CA2263643A1 - Color projection prism - Google Patents
Color projection prism Download PDFInfo
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- CA2263643A1 CA2263643A1 CA002263643A CA2263643A CA2263643A1 CA 2263643 A1 CA2263643 A1 CA 2263643A1 CA 002263643 A CA002263643 A CA 002263643A CA 2263643 A CA2263643 A CA 2263643A CA 2263643 A1 CA2263643 A1 CA 2263643A1
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- Prior art keywords
- prism
- optic axis
- angle
- component
- light
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
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Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/10—Beam splitting or combining systems
- G02B27/1006—Beam splitting or combining systems for splitting or combining different wavelengths
- G02B27/102—Beam splitting or combining systems for splitting or combining different wavelengths for generating a colour image from monochromatic image signal sources
- G02B27/1026—Beam splitting or combining systems for splitting or combining different wavelengths for generating a colour image from monochromatic image signal sources for use with reflective spatial light modulators
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/10—Beam splitting or combining systems
- G02B27/14—Beam splitting or combining systems operating by reflection only
- G02B27/145—Beam splitting or combining systems operating by reflection only having sequential partially reflecting surfaces
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- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04N—PICTORIAL COMMUNICATION, e.g. TELEVISION
- H04N9/00—Details of colour television systems
- H04N9/12—Picture reproducers
- H04N9/31—Projection devices for colour picture display, e.g. using electronic spatial light modulators [ESLM]
- H04N9/3102—Projection devices for colour picture display, e.g. using electronic spatial light modulators [ESLM] using two-dimensional electronic spatial light modulators
- H04N9/3105—Projection devices for colour picture display, e.g. using electronic spatial light modulators [ESLM] using two-dimensional electronic spatial light modulators for displaying all colours simultaneously, e.g. by using two or more electronic spatial light modulators
Abstract
A prism for color dispersion and recombination and a projector incorporating the prism. The prism comprises an aperture for a light beam and the normal to the aperture defines an optic axis. A first surface, intersecting the optic axis, is oriented at a first angle to the optic axis. The first angle is greater than 45~. The first surface disperses the light beam into a first component and an intermediate component. A second surface, intersecting the optic axis, is oriented at a second angle to the optic axis. The second surface disperses the intermediate component of the light beam into a second component and a third component.
Description
W O98/07061 PCTrUS97/14438 COLOR PROJECTION PRISM
TECHNICAL FIELD OF THE INVENTION
The present invention is directed to projection prisms, and more particularly to color projection prisms for dispersing and recombining light.
BACKGROUND OF T HE INVENTION
Color di~clwlllent and recombination are important aspects of color projection systems. In these systems, white light is created from, for example, an arc lamp. A prism or other such device is used to disperse the white light into three components: a red beam, a green beam and a blue bearn. These beams may be directed to reflective liquid crystal cells that interfere with and selectively reflect each beam. In other words, the interference imparts an image to each color bearn. More particularly, the reflective liquid crystal cells are often active matrix cells with a switching element for each pixel allowing each pixel to be individually addressed. The colors are recombined, and when projected on a screen form a full color image.
U.S. Patent No. 4,943,154 (1990), discloses a prior art projection system, as shown in Fig. 1. This system comprises a light source 51); a light ll~n~ 59; light valves 61, 62 and 63; a light combiner 64; a proJection lens 65; a drive circuit 67; an input side co~ gelll lens 68; an input side plane mirror 69; a central convergent lens 70; an output side plane mirror 71; and an output side convergent lens 72. The light source 50 comprises a lamp 51, a condenser lens 52, a concave mirror 53, and a heat absorbing filter 54. The lamp 51 radiates a light co..~ g three primary colors of red, green and blue. Rays of the radiant light from the lamp 51 are arranged in approximately parallel rays by the condenser lens 52 and the concave mirror 53. More specifically, the rays of light from the center of a luminous clenlenl 55 in the lamp 51 are tr~n~miltted in parallel to the optic axis 57 by the 25 condenser lens 52. From the light rays passed through the condenser lens 52, infrared rays are elimin~ted by the heat absorbing filter 54. The light rays from the light source 50 are sep~ted into three primary colors of red, green and blue. Red light passes through th -W O 98/07061 PCTrUS97114438 light tr~n~m~ r 59 and enters the red light valve 61. Green light is similarly tr~n~mitte~ to the green light valve 62, and blue light is transmitted to the blue light valve 63.
