U.S. patent application number 13/304891 was filed with the patent office on 2012-08-02 for method and apparatus for recording one-step, full-color, full-parallax, holographic stereograms.
Invention is credited to Alejandro Jose Ferdman, Mark Evan Holzbach, Michael Anthony Klug.
Application Number | 20120194888 13/304891 |
Document ID | / |
Family ID | 43427257 |
Filed Date | 2012-08-02 |
United States Patent
Application |
20120194888 |
Kind Code |
A1 |
Klug; Michael Anthony ; et
al. |
August 2, 2012 |
Method and Apparatus for Recording One-Step, Full-Color,
Full-Parallax, Holographic Stereograms
Abstract
Holographic stereograms and holographic optical elements are
printed using computer rendered images of 3D computer models or
processed images. Printing of one-step, full-color, full-parallax
holographic stereograms uses a reference beam-steering system to
expose a holographic recording material from different angles by a
reference beam. A coherent beam is split into object and reference
beams that interfere with each other at an elemental hologram on a
holographic recording material. A voxel-control lens can be placed
in the path of the object beam and in close proximity to the
holographic recording material to control resolution of a
holographic stereogram. Interchangable band-limited diffusers and
reference-beam masking plates, and viewing zone techniques can be
used in the rendering process.
Inventors: |
Klug; Michael Anthony;
(Austin, TX) ; Holzbach; Mark Evan; (Austin,
TX) ; Ferdman; Alejandro Jose; (Austin, TX) |
Family ID: |
43427257 |
Appl. No.: |
13/304891 |
Filed: |
November 28, 2011 |
Related U.S. Patent Documents
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Application
Number |
Filing Date |
Patent Number |
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12886130 |
Sep 20, 2010 |
8068264 |
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13304891 |
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10014681 |
Dec 11, 2001 |
7813018 |
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12886130 |
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09098581 |
Jun 17, 1998 |
6330088 |
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10014681 |
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60076237 |
Feb 27, 1998 |
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Current U.S.
Class: |
359/23 |
Current CPC
Class: |
G03H 2001/2695 20130101;
G03H 1/24 20130101; G03H 1/26 20130101; G03H 2001/2685 20130101;
G03H 1/20 20130101 |
Class at
Publication: |
359/23 |
International
Class: |
G03H 1/26 20060101
G03H001/26 |
Claims
1. An apparatus for printing holographic stereograms comprising: a
light source that produces a coherent beam: a beam splitter that
splits the coherent beam into an object beam and a reference beam;
a material holder holding a holographic recording material having
elemental holograms; an object beam unit for displaying a rendered
image and for conditioning the object beam with the rendered image
to interfere with the reference beam at a chosen elemental
hologram; a reference beam-steering system for directing the
reference beam to interfere with the object beam at the chosen
elemental hologram; and a computer programmed to control the
interference of the object beam and the reference beam and the
delivery of the rendered image to the object beam unit.
2.-62. (canceled)
Description
[0001] This application claims the benefit of U.S. Provisional
Application No. 60/076,237, filed Feb. 27, 1998.
1. BACKGROUND OF THE INVENTION
[0002] The present invention relates generally to the field of
holography. More particularly, it concerns methods and devices for
creating and printing variable size and variable resolution
holographic stereograms and holographic optical elements using
computer rendered images of three-dimensional computer models or
using computer processed images.
[0003] A holographic stereogram is a type of hologram synthesized
or composed from a set of two-dimensional views of a subject. A
holographic stereogram is capable of creating the convincing
illusion of a solid three-dimensional subject from closely spaced,
discrete-perspective, two-dimensional component views. In addition,
if the two-dimensional component views are properly generated, a
holographic stereogram can also create the illusion of an animated
image. Although holographic stereograms can project such special
effects, due to limitations in the methods and techniques for
printing holographic stereograms, holographic stereograms have
generally been expensive, difficult, and time consuming to
produce.
[0004] Techniques have been developed for reducing the number of
steps involved in producing holographic stereograms to one optical
printing step. One-step technology usually involves using computer
processed images of objects or computer models of objects to build
a hologram from a number of contiguous, small, elemental pieces,
known as elemental holograms or hogels. This one-step technology
eliminates the need to create a preliminary hologram.
[0005] To produce a full-parallax, holographic stereogram using
traditional one-step technology, a three-dimensional computer model
of an object or a scene is created. There are numerous computer
graphic modeling programs, rendering programs, animation programs,
three dimensional digitalization systems, or combinations of the
programs or systems that can be used to generate and manipulate a
three-dimensional computer model of an object or a scene. Examples
of such programs or systems include, but are not limited to
computer-aided-design (CAD) programs, scientific visualization
programs, and virtual reality programs.
[0006] In addition, to produce a holographic stereogram using
one-step technology requires that the position of the hologram
surface and individual elemental holograms relative to an object or
a scene be determined. Furthermore, a proper computer graphic
camera(s)'s description for an elemental hologram and the size and
location of a spatial light modulator (SLM), a device that can
display a two-dimensional image, need to be determined.
[0007] Once all the aforementioned initial parameters are
determined, a two-dimensional projection on the SLM for each
elemental hologram is computed based on the computer graphic model
of the object or scene that was created, the positions of the
elemental holograms, and the computer graphic camera's description
for the elemental holograms. The two-dimensional projection on the
SLM for each elemental hologram may be rendered using various
computer graphic techniques. The process of creating
two-dimensional views from a three-dimensional object and adding
qualities such as variations in color and shade to a computer
graphic model is often referred to as rendering. There are numerous
methods for rendering. One method is ray-tracing, which computes
images by accurately simulating sampled light rays in a computer
model. Another method is scan-line conversion, which computes
images one raster or line at a time. Typically scan-line rendering
does not produce as realistic results as ray tracing. However,
scan-line rendering is frequently used in animation packages
because it is faster. Another method for using computer graphics to
render images for one-step, full-parallax holographic stereograms
is described in an article by Halle and Kropp. Halle, M. and Kropp,
A., "Fast Computer Graphics Rendering for Full Parallax Spatial
Displays," Proc. Soc. Photo-Opt. Instrum. Eng. (SPIE), 3011:105-112
(Feb. 10-11, 1997), the disclosure of which is incorporated herein
by reference.
[0008] When holographic stereograms are produced by either the
multi-step or one-step techniques, the reconstructed images may
have geometric image distortions. These geometric image distortions
may be very apparent, especially in large, billboard size
holographic displays or holographic displays in other geometries,
such as an alcove or a partial cylinder.
[0009] One solution that has been incorporated into multi-step
techniques to correct for geometric image distortions for multiplex
holograms is discussed in an article by Okada. Okada, K., et. al.,
"A Method of Distortion Compensation of Multiplex Holograms,"
Optics Communications, vol. 48, no. 3, pp. 167-170 (Dec. 1, 1983),
the disclosure of which is incorporated herein by reference. The
technique discussed in Okada's article to correct distortion is a
method to correct geometrical and time distortion of a single or
monocular viewpoint of a finished hologram. Because it is a
post-processing method that takes place after image acquisition,
Okada's technique would be inefficient if adopted to generate
animated computer graphics for one-step, holographic stereograms.
Moreover, Okada's method only produces horizontal-parallax-only
transmission type holograms.
[0010] Others have developed techniques for pre-distorting
one-step, holographic stereograms to reduce distortion in the final
holographic display. One such pre-distortion technique is described
in a paper by Halle and others. Halle, M. et al, "The Ultragram: A
Generalized Holographic Stereogram," Proc. Soc. Photo-Opt. Instrum.
Eng. (SPIE), vol. 1461, Practical Holography V, p. 142 (February
1991), the disclosure of which is incorporated herein by reference.
Although widely used, typical pre-distortion techniques for
one-step methods for producing full-parallax, holographic
stereograms are significantly limited by available computer
processing speeds and the resolution of images produced by
traditional one-step methods. In addition, techniques for
pre-distorting one-step, full-parallax, holographic stereograms
have not been able to produce comprehensible, animated, one-step,
full-parallax, holographic stereograms.
[0011] Apparatus for printing one-step, monochromatic,
holographic-stereograms have been developed. Typically, such prior
art printers, as depicted in FIG. 1, include: a monochrome coherent
light source 1, lenses 42, mirrors 40, an optical system 89, a
shutter 10, a mechanism for translating film 69, holographic
recording material 70, usually in the form of film, a personal
computer 85 to control the timing for the exposure sequence, and a
separate high-speed computer 87 for image calculations. The prior
art printer depicted in FIG. 1, was discussed in two articles by
Yamaguchi. Yamaguchi, M. et al., "Development of a Prototype
Full-Parallax Holoprinter." Proc. Soc. Photo-Opt. Instrum. Eng.
