS 6605
... To do this, it is necessary to apply a mirror coating on the back surface of the photographic plate, with recorded on it hologram, as shown in Figure 6. Previously transmission holograms with a mirror were used to make holographic screen, which can display the stereoscopic images 8,9 . ...
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Objectives: This paper presents several variants of stable optical schemes of sight with Holographic Optical Element to solve a problem of changing direction of diffracted by it. Methods/Statistical Analysis: Optical scheme of holographic sight is presented where the transmission hologram together with mirror is working like the reflection one. Transmission hologram with mirror can be used to stabilize beam position for much bigger wavelength shift, than it is possible with reflection hologram. Findings: Results of calculations show that using of optical systems with a mutually inclined HOE and ADG allows reducing size of scheme with acceptable shift of image. Also it should be noted that the beneficial properties of reflection holograms can be realized using transmission holograms. Application/Improvements: Our results can be useful in devices with Holographic Optical Elements such as display systems and especially for development of holographic sight.
... The screen performs as both the image projection screen and viewing zone forming optics. As the screen, holographic optical elements [10,11], spherical mirror, Fresnel lens, radial and two parallel lenticular plates can be used [2]. The spatial multiplexing method can also be applied to a display panel by dividing the panel into sections with the same size and shape, corresponding to the number of different view images to be displayed [12]. ...
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The current multiview dimensional imaging systems are mostly based on a multiview image set. Depending on the methods of presenting and arranging the image set on a display panel or a screen, the systems are basically classified into contact- and projection-type. The contact-type is further classified into MV(Multiview), IP(Integral Photography), Multiple Image, FLA(Focused light array) and Tracking. The depth cue provided by those types are both binocular and motion parallaxes. The differences between the methods in a same type can only be identified by the composition of images projected to viewer eyes at the viewing regions.
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Three dimensional shifting sensitivity of volume holograms based on random phase encoding using a ground glass has been theoretically analyzed. There are different shifting tolerances in different shifting directions, which include laterally horizontal, laterally vertical, and longitudinal directions. The shifting sensitivity depends on the diameter of the illumination region on the random phase plate, the thickness of the hologram and the distance between them. We apply the theoretical calculation to a degeneracy condition, a point object, and theoretically analyze the shifting tolerance of shifting multiplexing in holographic storage and holographic confocal microscope.
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Holographic screen is an optical element of special kind with the directed light scattering, so that each pixel of the projected image on the screen sends light only in one observers eye (viewing zone). It is possible to record the holographic screen of two types: the reflection type screen and the transmission type one. In this paper the problem of compensation of high spectral dispersion of the transmission type holographic screen is considered. To overcome this problem the diffuse scatterer in the form of narrow long stripe, stretched in the direction to the reference beam axis, has been used. In order to simplify the recording setup, the large size holographic screen has been recorded with the diverging reference beam, because it is possible in this case to use small size optics. Experimentally the transmission type holographic screens have been recorded on the photoplates `Ilford' and PFG-01 (Russia). The screens have been used to display the stereoscopic and multiview color images from the slide-projector. The screen size was 30 X 40 cm. There is possibility to increase the screen size, if it is represented as mosaic of subscreens, each of them being recorded so, to minimize its aberrations.
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A new type of multi-viewing zone screen for multiview 3-D display is described. The screen is made by stacking a Fresnel lens and a reflective prism array plate. The screen performs both focusing and beam dividing functions and directs very narrow light beams to three viewing zones for three spectators. The results of experimental testing of the screen have demonstrated that current technology of Fresnel lens and prism grooves on PMMA(Ploymethyl Methacrylate) allows manufacture of screen having a pixel size of about 1-2 mm. This size is reasonable enough for a screen with dimensions about 1m size. Optical qualities of Fresnel lenses and grooved prism arrays achieve an angular resolution for the screen of several angular minutes.
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Viewing zone shape and size perform a key role in creating viewing comfort for the viewer. The horizontal and vertical sizes of viewing zones, formed by a full color transmission type holographic screen with a stereoscopic image projection are investigated. The screens have been recorded as holograms of a narrow stripe shaped object with different width; to extend the vertical size of the viewing zone the holograms were exposed two times with the hologram shifting between exposures. The viewing zone parameters were measured as a function of the stripe width of the object and of the exit pupil size of projection optics for several holographic screens having the size of the 30 ×\times 40 cm2\textrm{cm}^2 .
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Formulas for angular, lateral, and longitudinal magnification in reconstructed images by holography (imaging by reconstructed wavefronts) are derived and discussed as a function of object–hologram distance, radii of spherical reference and illuminating wavefronts, wavelength ratio of reconstructing to recording radiation, and scale-change factor of the hologram. Expressions for third-order aberrations in the reconstructed wavefronts of point objects are given and conditions are established under which one or more of the aberration coefficients vanish, taking into account an off-axis angle of both reference and illuminating beam.
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Citation REINHARD W. MEIER, "Depth of Focus and Depth of Field in Holography," J. Opt. Soc. Am. 55, 1693_1-1694 (1965) http://www.opticsinfobase.org/josa/abstract.cfm?URI=josa-55-12-1693_1
Conference Paper
The present state of research in the field of the holographic cinematography in the USSR is reviewed. Theoretical foundations of the holographic cine-process are discussed. Research work carried out in the USSR is described. It proves that the use of the holographic cinematography is promising.
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Full-color image display on a holographic screen 30 cm ϫ 40 cm in size
  • Fig
Fig. 6. Full-color image display on a holographic screen 30 cm ϫ 40 cm in size.