A light separator 90 is used to disperse the light into colored beams of red, green and blue. Separator 90 is shown having two plates 92 and 94. The tr~n.cmi~sive and reflective 5 properties of these plates are shown in the graphs of Figs. 2(a) and 2(b). Fig. 2(a) is a graph of tr~n~mi~sion (in percent) as a function of wavelength (in nanometers (nm)) for plates 92 and 94, corresponding to curves A and B, respectively. Fig. 2(b) is a graph of reflection (in percent) as a function of wavelength (in nm) for the same plates. In particular, Fig. 2(a) shows that plate 92, corresponding to curve A, has a low tr~n~mi~ivity for blue light but a 10 high tr~n~mi~ivity for green and red. Plate 94, corresponding to curve B, has a low trans-missivity for blue and green light but a high tr~nsmi.~sivity for red. Put another way, and as shown in Fig. 2(b), plate 92 reflects the blue light but transmits green and red. Of the green and red light that remains, plate 94 reflects the green but transmits the red. Thus, the two plates may be used to disperse the light before the light enters light valves 61, 62 and 63.
The light valves 61, 62 and 63 are liquid crystal panels each having matrix electrodes. The drive circuit 67 produces electric signals R, G and B according to a video signal Y to control the transmittance of pixels in respective light valves 61, 62 and 63. The modulated light outputs from the light valves 61, 62 and 63 are then combined into a composite flux of light substantially to reproduce a color picture at the position of the light 20 valve 62. An enlarged image of the color picture is finally projected by the projection lens 65 onto a screen 66.
Light combiner 64 may also be used to disperse the light into the different colors (this system is not shown). In this case, the light disperser/combiner often includes dichroic surfaces such as coated plates of glass or an int~-rn~lly-coated cçm~ntecl prism structure.
25 Coatings used as dichroic snrf~ces are typically thin films.
A disadvantage of coated plates is that such plates can introduce ~ctigm~ti~m in the optical path. Inserting additional non-coated plates may compensate for this defect at the expense of.simpliçity.
Prism structures have many advantages. They are ~ypically rugged, easy to mount,30 and useful for beam superposition applications. They deform less when subjected to stress than coated plates. Coatings used in prisms are resistant to degradation because they are usually sealed within the body of the cube.
Prism structures may also have some disadvantages. One may be a polarization dep~nllen~e of the reflected light arising from the coatings for the interior sllrf~ces. These coatings may be multilayered and reflective. As lihe angle of the plane of the coating to the direction of light moves away from 90~, specltral dirr~.~nces between the polarization components increase. In other words, the reflected light becomes at least partially polarized for some range of wavelengths, referred to as the transition region.
This effect may be seen, e.g., in Fig. 3(a), which shows the cG~ onding curves for 10 transmittance for a short-wave-pass beamsplittler or prism at 45~. In Fig. 3(a), the tr~n~mi.~sion (in percent) is plotted versus wavelength (in nm). The action of the beam-splitter is seen to be dependent on the polarization of the light. S-polarized light, i.e., light which has its electric field perpendicular to the plane of incidence, has a tr~n~mitt~nce curve which is shifted relative to that for p-polarized light, the latter being light which has its 15 electric field parallel to the plane of incidence. The amount of shifting is seen to be roughly 50 nm towards lower wavelengths. Thus, the transition region, in which polarization components may be subject to spectral differences, is about 50 nm wide.
Some beamsplitters have been constructed which reduce the spectral difference between the polarization components. Fig. 3(b) shows plots of wavelength (in nm) versus 20 reflection (in percent) for light of random polarization (*), s-polarization (+), and p-polarization (x) for a blue mirror made by Doctor Optic GmbH, of Vienna, Austria. It is seen that the s-polarization cG~ ,onen~ is shifted from the p-polarization component by about 5 nm. Thus, the transition region, in which polarization components may be subject to spectral dirf~.el-ces, is much smaller and is about 5 nm wide.