(SPIE), vol. 2406, Practical Holography IX, pp. 50-56 (February
1995); and Yamaguchi, M., et al., "High-Quality Recording of a
Full-Parallax Holographic Stereogram with a Digital Diffuser,"
Optics Letters, vol. 19, no. 2, pp. 135-137 (Jan. 20, 1994), the
disclosures of each are incorporated herein by reference. The prior
art printer depicted in FIG. 1 is capable of producing
monochromatic holographic stereograms, but not full-color
holographic stereograms.
[0012] A typical prior art hologram printer, like the one depicted
in FIG. 1, usually is supported by a vibration isolation table 80.
In addition, the prior art printer depicted by FIG. 1 uses a HeNe
laser for a light source 1 that produces a coherent light beam 5
that may be collimated. A shutter 10 is placed at the output of
light source 1. A beam-splitter 15 splits the light 5 from the
light source 1 into an object beam 20 and a reference beam 25. The
polarization of the object and reference beams 20, 25 are adjusted
by a pair of half-wave plates 30 and a pair of polarizers 35. The
half-wave plates 30 and polarizers 35 also control the ratio of the
beams. The prior art printer also uses a number of mirrors 40. In
addition, the prior art printer uses a system of enlarging lenses
42 to distribute the object beam 20 from the light source 1 into
the optical system 89 depicted in FIG. 1.
[0013] The optical system 89 of the prior art printer of FIG. 1
includes a band-limited diffuser 45, a liquid crystal display panel
(LCD panel) 50, and a converging lens 55. A band-limited diffuser
is a diffuser with a deterministic phase pattern designed to
diffuse light in a specific pattern or direction. The band-limited
diffuser 45 depicted in FIG. 1 is specifically designed for the
monochromatic light source being used--a HeNe laser. The LCD panel
50 used in the prior art printer of FIG. 1 is a gray scale,
electrically addressed panel with twisted-nematic liquid crystals.
The LCD panel 50 receives image data calculated by a high-speed
computer 87 by an analog video signal. The converging lens 55 shown
in FIG. 1 focuses the images from the LCD panel 50 to the
holographic recording material 70. The converging lens 55 generally
has a low f-number in order to produce a wide angle of view. Due to
the need to correct for spherical aberrations along the optical
axis, Yamaguchi utilized a converging lens 55 composed of three
lenses to reduce spherical aberration and realize a f-number of
around 0.8.
[0014] To prevent the exposure of parts of the holographic
recording material 70 that are not part of the elemental hologram
110 meant to be exposed, the prior art printer of FIG. 1, uses, in
close proximity to the holographic recording material 70, an object
beam masking plate 60 with an aperture the size of the elemental
hologram 110 to prevent the object beam 20 from exposing other
parts of the holographic recording material 70.
[0015] The band-limited diffuser 45 shown in FIG. 1 improves the
uniformity of the distribution of the object beam 20 over an
elemental hologram on the holographic recording material 70. If the
band-limited diffuser 45 is designed such that an object beam 20 is
focused only over the area of an elemental hologram, then an object
beam masking plate 60 is not needed to prevent exposure of areas
outside the elemental hologram. However, if used with such a
band-limited diffuser, the object beam masking plate 60 may have an
aperture larger than the size of the elemental hologram 110. An
object beam 20 and a band-limited diffuser 45 that allow even
illumination of an elemental hologram 110 by an object beam 20 need
to be matched by a reference beam masking plate 65 with an aperture
the size of the elemental hologram 110. Because the required
matching of a object beam 20, a band-limited diffuser 45, and
reference beam masking plate 65 to the size of a desired elemental
hologram, it has been difficult to change the sizes of elemental
holograms exposed by a hologram printer. Because of this lack of
flexibility, prior art printers cannot easily print holograms
having different sizes of elemental holograms, and are restricted
to printing holograms with single, fixed-sized elemental
holograms.
[0016] FIGS. 2-4 illustrate alternative prior art embodiments of
optical systems that function in the same way as the optical system
89 depicted in FIG. 1.
[0017] In FIGS. 2-4, an object beam 20 is directed through a SLM 90
that has a sample image point 100 on its surface. The object beam
20 may be normal to the SLM surface or off-axis from the normal.
SLM 90 may also have an array of pixels 95. LCD panels,
cinematography film, and transparencies have been used as SLMs
90.
[0018] In FIG. 2, the object beam is directed through a simple
diffuser 105, such as a section of ground glass, that scatters
light. When a simple diffuser 105 is used, then an object beam
masking plate 60 must be used to prevent exposing areas of the
holographic recording material 70 outside of the elemental hologram
110 that are not meant to be exposed.
[0019] In FIG. 3, an object beam 20 is directed through a
holographic optical element (HOE) 115. A HOE is a hologram that is
specially designed to redirect light emanating from a source in a
certain way. For instance, a HOE may be designed to act as a lens
to converge light to a single point. As another example, a HOE may
be designed to act as a band-limited diffuser that is paired with a
lens to converge light over an area rather than at a single point.
The HOE 115 depicted in FIG. 3 is one that is designed to evenly
expose an area the size and shape of an elemental hologram 110.
When such a HOE is used, an object beam masking plate 60 (shown in
FIG. 2) need not be used at all or, if used, may have an aperture
larger than the size of the elemental hologram 110 to be
exposed.
[0020] In FIG. 4, an object beam 20 is directed through a
band-limited diffuser, which may be a band-limited digital
diffuser, 45 and a converging lens 55. The band-limited diffuser 45
depicted in FIG. 4 is designed to converge the object beam 20, over
the area of elemental hologram 110. Thus, an object beam masking
plate 60 (shown in FIG. 2) need not be used at all or, if used may
have an aperture larger than the size of the elemental hologram 110
to be exposed.
[0021] In FIGS. 2-4, the sample image point 100 is an image point
of the SLM 90 that is recorded in an elemental hologram 110 on a
holographic recording material 70. Reference beam 25 is directed at
the elemental hologram 110 such that the interference pattern
formed by the interaction of the object beam 20 and the reference
beam 25 may be recorded on the elemental hologram 110 on the
holographic recording material 70.
[0022] To expose a two-dimensional array of elemental holograms,
the prior art printer of FIG. 1 uses a mechanism for translating
holographic film 69 that includes pulse controlled motors 71.
Typically, the holographic recording material 70 in a prior art
printer is photographic film. The film is held between the object
beam masking plate 60 and the reference beam masking plate 65. Both
masking plates 60 and 65 have apertures that are the size of the
elemental holograms 110 being exposed. The masking plates 60 and 65
are moved by a solenoid 72. Pulse controlled motors 71 translate
the film in two directions.
[0023] In the prior art system depicted in FIG. 1, the timing of
the exposure sequence is controlled by a personal computer. Thus,
the solenoid 72, as well as the pulse controlled motors 71 and the
shutter 10, are controlled by the personal computer 85. In
contrast, the images for the exposures are calculated off-line by a
high-speed computer 87. The image calculations are transferred by
an analog video signal to the LCD panel 50.
[0024] For a holographic stereogram to be reconstructed, an
illumination source must be placed at an appropriate angle. If the
illumination source is not placed correctly, a holographic
stereogram will not be reconstructed or will appear with
distortions, such as magnification distortions. Despite advances in
holographic techniques and equipment, the display illumination
geometry of a one-step, holographic stereogram remains a problem.
The display illumination geometry, i.e., the placement of an
illumination source with respect to a holographic stereogram,
depends on the cumulative effect of the angles at which a reference
beam exposed each of a holographic stereogram's elemental
holograms. For example, if the angle at which all of the elemental
holograms on a holographic stereogram are exposed to a collimated
reference beam is constant, and if the surface of the holographic
stereogram is flat, then the holographic stereogram needs a
collimated illumination source to illuminate each of the elemental
holograms from the appropriate angle if the hologram is to be
properly reconstructed without defects such as magnification
distortion.
[0025] Furthermore, in practice, it has been common to create
reflection holographic stereograms which are meant to be
illuminated with a diverging light source such as a point source.
However, the prior art has not overcome the difficulty in designing
a printer in which the angle of a reference beam is automatically
and flexibly changeable to allow reconstruction by a point source
and with minimal distortion.