The partially polarized light is usually inci~lPnt on the cell which imparts an image to the light. The cell, which may use a scattering lilquid crystal material, may have at least a partial depolarizing effect. This may be Im(lesir~l~le. For example, if the incident beam is highly polarized, and the cell depolarizes that same state of polarization, then the i~Len~ily of the beam passing back through the prism may be ~ e.~ l In extreme cases, the intensity may drop to about half the incident intensity because the beam is not propclly reflected.
This type of alt~ml~tion is generally caused by each of the three cells. The overall effect is to reduce the tr~n.cmi~sion of the prism system. For example, a typical ratio of the 5 amount of light exiting the prism system to that entering is about fifty percent for dichroic surfaces that are oriented 45~ to the direction of the light. For cells that use polarization of the light for their optical action, this polarizing effect can be used to increase their contrast ratio. However, this may severely ~ e the light h~ellsily, perhaps by about sixty percent.
Some solutions have been proposed for the above problems. For example, U.S.
Patent No. 4,969,730 (1990), discloses a prism system with two air gaps. While these air gaps may reduce attenuation, they may produce undesirable "ghost" images.
Accordingly, an object of the invention is to provide an optical prism in which the ratio of the amount of light exiting the prism system to the amount entering is m~xi...i~.l Another object is to provide a prism system for color dispersement and recombination in which dispersement occurs while introducing a minimum of polarization in the dispersed light.
Additional objects and advantages of the invention will be set forth in the des-cription which follows, and in part will be obvious from the description, or may be learned 20 by practice of the invention. The advantages of the invention may be realized and obtained by means of the instr.~ nt~lities and combinations particularly pointed out in the claims.
BRIEF SUMMARY OF THE INVENTION
In one aspect, the present invention is directed to a prism for color tli~p~r~ion and recombination. The prism comprises an a~e~ c for a light beam. The normal to the25 a~ellult; defines an optic axis. A first surface, intersecting the optic axis, is oriented at a first angle to the optic axis. The first angle is greater than 45~. The first surface disperses the light beam into a first con~pol enl and an intermediate component. First, second and third working faces are located along dirre,ell- segment~ of the pel;phel~ of the prism. A
second surface, inte~eclillg the optic axis, and oriented at a second angle to the optic axis, disperses the intermediate component of the ligh1: beam into a second component and a third component. At least one of the first, second or third components passes directly to the first, second or third working faces, respectively, from one of the first or second surfaces.
ImplemPnt~tions include the following features. The prism may further comprise first, second and third cells for hnpa~ g images to the first, second and third components, ,~,i,pe~ilively. The cells may be liquid crystal cells having a plurality of picture elements which change from a more scattering state to a ]ess scattering state upon application of an input such as an electric field. The first and second surfaces of the prism may be coated with multilayer dichroic reflective coatings. Each of the first and second angles to the optic lO axis may be in the range of about 55~ to 85~, and more particularly in the range of about 60~
to 70~, and even more particularly may be about 65~.
In another aspect, the invention is direcled to an system for color dispersion and recombination. The system comprises an apertlure for a light beam. The normal to the al~,.Lul~ defines an optic axis. A first coated glass plate intersects the optic axis and has a 15 surface oriented at a first angle to the optic axis. The first angle is greater than 45~. The surface of the first coated glass plate disperses the light beam into a first component and an interrn~ t~ component. A second coated glass plate intersects the optic axis and has a surface oriented at a second angle to the optic axis. The second coated glass plate ~ p~r~es the int~rrn~ te cc,lllponel,l of the light bearn into a second component and a third 20 component.
In another aspect, the invention is directed to a projection system. The system has a light source, a reflector adjacent the light source for directing the light to a steering mirror and a field lens for collecting light received from the steering mirror. A prism is provided to collect light from the field lens. The prism may be such as described above.
In another aspect, the invention is directed to a prism having at least one working face located along the periphery thereof for color dispersion and recombination. The prism compri.~e~ an ~llule for a light beam, where the normal to the al~c,lu~e defines an optic axis. A plurality of surfaces intersect the optic axis and at least one of the plurality of snrf~ces is oriented at a first angle to the optic axis. The first angle is greater than 45~ and 30 disperses the light beam into a first component and an interme~ te component. The first component passes directly to the working face from one of the plurality of surfaces. The plurality of surfaces includes dichroic surfaces.
An advantage of the invention is that the ratio of the light exiting the prism to the light entering the prism is high because light reflected inside the prism is only weakly 5 polarization dependent.
A further advantage of the invention is that the use of a prism structure makes the system rugged, easy to mount, and useful for beam superposition applications. Prisms deform less when subjected to stress than coated plates. Coatings used in prisms are resistant to degradation because they are usually sealed within the body of the cube.
BRIEF DESCRIPTION OF THE DRAWING(S) The accompanying figures, which are incorporated in and co~ ilule a part of the specification, schem~tically illustrate the invention and, together with the general description given above and the detailed description given below, serve to explain the principles of the invention.
Fig. 1 is a top plan view of a more detailed prior art projection system.
Figs. 2(a) and 2(b) are graphs of tr~n~mi~ivity and reflectivity, respectively, for plates 92 and 94 of Fig. 1.
Figs. 3(a) and 3(b) are graphs showing spectral differences between polarizationcomponents.
Fig. 4 is a top plan view of an embodiment of the present invention.
Fig. 5 is a top plan view of an embodiment of the present invention as used in aprojection system.
DETAILED DESCRIPTION OF THE INVENTION
Referring to Fig. 4, a color projection prism 120 includes an apcll~e 121. Aperture 121 is the area through which the white light enters the prism and through which the color-imaged light exits the prism. It may be as simple as the face of the prism itself, but is usually defined by the a~ Lul~ of the lens. The normal to the plane of aperture 121 generally defines an optic axis of the system. First, second and third reflection cells 122, W O 98/07061 PCTAUSg7/14438 127 and 129 are also provided and are denoted here as green (G) cell 122, blue (B) cell 127 and red (R) cell 129. Such cells, which may be oi the type using nematic curvilinear aligned phases (NCAP) liquid crystal materials or other types, are often used with the color projection prism of the present invention to form a color projection system, but this is not 5 necessary.
An NCAP liquid crystal cell uses a liquiàl crystal material which is ellr~rs~ ted in or dispersed in a col-t~in~ nt medium such as a polymer. Suitable enc~psul~ting media include, but are not limited to, gelatin, polyurethane, polyethylene oxide, polyvinyl pyrrolidone, cellulosic polymers, natural gums, acrylic and methacrylic copolymers, 10 epoxies, polyolefins, vinyl polymers, aqueous :lattices, and the like. In particular, the enc~psl-l~ting medium may be polyvinyl alcohol or a polyurethane latex. The liquid crystal m~t~ri~l may be nematic or operationally nematic, and may have a positive dielectric anisotropy. Alternately, the liquid crystal material may be smectic or chiral nematic. In addition, a pleochroic dye may be dissolved in the liquid crystal material.
Generally, such liquid crystal cells have a ]plurality of picture elements which change from a more sc~ttering state to a less scattering state upon application of an input, such as an electric field.
Prism 120 may be constructed of a number of prism segm~nt~ These prism segment~ have at least some surfaces which are coated with dichroic thin film reflectors such as a multilayer stack of al~ "~ g refractive index m~teri~l~. The precise design of the multilayer stack depends on the requirements of the ~lesigner. The segments are bonded together with an adhesive to form prism 120. In Fig. 4, two coated surfaces are formed:
first surface 123 and second surface 125. The coatings of these sl.rf~es are dichroic. The angle x between surfaces 123 and 125 is generally less than 90~.
White light enters the prism 120 along the direction of arrow 124 and is incident on surface 123 at an angle to the optic axis of greater than 45~. This white light beam may be ge~ d by an arc lamp, for example. A first component of the white light, in particular the blue bearn, is reflected from surface 123 and is directed towards a first working face 126 of the prism, a(ljac~nt to which is blue cell 127. The terrn ".working face" is defined herein as a face on which an active optic elem~nt would be placed or a face through which light may be directed to a cell. First working face, as well as second and third working faces described below, are generally located along dirrelelll portions of the periphery of the prism.