[0026] In addition, it remains difficult to control the resolution
or elemental hologram density of a holographic image. The sharpness
of a holographic image depends on the image resolution and the
extent of any blurring. Blurring can be caused by having a large
illumination source, such as that of a long florescent light,
illuminate a hologram. In addition, blurring can be caused by the
large spectral spread of an illumination source. If an illumination
source that is small and monochromatic, such as a laser source
expanded through a microscope objective lens (i.e. a small,
inexpensive, achromatic, high-power lens), is used, blurring may be
minimized, and the sharpness of the holographic image will mainly
depend on the image resolution of the hologram.
[0027] The image resolution of a three-dimensional image is defined
as the volumetric density of individually distinguishable image
points in an image volume. For one-step, holographic stereograms,
including full-parallax and horizontal-parallax holograms, this
resolution is usually not constant throughout an image volume. For
small images of little depth, the variation of image resolution
with depth is hardly noticeable. However, for holographic
stereograms with significant depth, the variation in image
resolution with depth can be very apparent.
[0028] As shown in FIG. 5, if the light from an illumination source
130 that is the same type of light source as that which generated
the reference beam 25 that exposed an elemental hologram 110
illuminates the elemental hologram 110 from the appropriate
conjugate angle, the reconstruction 125 of the sample image point
100, (shown in FIGS. 2-4), on the reconstruction 120 of the image
of the SLM is formed at the same apparent distance and position
relative to the elemental hologram 110 as it appeared to the
elemental hologram 110 at the time of recording.
[0029] FIG. 6 shows lines drawn from the boundaries between
neighboring elemental holograms 110 on a holographic recording
material 70 through the boundaries between neighboring
reconstructed pixels 135 of the reconstructed image 120 of a SLM.
The areas bounded between the lines drawn from the boundaries of at
least two elemental holograms represent independently addressable
volume elements, or voxels 140. A voxel 140 is a component unit
which represents an arbitrary three-dimensional object or scene.
Assuming that the elemental holograms 110 are larger than the SLM
pixels, as shown in FIG. 6, the sizes of the voxels 140 increase
with increasing distance from the surface of a reconstructed image
of a SLM 120. If the sizes of the voxels 140 are too coarse
relative to the desired detail size of a three-dimensional object
or scene, the reproduced image will be poor or indiscernible. If
the three-dimensional image of an object or scene extends over a
wide range of depth, a variation in the sizes of the voxels will
also be very undesirable because such a variation would lead to
poor image quality.
[0030] Thus, hologram printers of the prior art have limitations
that make them impractical for commercial purposes. In particular,
these prior art printers suffer from: lack of ability to print
full-color holographic stereograms; lack of ability to
simultaneously expose multiple elemental holograms; lack of
flexibility to quickly and easily adjust a hologram printer to
print at different elemental hologram sizes; lack of flexibility to
easily change the angle of a reference beam to a holographic
recording material; lack of ability to control the resolution of a
hologram; and lack of ability to create computer generated images
which display animation or different images with a change of
viewing position.
SUMMARY OF THE INVENTION
[0031] The present invention overcomes many of the above-noted
limitations and problems of prior art hologram printers and methods
used to print holographic stereograms with the following structures
and methods.
[0032] The present invention is an apparatus and method for
printing one-step, full-color, full-parallax holographic
stereograms utilizing a reference beam-steering system that allows
a reference beam to expose a holographic recording material from
different angles. More particularly, a coherent beam is split into
object and reference beams. The object beam passes through an
object beam unit in which a rendered image is displayed, while the
reference beam passes through the reference beam-steering system.
The object and reference beams interfere with each other at an
elemental hologram on a holographic recording material. A computer
controls the exposure time and the movement of the recording
material and may also render the images displayed in the object
beam unit. In addition, the computer may also store the images
before they are displayed in the object beam unit.
[0033] In addition, the present invention may also utilize a
voxel-control lens placed in the path of the object beam and in
close proximity to the holographic recording material to control
the resolution of a holographic stereogram.
[0034] In addition, the present invention may also utilize
interchangable band-limited diffusers and reference-beam masking
plates.
[0035] Furthermore, the present invention incorporates viewing zone
techniques to the rendering process for one-step, holographic
stereograms to produce animated, one-step, holographic
stereograms.
[0036] In accordance with long-standing patent law convention, the
words "a" and "an" when used in this application, including the
claims, denotes "at least one."
BRIEF DESCRIPTION OF THE DRAWINGS
[0037] The following drawings form part of the specification and
are included to further demonstrate certain aspects of the present
invention. The invention may be better understood by reference to
one or more of these drawings in combination with the detailed
description of specific embodiments presented herein.
[0038] FIGS. 1(a) and (b) are schematic, top-view drawings of a
prior art hologram printer.
[0039] FIGS. 2(a) and (b) are simplified, top-view illustrations of
a one-step, reflection, elemental hologram recording using an
optical system including a simple diffuser.
[0040] FIG. 3 is a simplified, top-view illustration of a one-step,
reflection, elemental hologram recording using an optical system
including a holographic optical element.
[0041] FIG. 4 is a simplified, top-view illustration of a one-step,
reflection, elemental hologram recording using an optical system
including a band-limited diffuser and a converging lens.
[0042] FIG. 5 is a simplified, top-view illustration of the
reconstruction of an elemental hologram of a holographic
stereogram.
[0043] FIG. 6 is an illustration of the changes in sizes of voxels
with distance from a reconstructed image of a SLM.
[0044] FIG. 7 is a top-view, schematic drawing of one embodiment of
the present invention for a one-step, full-color, full-parallax
printer for holographic stereograms.
[0045] FIG. 8 is a top-view, schematic drawing of another
embodiment of the present invention for a one-step, full-color,
full-parallax printer for holographic stereograms.
[0046] FIG. 9 is an illustration of a particular embodiment of the
present invention to control the variation in sizes of voxels.
[0047] FIGS. 10(a) and (b) illustrate how the apparent distance of
a SLM, as seen by an elemental hologram, may change when a
voxel-control lens is utilized.
[0048] FIG. 11 is an illustration of voxel boundary lines that are
approximately parallel to each other.
[0049] FIG. 12 is a schematic illustration of an embodiment of the
reference beam-steering system of the present invention.
[0050] FIG. 13 is a schematic illustration of another embodiment of
the reference beam-steering system of the present invention.
[0051] FIG. 14 is a schematic illustration of an embodiment of the
reference beam-steering system of the present invention that
utilizes a beam-steering aperture.
[0052] FIG. 15 is an orthogonal-view illustration of an embodiment
of the beam-steering mirror system of the present invention.
[0053] FIG. 16 is a front-view illustration of another embodiment
of the beam-steering mirror system of the present invention.
[0054] FIG. 17 is a schematic illustration of an embodiment of the
reference beam-steering system of the present invention that
utilizes fiber optics and a translation system.
[0055] FIG. 18 is a simplified, orthogonal-view illustration of an
embodiment of the reference beam-steering system of the present
invention that utilizes fiber optics and a translation system.
[0056] FIG. 19 is a simplified, orthogonal-view illustration of an
embodiment of a reference beam-steering system of the present
invention that utilizes fiber optics, a translation system, and a
optical combiner unit.
[0057] FIG. 20 is a schematic illustration of an object beam unit
of the present invention that utilizes fiber optics.
[0058] FIG. 21 is a top-view, schematic drawing of one embodiment,
which utilizes fiber optics, of the present invention for a
one-step, full-color, full-parallax printer for holographic
stereograms.
[0059] FIG. 22 is a simplified, orthogonal-view illustration of an
embodiment of a material holder of the present invention.
[0060] FIG. 23 is a schematic illustration of an embodiment of the
present invention with fixed object beam units and fixed reference
beam-steering systems.
[0061] FIG. 24 is a schematic illustration of an embodiment of the
present invention with mobile object beam units and mobile
reference beam-steering systems.
[0062] FIG. 25 is a schematic illustration of another embodiment of
the present invention with mobile object beam units and mobile
reference beam-steering systems.
[0063] FIG. 26 is a schematic illustration of yet another
embodiment of the present invention with mobile object beam units
and mobile reference beam-steering systems.
[0064] FIGS. 27(a), (b), and (c) are orthogonal-view illustrations
of removable band-limited diffusers and removable reference beam
masking plates.
[0065] FIG. 28 is a flow chart illustrating the steps for creating
an animated, one-step, full-parallax holographic stereogram.
[0066] FIG. 29 is an illustration of viewing zones for a
holographic stereogram that displays different images when viewed
from different viewing zones.
[0067] FIG. 30 is an illustration of rays projecting from the
perimeter of viewing zones.
[0068] FIG. 31 is an illustration of viewing zone mask volumes.
DESCRIPTION OF ILLUSTRATIVE EMBODIMENTS
[0069] The following examples are included to demonstrate
illustrative embodiments of the present invention. It should be
appreciated by those with skill in the art that the techniques
disclosed in the following examples represent techniques discovered
by the inventors to function well in practice and thus can be
considered to constitute exemplary modes for its practice. However,
those with skill in the art will, in light of the present
disclosure, appreciate that many changes can be made in the
specific embodiments which are disclosed and still obtain a like or
similar result without departing from the spirit and scope of the
invention. For instance, a HOE or other appropriate optics may
replace the combination of a lens and a band-limited diffuser. In
addition, a HOE may also replace a lens or a combination of lenses.
Furthermore, SLMs may include, but are not limited to LCD panels,
digital micro-mirror arrays, film, or transparencies. In addition,
computer storage devices may include, but are not limited to hard
disks, static or dynamic RAM, flash memory, DVD drives, or tape
drives. Moreover, motors may include, but are not limited to DC
servo motors, stepper motors, or actuators.
[0070] The present invention provides a system and method for
printing one-step, full-color, full-parallax holographic
stereograms. Some presently illustrated embodiments are depicted in
FIGS. 7-31.
[0071] One embodiment of the present invention for a printer is
illustrated in FIG. 7. As depicted in FIG. 7, most of the parts of
the printer, except for a computer 230 and controllers 305 and 455,
are isolated from vibrations by, for example, being supported on
vibration isolation table 80. The table 80 may be composed of steel
with a honeycomb interior. The legs of the table 80 may be air
pistons which can absorb vibrations. Other types of vibration
isolation may also be acceptable. In some embodiments, the computer
230 and controllers 305 and 455 may be supported on table 80. The
computer 230 may have multiple ports and serial or parallel cables
through which the computer 230 can control devices, like motor
controllers, or through which the computer 230 can send output,
such as images. In addition, computer 230 may have computational
power and speed sufficient for three-dimensional computer graphics.
Furthermore, computer 230 may include one or more central
processing unit and may include one or more storage devices, for
example, hard disks, a redundant array of independent disks, FLASH
memory, or static or dynamic RAM, in which rendered images are
stored. If more than one central processing unit is used, they may
operate independently or in parallel. If more than one storage
device is used, they may also operate independently or in parallel.
In some embodiments, lasers 200 are not supported by table 80. The
lasers 200 may be lasers of three different colors. For example,
one laser 200 may be a krypton ion or a HeNe laser to produce a red
beam of light, another laser 200 may be an argon ion or a YAG laser
to produce a green beam of light, and a third laser 200 may be an
argon ion or a HeCd laser to produce a blue beam of light. Other
light wavelengths are also acceptable. In addition, lasers 200 may
be solid state diodes or other types of lasers. The beams of light
from the lasers 200 may go through open air. In addition, the beams
of light from the lasers 200 may go through pipes so that
instabilities due to air currents will be reduced. Also, the beams
may be transmitted through polarization-preserving optical
fibers.
[0072] In FIG. 7, the coherent light beams 5 produced by the lasers
200 are directed at variable beam splitters 205. Variable beam
splitters are half-mirrors that split a beam by reflecting part of
the beam and transmitting most of the rest of the beam. If fiber
optics are used to transmit beams, then fiber optic beam splitters
that work by contacting two parallel fibers together and letting
the light from the fibers couple may be used. The coherent light
beam 5 from each of the lasers 200 is split into two beams, an
object beam 20 and a reference beam 25. In some embodiments, each
object beam 20 and each reference beam 25 may be directed through
half-wave plates 30 and polarizers 35. In other embodiments, if
polarization-retaining fiber optic cables are used to transmit a
beam and if the cables are rotatable about their center axes,
half-wave plates 30 need not be used. If needed, each object beam
may be reflected off one or more mirror 40. The mirrors 40 of the
present invention may be, for example, first surface or front
surface mirrors. Each object beam 20 may be directed through a low
pass spatial filter 220 to remove unwanted noise. A low pass
spatial filter 220 may include a microscope objective lens and a
pinhole. Each object beam 20 may then pass through a beam shutter
225. In one embodiment, the beam shutters 225 may be high-speed,
mechanical iris shutters, for example, those used in made the
photography industry. In other embodiments, the beam shutters 225
may be electro-optical systems such as liquid crystal cells or
acousto-optical modulator crystals. In another embodiment, instead
of using separate beam shutters 225, the SLM 90 in the object beam
unit, generally 700, can function as a shutter for all three object
beams. The shutters 225 are controlled by the computer 230. The
object beams 20 may be then directed through an object beam unit
700. In the object beam unit 700, the object beams 20 may be
directed such that the object beams 20 converge at the plane of a
SLM 90. SLM 90 may include, but is not limited to, a transmissive
LCD panel, a reflective LCD panel, an optically addressed LCD
panel, a digital micro-mirror array, film, a projection or a
transparency. The SLM 90 may receive image input by a video cable
from the computer 230. In addition, multiple SLMs may receive
images generated in parallel by multiple central processing units.
Moreover, multiple SLMs may receive images from the storage device
or devices of computer 230. After passing through the SLM 90, the
object beam 20 may pass through a HOE 115, or another system, like
those illustrated in FIGS. 2-4, that is designed to converge the
object beam and evenly expose an area the size of an elemental
hologram. In one implementation, the HOE 115 may be a
transmission-type hologram that can converge three different
monochromatic object beams at slightly different angles onto the
elemental holograms to be exposed without allowing zeroth-ordered
light from any of the object beams to intersect the elemental
holograms to be exposed. After passing through the object beam unit
700, the object beam 20 may then be transmitted through a voxel
control lens 500 and may then expose an elemental hologram 110 on a
holographic recording material 70 in a material holder 300. The
holographic recording material 70 may be, but is not limited to, a
pan-chromatic photopolymer, a pan-chromatic or monochromatic silver
halide photographic emulsion, dichromated gelatin, or other
suitable photopolymers. The holographic recording material 70 may
be held securely by a material holder 300 that may be able to
translate the holographic recording material in two directions. The
movement of the material holder 300 may be controlled by film
holder motor controller 305 which may be controlled by computer
230.
[0073] As further depicted in FIG. 7, after the beams are split
into object beams 20 and reference beams 25 by the variable beam
splitters 205, each of the reference beams 25 passes through a
variable attenuator 210 which allows the intensity of each
reference beam 25 to be independently adjusted. The reference beams
may be reflected off of a mirror 40 before passing through dichroic
combiners 215 or other suitable optical combiners. A dichroic
combiner is a wavelength selective mirror which reflects some
wavelengths, but is transparent to other wavelengths. The dichroic
combiners 215 in FIG. 7 combine the three reference beams 25 into
one beam which may then pass through a beam shutter 225 before
passing through a low pass spatial filter 220. The reference beam
25 then passes through a reference beam steering system 400 which
controls the angle which the reference beam 25 intersects with the
holographic recording material 70. A beam-steering mirror system of
the reference beam-steering system is controlled by a mirror system
motor controller 455 that is controlled by computer 230.
[0074] Furthermore, the present invention allows separate elemental
holograms to be printed in different colors. For instance, by
placing a beam shutter in the path of each object beam and
reference beam and then selectively closing the beam shutters, one
elemental hologram may be exposed to only red object and reference
beams, another may be exposed to only green object and reference
beams, and another may be exposed to only blue object and reference
beams.
[0075] An embodiment of the present invention in which multiple
elemental holograms are simultaneously exposed is depicted in FIG.
8. The beams from lasers 200 are split by variable beam splitters
205 and then after being reflected by mirrors 40 are split again by
additional variable beam splitters 205, thereby forming two or more
object beams 20 and two or more reference beams 25 from each laser
200. In other embodiments, the beams from lasers 200 may be split
even more times to form more object beams 20 and more reference
beams 25. Each object beam 20 passes through a low pass filter 220
and a beam shutter 225. Each set of three object beams 20 may be
reflected by mirrors 40 and pass through a SLM 90, a HOE 115, and a
voxel control lens 500 to expose an elemental hologram 110 on a
holographic recording material 70 held by a material holder 300.
The movement of the material holder 300 is controlled by film
holder motor controllers that are controlled by computer 230. Each
set of three reference beams 25 passes through variable attenuators
210 and are combined into a beam by a dichroic combiner 215 or
other suitable optical combiners. Each of the resulting two
reference beams 25 passes through a beam shutter 225 and a low pass
spatial filter 220. Each reference beam 25 then passes through a
beam-steering system 400 before hitting an elemental hologram 110.
Thus, as depicted in FIG. 8, multiple elemental holograms may be
simultaneously printed.