The choice of which color beam is reflected first is dependent on the nature of surface 123 and may be changed according to the preference of the user. Usually either blue or red is reflected first because l) they are nearer to the ends of the spectrum and 2) high and low pass reflectors are easier to form than band pass reflectors. In particular, the coating of surface 123 is a multilayer stack of altçrn~tine refractive index materials, e.g., silicon dioxide with a refractive index of about 1.5 and alumina with a refractive index of about 1.7. The thickness of each layer is designed to reflect substantially all light below a 10 certain wavelength, e.g., for blue, 490 nm is used. For red light, they are designed to reflect substantially all light above a certain wavelength, e.g., 570 nm. The reflection from surface 123 may cause some disparity between the s-polarized and p-polarized portions of the blue bearn, as described above in connection with Fig. 3(a). However, the closer surface 123 is to being 90~ to the optic axis, the less this difference will be.
Surface 123 is designed to increase the angle to the optic axis. It is oriented at a first angle to the optic axis of greater than 45~. This first angle may be in the range of about 55~
to 85~, and can be about 65~. In part, as this angle is closer to norrnal than, for example, a 45~ angle, the amount of polarization introduced into the beam, in this case the blue beam, is less than in prior systems.
Blue cell 127 imparts an image to the blue beam and reflects the same back towards surface 123. Blue cell 127 may have a partial depol~n~ing effect on the blue beam, as described above. However, in the present embodiment, the blue beam leaves surface 123 with less difference between its s- and p-polarizations (because of the angle to the optic axis) than, for example, if the angle to the optic axis was 45~. Therefore, there is less 25 chance of the blue beam being transmitted by surface 123 on its return.
The blue beam emerges from blue cell 127, passes through the first working face 126 of the prism, and is directed towards surface 123. Surface 123 reflects the blue beam back in a direction parallel but opposite to arrow 124.
Light transmitted through surface 123 is composed of an int~nne~ te component:
30 the white light minus the blue beam. This light is incident on surface 125 at an angle to the optic axis which is again greater than 45~. This surface disperses the intermediate component into second and third components, i.e., into a reflected red beam and a transmitted green beam.
A polarization effect similar to that above occurs for the red beam. The reflection S from surface 125 partially polarizes the red beam. However, surface 125 provides an angle to the optic axis which is closer to normal, i.e., 90'', than in prior systems. Therefore, for the same reasons as above, surface 125 introduces less of a dirr~lcnce between the polarizations of the beam, i.e., less polarization dep~n~ence, than if the angle to the optic axis were, for example, 45~.
Surface 125 reflects the red beam towards, a second working face 128 and red cell 129, and transmits the rem~ining light, the green beam, towards a third working face 130 and green cell 122. Red cell 129 imparts an ima;ge to the red beam and reflects the same back towards surface 125. Surface 125 directs the beam in a direction parallel but opposite to arrow 124. Any light is which ~ sllliLled lthrough surface 125 is lost by multiple 15 reflection and scattering. Any depolarizing effects of red cell 129 will produce, at most, only minim~l effects on the red beam because of the dichroic surface's weak polarization depçn~n.~e The green beam lcprcsellts the rern~in-lçr of the light after the blue and red beams are removed by reflections from surfaces 123 and 125. The green beam is transmitted 20 directly through the prism with little change in ~mgle and is incident on green cell 122 because the dichroic surfaces do not reflect green light. Rather, they allow it to pass through without angular deviation. Green cell 122 imparts an image to the green beam and reflects the green beam back towards surface 125. The green beam passes through surface 125 and is recombined with the reflected red bearm. The combination then passes through 25 surface 123 where it is also recombined with the blue bearn. The combination of the red, green and blue beams then emerges from a~c~ e ]121 in a direction parallel but opposite to arrow 124.
In the above system, the dirr~.~,lll co~llpollents of the light generally pass directly from surface 123 or surface 125 to working face 126, 128 or 130, where a direct passage 30 refers to a passage without reflection. Of course, it is understood that such light may pass ~ , . . .
directly through a lens, without undergoing reflection, and the inclusion of such optical elements as lenses are fillly contemplated by the present invention. Depending on the requirements of the optical designer, a certain subset of the components may undergo a reflection, but preferably not all.