[0076] An embodiment of the present invention in which the
variation in voxel size is controlled is illustrated by FIGS. 9 and
10. As shown in FIGS. 9 and 10, this control is accomplished by
placing a voxel-control lens 500 in the path of an object beam 20
between SLM 90 and holographic recording material 70. The
voxel-control lens 500 may be placed in close proximity to
holographic recording material 70. The voxel-control lens 500 may
be capable of making an SLM or a projected image of a SLM seen from
the viewpoint of an elemental hologram 110 appear at a greater
apparent distance relative to the holographic recording material 70
during recording, so that a sample image point 100 on the SLM 90
surface is reconstructed at a greater distance away from the
holographic recording material 70. FIG. 10(a) illustrates how an
image 505 of a SLM may appear to an elemental hologram 110 in a
printer without a voxel-control lens. FIG. 10(b) illustrates how an
image 505 of a SLM may appear to an elemental hologram in a printer
with a voxel-control lens 500. As shown in FIG. 10, the voxel
control lens magnifies the image 505 of a SLM, such that the angle
.alpha. subtended by the image does not change but the angle .phi.
subtended by an elemental hologram decreases to .theta. when a
voxel control lens is used. The distance between the image 505 of a
SLM and the holographic recording material 70 may be varied by
varying the focal length of the voxel-control lens 500 or its
position between the holographic recording surface 70 and the
converging lens 55 or other optical systems, including simple
diffusers or HOEs, as shown in FIGS. 1-3, used in the prior art to
converge light onto the holographic recording material 70. In some
embodiments, the voxel control lens 500 may be part of the object
beam unit 700.
[0077] In one particular embodiment of this invention, it is
possible to make the voxel sizes fairly constant over a wide range
of distances from a holographic recording material 70. This is
accomplished by choosing a voxel-control lens 500 with a focal
length equal to the distance between the voxel-control lens 500 and
the actual location of the SLM or the location of a projected image
of the SLM as seen by an elemental hologram in a printer without a
voxel-control lens. Such a voxel-control lens 500 and geometrical
layout will effectively reconstruct the SLM 120 at an infinite
distance relative to holographic recording material 70. If the size
of the pixels 95 on a SLM 90 are small compared to the size of the
elemental holograms 110, the voxel 140 boundary lines for such an
embodiment will no longer intersect close to the holographic
recording material 70 as depicted in FIG. 6, but instead become
approximately parallel lines which extend out to a great distance
without intersecting as shown in FIG. 11.
[0078] Although the characteristics of a voxel-control lens 500 may
depend on the desired results, typically it is desirable for the
voxel-control lens 500 to be achromatic and have an f-number of
around 3.0 or lower. In one particular embodiment, the
voxel-control lens may be achromatic and have an f-number of 2.4.
In other embodiments, the voxel-control lens may have lower
f-numbers, such as 0.5. Lower f-numbers are desirable because they
allow for a wider angle of view. In yet other embodiments, the
voxel-control lens may be monochromatic.
[0079] FIG. 12 depicts yet another embodiment of the present
invention. Referring to FIGS. 12-16, a reference beam-steering
system, generally 400, may use a beam-steering mirror system 450 to
direct a reference beam 25, through a first beam-steering lens 410
and a second beam-steering lens 405 to an elemental hologram 110 on
a holographic recording material 70 which, if desired, may be
inclined with respect to the normal to the center axis 420.
[0080] The beam-steering mirror system, generally 450, may be
embodied in various ways. One particular embodiment is depicted in
FIG. 15. In FIG. 15, a deflection mirror 460 is fixedly mounted to
a first rotatable mount 465, such that when the first rotatable
mount 465 rotates, the deflection mirror 460 rotates about a first
axis 451 which passes through center point 461 of the deflection
mirror 460. A motor for the first rotatable mount 470, which is
controlled by a motor controller 455, rotates the first rotatable
mount 465. The motor for the first rotatable mount 470 is fixedly
attached to a support 475. First rotatable mount 465 is rotatably
mounted to a support 475 with bearings or bushings to allow the
first rotatable mount 465 to rotate about the first axis 451.
Support 475 is fixedly mounted by an attaching device on a second
rotatable mount 480 such that when the second rotatable mount 480
rotates, the deflection mirror 460 rotates about a second axis 452
which passes through the center point 461 of the deflection mirror
460 and which is orthogonal to the first axis 451. A motor for the
second rotatable mount 485, which is controlled by a motor
controller 455, rotates the second rotatable mount 480. The motor
for the second rotatable mount may be fixedly attached to a
vibration isolation table 80. The motors for the first and second
rotatable mounts, 470 and 485, may be, but are not limited to,
stepper motors or DC servo motors. The same or a separate motor
controller 455 controlled by computer 230 may control the motors
for the first and second rotatable mounts 470 and 480.
[0081] Another embodiment of a beam-steering mirror system 450 is a
deflection mirror attached to a gimbal mount. In FIG. 16, a
deflection mirror 460 is fixedly mounted to a first axle 490 such
that the deflection mirror 460 rotates about a first axis 451 which
passes through the center point 461 of the deflection mirror 460.
First axle 490 is rotated by a motor 491 for the first axle which
is controlled by a motor controller 455. The motor 491 for the
first axle is fixedly attached to a first gimbal mount 494. First
axle 490 is rotatably mounted by bearing or bushing to the first
gimbal mount 494. The first gimbal mount 494 is fixedly mounted by
an attaching device to a second axle 492 at the opposite ends of a
diameter of the first gimbal mount 494 that coincides with a second
axis 452. Second axle 492 is rotated by a motor 493 for the second
axle and is controlled by a motor controller 455. The deflection
mirror 460 rotates about the second axis 452 which passes through
the center point 461 of the deflection mirror 460 and which is
orthogonal to the first axis 451. Second axle 492 is rotatably
mounted by bearing or bushing to a second gimbal mount 496. The
motors 491 and 493, for the first and second axles, 491 and 493,
may be, but are not limited to, stepper motors or DC servo motors.
The same or separate motor controllers 455, controlled by a
computer 230, may control the motors for the first and second
axles, 491 and 493.
[0082] As shown in FIGS. 12-16, the center axis 420 of the
beam-steering lenses 405, 410 intersects the first axis 451 and the
second axis 452 and passes through the center of an elemental
hologram. A reference beam 25 may be directed at the center point
461 of the deflection mirror 460. A computer 230 controls the
mirror system motor controller or controllers 455 of the
beam-steering mirror system 450, such that a reference beam 25
reflected off the deflection mirror 460 hits an elemental hologram
110 on a holographic recording material 70 at a desired angle. The
deflection mirror 460 may be placed at a distance of one focal
length 411 of the first beam-steering lens away from a first
beam-steering lens 410. The first beam-steering lens 410 may be
placed at a distance of the sum of the focal length 411 of the
first beam-steering lens and the focal length 406 of the second
beam-steering lens away from the second beam-steering lens 405. The
second beam-steering lens 405 may be placed at a distance of one
focal length 406 of the second beam-steering lens, away from the
holographic recording material 70. The beam-steering system 400 of
the present invention allows the reference beam 25 to be steered to
intersect with elemental holograms 110 at different angles.
[0083] In another embodiment, depicted in FIG. 13, the
beam-steering system 400 of the present invention may include a
reference-beam converging lens 415 which may be achromatic or
monochromatic. After a reference beam 25 passes through the
reference-beam converging lens 415, the reference beam 25 is
reflected by a beam-steering mirror system 450 before passing
through beam-steering lenses 410 and 405. The first and second
beam-steering lenses 410, 405 are placed such that the reference
beam 25 that passes through the converging lens and the first
beam-steering lens 410 converges in the focal plane 425 of the
second beam-steering lens 405. In addition, the center point 461
shown in FIGS. 15 and 16 of a deflection mirror 460 shown in FIGS.
15 and 16 is located at a distance of one focal length 411 of the
first beam-steering lens from the first beam-steering lens 410.
Furthermore, the elemental hologram 110 to be exposed is located at
a distance of one focal length of the second beam-steering lens 406
away from the second beam-steering lens 305.
[0084] In another embodiment, depicted in FIG. 14, the beam
steering system 400 of the present invention may include a
beam-steering aperture 430 which eliminates the need to have a
reference beam masking plate. In an embodiment, a reference beam 25
passes through a beam-steering aperture 430 that has the aperture
of the area of the elemental hologram 110 to be exposed. If the
reference beam passes through lenses that magnify or minify it,
then the beam-steering aperture 430 should be sized such that the
cross-section of the reference beam that intersects the elemental
hologram to be exposed has the same size and shape of the elemental
hologram. The reference beam 25 then passes through two aperture
relay lenses 435, is reflected off of a deflection mirror 460
(shown in FIGS. 15 and 16) of the beam-steering mirror system 450,
passes through the first beam-steering lens 410, passes through the
second beam-steering lens 405, and then intersects the elemental
hologram 110 to be exposed. The beam-steering aperture 430 is
placed at a distance of one focal length 436 of the aperture relay
lenses from one aperture relay lens 435. The aperture relay lenses
435 are located two focal lengths 436 of the aperture relay lens
away from each other. Then the center point 461 (shown in FIGS. 15
and 16) of the deflection mirror 460 (shown in FIGS. 15 and 16) is
located at a distance of one focal length 436 of the aperture relay
lens away from the second aperture lens 435 that the reference beam
passes through.
[0085] Another embodiment of a reference beam-steering system 400
is illustrated by FIGS. 17, 18, and 21. In this embodiment, an
optical coupler lens 670 channels a reference beam 25 that has just
passed through a beam shutter to the fiber optic end 660 of a fiber
optic cable 650. The fiber optic cable 650 delivers the reference
beam 25 to a fiber optic tip 655 which is placed in the focal plane
425 of a second beam-steering lens 405. The reference beam 25
passes through a beam-steering lens 405 to an elemental hologram
110. The beam-steering lens 405 is located at a distance of one
focal length 406 of the second beam-steering lens from the
elemental hologram 110 being exposed. The fiber optic tip 655 is
translated by a translation system, generally 600.
[0086] FIG. 19 illustrates another embodiment of the reference
beam-steering system 400. In this embodiment, three reference beams
25 which may each be a different color are channeled by three
optical coupler lenses 670 toward three fiber optic ends 660 of
three fiber optic cables 650. The fiber optic cables 650 deliver
the reference beams 25 to fiber optic tips 655 to direct the
reference beams 25 into optical combiner unit 640. Optical combiner
unit 640 may have two dichroic combiners 215, which may combine the
three reference beams 25 into a single reference beam 25, other
suitable optical combiners. The optical combiner unit 640 is placed
in the focal plane 425 (shown in FIG. 17) of a beam-steering lens
405. The single reference beam 25 from the optical combiner unit
640 passes through the beam-steering lens 405 to an elemental
hologram 110. The beam-steering lens 405 is located at a distance
of one focal length 406 of the beam-steering lens from the
elemental hologram 110 being exposed. The optical combiner unit 640
is fixedly mounted to a platform 630 which is fixedly mounted to a
second movable support 622.
[0087] In another embodiment, three reference beams 25 are
transmitted by fiber optic cables 650 to a optical combiner unit
640. The single reference beam 25 that is output from the optical
combiner unit 640 is channeled by an optical coupler lens 670 into
a single fiber optic cable 650 which is attached to and carried by
an attaching device to a translation system 600. The fiber optic
tip 655 of the single fiber optic cable 650 is located in a focal
plane 425 of a beam-steering lens 405.
[0088] In still another embodiment, the three reference beams 25
are transmitted by fiber optic cables 650 to a optical combiner
unit 640. The single reference beam 25 that is output from the
optical combiner unit 640 passes through a beam shutter 225 before
it is channeled by an optical coupler lens 670 into a single fiber
optic cable 650 which is fixedly attached to a translation system
600. The fiber optic tip 655 of the fiber optic cable 650 is
located in a focal plane 425 of a beam-steering lens 405.
[0089] The translation system 600, as depicted in FIG. 18 and FIG.
19, is able to translate in two orthogonal directions. The
translation system includes a x-translation stage and a
y-translation stage.
[0090] One illustrative embodiment of a x-translation stage 680
includes a first lead screw 602 which is rotatably mounted by
bushing, bearing, or other rotatable means to first end plates 608,
and which may be rotated about the axis 601 of the first lead screw
by a motor 604 for the first lead screw which is fixedly mounted to
one of the first end plates 608. Two first guide bars 610 are
fixedly mounted to the first end plates 608 such that the first
guide bars 610 lie parallel to the axis of the first lead screw
601. The two first guide bars 610 pass through two holes in a first
movable support 612. The first lead screw 602 is threaded through a
hole in the first movable support 612. Thus, in this embodiment of
the x-translation stage 680, when the first lead screw 602 is
rotated by the motor 604 for the first lead screw, the first
movable support 612 will move along the axis 601 of the first lead
screw.
[0091] One illustrative embodiment of a y-translation stage 680
includes a second lead screw 618 which is rotatably mounted by
bushing, bearing, or other rotatable means to second end plates
614, and which may be rotated about the axis 617 of the second lead
screw 618 by a motor 620 for the second lead screw which is mounted
to one of the second end plates 614. The other of the second end
plates 614 is mounted to the first movable support 612 such that
the axis 617 of the second lead screw is orthogonal to the axis 601
of the first lead screw. Two second guide bars 616 are fixedly
mounted to the second end plates 614 such that the second guide
bars 616 lie parallel to the axis 617 of the second lead screw. The
two second guide bars 616 pass through two holes in a second
movable support 622. The second lead screw 618 is threaded through
a hole in the second movable support 622. Thus, in this embodiment
of the y-translation device 690, when the second lead screw 618 is
rotated by the motor for the second lead screw 620, the second
movable support 622 will move along the axis 617 of the second lead
screw.
[0092] The motors 604 and 620, for the first and second lead screws
which may be, but are not limited to stepper, DC servo or linear
motors, may be controlled by a motor controller 606 for the motors
for the lead screws which may be controlled by computer 230.
[0093] Although the types, focal lengths, and number of
beam-steering lenses may be varied, for some embodiments, it may be
desirable for the beam-steering lenses to be achromatic and have
f-numbers of around 3.0 or less. In other embodiments, it may be
desirable for the beam-steering lenses to be achromatic, confocal,
f-.theta. lenses, which are also known as flat-field laser-scan
lenses. In some embodiments, it may also be desirable to have
lenses of lower f-number to allow for a wider range of reference
beams. In one particular embodiment, it may be desirable to have
the beam-steering lenses be achromatic and have f-numbers of around
1.0. In addition, the beam-steering lenses may be monochromatic in
other embodiments.
[0094] The beam-steering system of the present invention may be
utilized to create holographic stereograms that display a
particular image when illuminated by an illumination source from
one angle, but display another image when illuminated by an
illumination source from another angle. For instance, after
exposing an elemental hologram with an object beam conditioned with
a particular image on an SLM and a reference beam at a particular
angle, the elemental hologram may then be exposed to an object beam
conditioned with another image on the SLM and a reference beam at
another angle. In addition, a set of elemental holograms on a
holographic recording material may be exposed by a reference beam
at a particular angle, while another set of elemental holograms may
be exposed by a reference beam at another angle. Thus, a printer of
this invention can create a holographic stereogram that displays a
different image depending on the angle of the illumination source.
Furthermore, the same printer with a beam-steering system may be
used to create multiple holographic stereograms, each with a
different reference angle, such that the images of each will only
appear when illuminated by an illumination source at the correct
angle. If such multiple holographic stereograms are mounted on top
of each other, then different images may be displayed by simply
changing the angle at which the illumination source intersects the
holographic recording materials.
[0095] Another embodiment of the present invention, illustrated by
FIG. 20, utilizes multiple SLMs 90 to produce full-color
holographic stereograms. In FIG. 20, two dichroic combiners 215 in
an "x" configuration, or other suitable optical combiners, may be
used in combination with three object beams 20, one object beam
being red light, the other green light, and the other blue light.
The three object beams 20 may be directed through three separate
gray-scale SLMs 90. In one embodiment of the present invention the
SLMs are LCD panels of high resolution such as 1,280.times.1,024
pixels where the total size of the LCD panel is approximately 10
cm.times.10 cm. However, smaller LCD panels may be used. For
instance, LCD panels with the same or fewer number of pixels but
that are around 2 cm.times.2 cm in size or smaller may be used.