Reflections are mini,.. i~Pd in the present invention because any extra deviations introduce aberrations, and aberrations by mirrors are often twice as bad as those caused by refractive deviations. Of course, the more aberrations, the poorer the image. Therefore, it is r~lled that the number of reflections be minimi7~1 The prism of the present invention may be used as part of an overall projection 10 system, as shown in Fig. 5. In this system, a light source 154, which may be an arc lamp, is collim~ted by a parabolic reflector 155, causing light to be focused and incident on a steering mirror 153. Steering mirror 153, which is located slightly off an optic axis 157, diverges and directs the light to field lens 156, which may be identified as serving a similar purpose to ape~ e 121 (see Fig. 4).
The path of the light within prism 120 is the same as that described before. Of course, the choice of order in which the colors are separated is not limited by that described above. By a suitable choice of filters, the colors could be separated. If band-pass filters are employed, for example, the green beam could be separated first. Moreover, the light need not be separated into 3 colors of red, green and blue. For example, a suitable choice of 20 filters, which may include a plurality of dichroic s..rf~ces, may separate the white light into four or even more beams. When the light emerges from prism 120, it is directed to a projection lens 152, this lens being located on optic axis 157, and finally is projected on projection screen 151.
The present invention has been described in terms of pfer~ d embodiments. The 25 invention, however, is not limited to the emborliment~ depicted and described. Rather, the scope of the invention is defined by the appended claims.
-1~
TECHNICAL FIELD OF THE INVENTION
The present invention is directed to projection prisms, and more particularly to color projection prisms for dispersing and recombining light.
BACKGROUND OF T HE INVENTION
Color di~clwlllent and recombination are important aspects of color projection systems. In these systems, white light is created from, for example, an arc lamp. A prism or other such device is used to disperse the white light into three components: a red beam, a green beam and a blue bearn. These beams may be directed to reflective liquid crystal cells that interfere with and selectively reflect each beam. In other words, the interference imparts an image to each color bearn. More particularly, the reflective liquid crystal cells are often active matrix cells with a switching element for each pixel allowing each pixel to be individually addressed. The colors are recombined, and when projected on a screen form a full color image.
U.S. Patent No. 4,943,154 (1990), discloses a prior art projection system, as shown in Fig. 1. This system comprises a light source 51); a light ll~n~ 59; light valves 61, 62 and 63; a light combiner 64; a proJection lens 65; a drive circuit 67; an input side co~ gelll lens 68; an input side plane mirror 69; a central convergent lens 70; an output side plane mirror 71; and an output side convergent lens 72. The light source 50 comprises a lamp 51, a condenser lens 52, a concave mirror 53, and a heat absorbing filter 54. The lamp 51 radiates a light co..~ g three primary colors of red, green and blue. Rays of the radiant light from the lamp 51 are arranged in approximately parallel rays by the condenser lens 52 and the concave mirror 53. More specifically, the rays of light from the center of a luminous clenlenl 55 in the lamp 51 are tr~n~miltted in parallel to the optic axis 57 by the 25 condenser lens 52. From the light rays passed through the condenser lens 52, infrared rays are elimin~ted by the heat absorbing filter 54. The light rays from the light source 50 are sep~ted into three primary colors of red, green and blue. Red light passes through th -W O 98/07061 PCTrUS97114438 light tr~n~m~ r 59 and enters the red light valve 61. Green light is similarly tr~n~mitte~ to the green light valve 62, and blue light is transmitted to the blue light valve 63.
A light separator 90 is used to disperse the light into colored beams of red, green and blue. Separator 90 is shown having two plates 92 and 94. The tr~n.cmi~sive and reflective 5 properties of these plates are shown in the graphs of Figs. 2(a) and 2(b). Fig. 2(a) is a graph of tr~n~mi~sion (in percent) as a function of wavelength (in nanometers (nm)) for plates 92 and 94, corresponding to curves A and B, respectively. Fig. 2(b) is a graph of reflection (in percent) as a function of wavelength (in nm) for the same plates. In particular, Fig. 2(a) shows that plate 92, corresponding to curve A, has a low tr~n~mi~ivity for blue light but a 10 high tr~n~mi~ivity for green and red. Plate 94, corresponding to curve B, has a low trans-missivity for blue and green light but a high tr~nsmi.~sivity for red. Put another way, and as shown in Fig. 2(b), plate 92 reflects the blue light but transmits green and red. Of the green and red light that remains, plate 94 reflects the green but transmits the red. Thus, the two plates may be used to disperse the light before the light enters light valves 61, 62 and 63.