[0096] In an embodiment shown in FIG. 20 and FIG. 21, after passing
through beam shutters 225, object beams 20 are directed through
optical coupler lenses 670 to converge at fiber optic ends 660. The
object beams 20 are then transmitted by fiber optic cables 650 to
the fiber optic tips 655 which are placed in the focal planes of
singlet lenses 705. The object beams 20 may pass through the
singlet lenses 705, if necessary, reflect off mirrors 40, and pass
through SLMs 90 and band-limited diffusers 45, which may be color
specific. The singlet lenses 705 expand and collimate the object
beams 20 such that the object beams 20 may more evenly illuminate
the SLMs 90. The object beams 20 are then directed through a
optical combiner unit 640 that may use two dichroic combiners 215
in an "x" configuration, or other suitable optical combiners, to
combine the three object beams 20 into a single beam. The single
object beam 20 may then pass through a first projection lens 715
and a Fourier transform filter 710 that may remove undesired
effects such as, but not limited to, high frequency image
components such as pixel or grid artifacts that resulted from an
SLM display with pixels. The object beam 20 may then pass through a
second projection lens 720 and then a converging lens 55. The first
projection lens 715 is located such that images of the SLMs all lie
in the focal plane of the first projection lens. The Fourier
transform filter 710 is located in the focal planes of both the
first projection lens and the second projection lens. The
converging lens 55 is located such that its focal plane intersects
the holographic recording material 70 at the elemental hologram 110
to be exposed. In other embodiments of the object beam unit 700,
the first and second projection lenses 715 and 720 and the Fourier
transform filter 710 are not used. In still other embodiments of
the object beam unit 700, a voxel control lens 500 may be included
in the object beam unit 700 and lie in close proximity to the
holographic recording material 70.
[0097] In one embodiment of the present invention, a material
holder, generally 300, may be used to translate holographic
recording material 70. As depicted in FIGS. 22-25, a material
holder 300 may include a frame 324 attached to a x-translation
stage 680 that is attached to a y-translation stage 690.
[0098] An embodiment of the y-translation stage 680, as depicted in
FIGS. 22-25, may have first holder end plates 302 to which first
holder guide rods 306 are fixedly attached. A first holder lead
screw 308 and a first holder driven lead screw 309 are rotatably
attached by bushing or bearing or other suitable means to the first
holder end plates 302. The first holder lead screw 308 and the
first holder guide rods 306 are parallel to the axis of the first
holder driven lead screw 307. The first holder driven lead screw
309 may be rotated by a motor 310 for the first holder driven lead
screw, which is controlled by holder motor controller 305, which is
controlled by computer 230. The motor 310 may also drive both lead
screws 308 and 309 with a timing belt or other linkage. In
addition, two motors 310, each coupled to a lead screw, may drive
the lead screws. The first holder driven lead screw 309 passes
through a threaded hole in the a first holder movable support 312.
The two first holder guide rods 306 in close proximity to the first
holder driven lead screw 309 pass through holes in the same first
holder movable support 312. The first holder lead screw 308 passes
through a threaded hole in another first holder movable support
312, and the two first holder guide rods 306 in close proximity to
the first holder lead screw 308 pass through holes in the same
first holder movable support 312.
[0099] An embodiment of the x-translation stage 680, as depicted in
FIGS. 22-26, may have a second holder lead screw 318 and a first
holder driven lead screw 319 rotatably attached by bushing or
bearing or other suitable means to second holder end plates 314.
The axis of the second holder driven lead screw 317 is orthogonal
to the axis of the first holder driven lead screw 307. The second
holder lead screw 318 and the second holder guide rods 316 are
parallel to the axis of the second holder driven lead screw 317.
The second holder driven lead screw 319 may be rotated by a motor
320, for the second holder driven lead screw which is controlled by
holder motor controller 305, which is controlled by computer 230.
The second holder driven lead screw 319 passes through a threaded
hole in the a second holder movable support 322. The two second
holder guide rods 316 in close proximity to the second holder
driven lead screw 319 pass through holes in the same second holder
movable support 322. The second holder lead screw 318 passes
through a threaded hole in another second holder movable support
322, and the two second holder guide rods 316 in close proximity to
the second holder lead screw 318 pass through holes in the same
second holder movable support 322.
[0100] As depicted in FIGS. 22 and 23, the x-translation stage 680
may be mounted to the y-translation stage 690. In one embodiment,
the first holder movable supports 312 are fixedly mounted to the
second holder end plates 314. The second holder movable supports
322 are fixedly attached to a frame 324. A second frame 324 may be
clamped to a first frame 324 by detachable couplings 325 which may
include, but are not limited to, clamps, snaps, screws, and bolts.
A holographic recording material may be held in between two
detachably coupled frames 324. In an alternative embodiment, the
natural adhesive property of a holographic recording material may
hold the material on one side of a transparent plate that is
secured to frames 324. The frames 324 may be composed of
stress-relieved aluminum, titanium, composites, or other rigid,
strong, and lightweight materials.
[0101] As illustrated in FIG. 23, object beam units 700 and
reference beam-steering systems 400 may be fixed to bases 326.
[0102] As illustrated in FIGS. 24 and 25, one or more object beam
units 700 may be fixedly mounted to unit mounts 328 which are
fixedly mounted to second holder movable supports 322 of a
x-translation stage 680. Similarly, one or more reference
beam-steering systems 400 may be fixedly mounted to other unit
mounts 328 which are fixedly mounted to other second holder movable
supports 322 of another x-translation stage 680. In addition, in
some embodiments, a frame 324 may be fixed to the first movable
supports 312 of a y-translation stage 690. Thus, in some
embodiments, the holographic recording material 70 clamped between
two frames 324 may translate vertically, while the object beam
units 700 and reference beam-steering systems 400 translate
horizontally.
[0103] In the embodiment depicted in FIG. 24, two motors 320, which
are controlled by holder motor controller 305, drive the second
holder driven lead screws 319 of the x-translation stages 680. In
an alternative embodiment depicted in FIG. 25, one motor 320, in
combination with a timing belt 330 that is linked to a belt mount
332 that is fixedly attached to one of the second holder driven
lead screws 319, drives both second holder driven lead screws 319
of the x-translation stages 680.
[0104] In another embodiment depicted in FIG. 26, the object beam
units 700 and reference beam-steering systems 400 are attached to
unit mounts 328 which are attached to the second holder movable
supports 322 of x-translation stages 680. A holographic recording
material 70 translates vertically by a y-axis roller system 350
with rollers 342 and 344. The holographic recording material 70 may
be wrapped around a top roller 342 and a bottom roller 344. The top
and bottom rollers 342 and 344 are rotatably mounted by bushing,
bearing, or other suitable means between roller end plates 340. The
top roller 342 may be rotated by a motor for the rollers 346, which
is controlled by a motor controller 305 which is controlled by a
computer 230.
[0105] The motors used in the various embodiments of the
translation systems may be, but are not limited to stepper
motors.
[0106] As depicted in FIGS. 23-26, there may be simultaneous or
parallel printing of elemental holograms. In some embodiments, the
printer may include object beam units and reference beam-steering
systems attached to translation systems with x-translation stages
that are attached to y-translation stages. In such systems, the
holographic recording material may be fixed, while the object beam
units and reference beam-steering systems are moved by the
translation system to record an array of elemental holograms.
[0107] In an alternative embodiment, multiple layers of holographic
recording material 70 may be held in a material holder 300. In
addition, each layer may be sensitive to a particular wavelength of
light.
[0108] In another embodiment of the present invention, for a given
object beam, a matched set of a band-limited diffusers 45 and a
reference beam masking plate 65 may be configured to allow for even
exposure of an elemental hologram 110 of a particular size or shape
and to prevent exposing portions of the holographic recording
material 70 that are not part of the elemental hologram 110
intended to be exposed. As illustrated by FIGS. 27(a), (b), and
(c), matched sets of band-limited diffusers 45 and reference beam
masking plates 65 can be constructed to allow the exposure of
elemental holograms 110 of different sizes or shapes. If the sets
of band-limited diffusers 45 and reference beam masking plates 65
are constructed such that the band-limited diffusers 45 of all the
sets have the same outer dimensions and can be placed in the same
position in a hologram printer, and such that the reference beam
masking plates 65 of all the sets have the same outer dimensions
and can be placed in the same position in a hologram printer, then
sets can be conveniently switched to easily change the size of the
elemental hologram printed. Thus, a matched set of a band-limited
diffuser 45 and a reference beam masking plate 65 can be replaced
with another set of a band-limited diffuser 45 and a reference beam
masking plate 65 so as to allow printing of a larger, smaller, or
differently shaped elemental hologram. As depicted in FIG. 27(b), a
band-limited diffuser 45 may be mounted onto a plate 510 housed in
a threaded frame 515. The plate 510 may be a sheet transparent
sheet of glass with an anti-reflective coating. The threaded frame
515 may be threaded into positioning device 525 which has a base
526 and a threaded ring 520. The positioning device 520 may allow
translational adjustment in three orthogonal directions by three
adjustable screws 530. As depicted in FIG. 27(c), a reference beam
masking plate 65 may be housed in a threaded plate frame 560. A
threaded plate frame 560 may be threaded into a threaded
positioning device 565.
[0109] Some examples of full-color embodiments of the present
invention are depicted in FIGS. 7, 8, 19, and 21. Another
embodiment of the present invention includes a full-color printer
with three different colored lasers, optical combiners, such as but
not limited to dichroic combiners, to combine the three beams from
the lasers, a full-color SLM, and achromatic optics to print
full-color holographic sterograms. Still another embodiment of the
present invention includes a full-color printer with three
different colored lasers, an object beam unit that combines three
object beams using three band-limited diffusers, three gray-scale
SLMs, and an optical combiner, achromatic optics, such as
achromatic lenses, to manipulate or condition the full-color beams
produced by the printer, and an optical combiner to combine three
reference beams into a combined, full-color, reference beam. Yet
another embodiment of the present invention includes a full-color
printer with three different colored lasers, an object beam unit
with an HOE that combines three different colored object beams into
one combined, full-color, object beam and that also evenly
distributes the combined object beam over an elemental hologram, an
optical combiner to combine three reference beams into a combined,
full-color, reference beam, and achromatic optics to manipulate or
condition the full-colored beams.
[0110] Another aspect of the present invention involves a method of
creating animated, one-step, full-parallax, holographic
stereograms. One embodiment involves using multiple or sub-divided
viewing zones, which typically are not needed to produce static
image, full-parallax holographic stereograms, to produce one-step,
full-parallax, holographic stereograms that can display animated
subjects or different images through different viewing zones.
Viewing zones are typically planar areas located at a distance from
the holographic recording material in which a viewer's eye looking
through that plane could see the holographic image produced by an
array of elemental holograms. Thus, a viewing zone may be analogous
to a window in front of a hologram. However, rather than being
planar, viewing zones may also be constructed from a series of
points. Unlike traditional techniques for producing one-step,
full-parallax holographic stereograms in which the view of a
three-dimensional object or a scene is determined for each
elemental hologram, the present invention produces animated,
one-stop, full-parallax holographic stereograms by determining the
view of an object or scene that an observer would see in each
viewing zone.
[0111] Referring to FIGS. 28-31, and assuming that a voxel-control
lens 500 is used such that the image 505 (shown in FIG. 10(b)) of
an SLM would appear at an infinite distance from the surface of the
holographic recording material, the steps for producing a
holographic element of an animated holographic stereogram or a
holographic stereogram that displays different images in different
viewing zones are as follows. [0112] 1) Select the size and shape
of a holographic stereogram, and the size and shape of its
elemental holograms. [0113] 2) Select the desired effect. One
example of an effect is changing the orientation of an object or a
scene (e.g., its position or rotation) when a viewer moves. Another
example of an effect is changing the shape or color of an object or
a scene when a viewer moves. [0114] 3) Select the reference
illumination geometry for the final holographic stereogram. [0115]
4) Select the shape(s), size(s), and location(s) of the viewing
zone or zones with respect to the holographic recording material.
In the plane of the viewing zone, a viewer would see a sharper
transition between the different objects or scenes depicted by the
holographic stereogram than a viewer not in the plane of the
viewing zones. Thus, it may be desirable to select the location of
the viewing zones to be at a distance from the holographic
recording material where most viewers would be located. [0116] 5)
Select the objects or scenes or the attributes of the objects or
scenes to be displayed by the holographic stereogram. [0117] 6)
Select the location and placement with respect to the holographic
recording material of the holographic images of the objects that
will be displayed by the holographic stereogram to be created (i.e.
whether the image will be located in front of, in back of, or
straddle the holographic recording material). [0118] 7) Using a
computer 230, generate computer models and model attributes for
each viewing zone using traditional computer graphic techniques and
programs of the objects or scenes. For instance, generate a
computer model of an object `A` 835 which can only be seen from one
viewing zone 805, and generate a computer model of an object `B`
840 which can only be seen from another viewing zone 810. [0119] 8)
Set up the hologram printer. For instance, put holographic
recording material 70 (shown in FIG. 7) into a material holder 300
(shown in FIG. 7), calibrate and initialize beam shutters 225
(shown in FIG. 7), motor controllers 305, 455 the SLM 90 (shown in
FIG. 7), the beam-steering system 400 (shown in FIG. 7), and
initialize the computer graphics program, and the computer 230
(shown in FIG. 7). [0120] 9) Using a computer 230, for each
elemental hologram 110 in a holographic stereogram that may be a
one-step, full-parallax, holographic stereogram: [0121] A) Project
lines from the perimeter of the elemental hologram 110 through the
perimeter of each of the view zones 805 and 810. Since in a typical
printer, a SLM is usually centered in front of an elemental
hologram when the elemental hologram is exposed, the virtual image
of the SLM that an elemental hologram would see through a
voxel-control lens is also usually centered in front of the
elemental hologram, as shown in FIG. 29. As depicted in FIG. 30,
the projected lines intersect a virtual two-dimensional image 505
(shown in FIG. 10(b)) of a SLM image. The elemental hologram will
only see the portion of the virtual image 505 of the SLM, such as
815 or 820, bounded by the projecting lines. As shown in FIG. 30,
the projected lines define mask volumes 825, 830, which may differ
from one elemental hologram to another for a given viewing zone.
[0122] B) For a desired viewing zone mask volume, such as 825, for
an elemental hologram 110, using traditional rendering techniques,
such as but not limited to, ray-tracing or scan-line conversion,
render the portion of the appropriate computer model of an object
or scene 835 (shown in FIG. 30) enclosed by the projected mask
volume 825 to create a complete two-dimensional image of a
projection on the portion of the virtual image 505 of the SLM of
the computer graphic models of the objects or scenes 835 or 840
from the perspective of an elemental hologram. For instance, if a
person were to look at a particular elemental hologram from within
a mask volume 825, only the `A` object 835 is seen. From mask
volume 825, the `B` object 840 is not viewable. Thus, to a viewer
in mask volume 825, the bottom of the virtual image of the SLM is
not visible. Similarly, if a person were to look at the particular
elemental hologram from within a mask volume 830, only the `B`
object 840 is seen. From mask volume 830, the `A` object 835 is not
viewable. Thus, to a viewer in mask volume 830, the top of the
virtual image of the SLM is not visible. [0123] C) When rendering
is complete for all the viewing zones 805 and 810 for an elemental
hologram, composite the rendered images for the viewing zones.
[0124] D) Display the composite rendered image for the viewing
zones 805 and 810 on the SLM 70 and allow light to pass through the
beam shutters 225 for the proper time period to expose the
elemental hologram. [0125] E) Translate the material holder such
that another elemental hologram can be exposed. [0126] F) Repeat
steps A through E until all the elemental holograms have been
exposed.
[0127] In an alternative embodiment, rendering for multiple
elemental holograms may be completed before exposing any of the
elemental holograms on a holographic recording material.
[0128] In an alternative embodiment, the same method applied for
creating holographic stereograms with changing views may be used to
create a holographic optical element (HOE). For instance, if it is
desirable to create a HOE that acts like a lens to a converge
diverging white light to a point, then by using the same viewing
zone method as described, but determining a view point located at
where the light should be focused, rather than a view zone, a HOE
may be created. Alternatively, such a HOE can be created by
determining a white computer-graphic object with the exact size,
shape, and position of a given voxel, and printing a holographic
stereogram of such an object.
[0129] In one embodiment of the present invention, the same
computer 230 may be programmed to control the motors controlling
the beam shutters, the motor controllers for the beam-steering
mirror system, the motor controllers for the translation systems,
conducts the computer graphics creation and rendering, and controls
the display of the SLM. In an alternative embodiment, the same
computer may also conduct the computations necessary for animation.
The computer 230 may be connected to the beam shutters, the motor
controllers for the beam-steering mirror system, and the SLM,
through cables connected at both ends to serial or parallel
communication ports. One end of the cables may be connected to the
communication ports of the computer and the other ends of the
cables may be connected to the devices controlled by the computer.
In other embodiments, multiple computers 230 may be used.
[0130] While the methods and apparatus of this invention have been
described in terms of illustrated embodiments, it will be apparent
to those of skill in the art that variations, such as but not
limited to different combination of lens set-ups to create the same
effect as the voxel-control lens or the beam-steering lenses
described herein, may be applied to the methods and apparatus and
in the step or in the sequence of steps of the methods described
herein without departing from the concept, spirit and scope of the
invention. All substitutes and modifications apparent to those
skilled in the art are deemed to be within the spirit, scope and
concept of the invention as defined by the appended claims.
* * * * *