The light valves 61, 62 and 63 are liquid crystal panels each having matrix electrodes. The drive circuit 67 produces electric signals R, G and B according to a video signal Y to control the transmittance of pixels in respective light valves 61, 62 and 63. The modulated light outputs from the light valves 61, 62 and 63 are then combined into a composite flux of light substantially to reproduce a color picture at the position of the light 20 valve 62. An enlarged image of the color picture is finally projected by the projection lens 65 onto a screen 66.
Light combiner 64 may also be used to disperse the light into the different colors (this system is not shown). In this case, the light disperser/combiner often includes dichroic surfaces such as coated plates of glass or an int~-rn~lly-coated cçm~ntecl prism structure.
25 Coatings used as dichroic snrf~ces are typically thin films.
A disadvantage of coated plates is that such plates can introduce ~ctigm~ti~m in the optical path. Inserting additional non-coated plates may compensate for this defect at the expense of.simpliçity.
Prism structures have many advantages. They are ~ypically rugged, easy to mount,30 and useful for beam superposition applications. They deform less when subjected to stress than coated plates. Coatings used in prisms are resistant to degradation because they are usually sealed within the body of the cube.
Prism structures may also have some disadvantages. One may be a polarization dep~nllen~e of the reflected light arising from the coatings for the interior sllrf~ces. These coatings may be multilayered and reflective. As lihe angle of the plane of the coating to the direction of light moves away from 90~, specltral dirr~.~nces between the polarization components increase. In other words, the reflected light becomes at least partially polarized for some range of wavelengths, referred to as the transition region.
This effect may be seen, e.g., in Fig. 3(a), which shows the cG~ onding curves for 10 transmittance for a short-wave-pass beamsplittler or prism at 45~. In Fig. 3(a), the tr~n~mi.~sion (in percent) is plotted versus wavelength (in nm). The action of the beam-splitter is seen to be dependent on the polarization of the light. S-polarized light, i.e., light which has its electric field perpendicular to the plane of incidence, has a tr~n~mitt~nce curve which is shifted relative to that for p-polarized light, the latter being light which has its 15 electric field parallel to the plane of incidence. The amount of shifting is seen to be roughly 50 nm towards lower wavelengths. Thus, the transition region, in which polarization components may be subject to spectral differences, is about 50 nm wide.
Some beamsplitters have been constructed which reduce the spectral difference between the polarization components. Fig. 3(b) shows plots of wavelength (in nm) versus 20 reflection (in percent) for light of random polarization (*), s-polarization (+), and p-polarization (x) for a blue mirror made by Doctor Optic GmbH, of Vienna, Austria. It is seen that the s-polarization cG~ ,onen~ is shifted from the p-polarization component by about 5 nm. Thus, the transition region, in which polarization components may be subject to spectral dirf~.el-ces, is much smaller and is about 5 nm wide.
The partially polarized light is usually inci~lPnt on the cell which imparts an image to the light. The cell, which may use a scattering lilquid crystal material, may have at least a partial depolarizing effect. This may be Im(lesir~l~le. For example, if the incident beam is highly polarized, and the cell depolarizes that same state of polarization, then the i~Len~ily of the beam passing back through the prism may be ~ e.~ l In extreme cases, the intensity may drop to about half the incident intensity because the beam is not propclly reflected.
This type of alt~ml~tion is generally caused by each of the three cells. The overall effect is to reduce the tr~n.cmi~sion of the prism system. For example, a typical ratio of the 5 amount of light exiting the prism system to that entering is about fifty percent for dichroic surfaces that are oriented 45~ to the direction of the light. For cells that use polarization of the light for their optical action, this polarizing effect can be used to increase their contrast ratio. However, this may severely ~ e the light h~ellsily, perhaps by about sixty percent.
Some solutions have been proposed for the above problems. For example, U.S.
Patent No. 4,969,730 (1990), discloses a prism system with two air gaps. While these air gaps may reduce attenuation, they may produce undesirable "ghost" images.
Accordingly, an object of the invention is to provide an optical prism in which the ratio of the amount of light exiting the prism system to the amount entering is m~xi...i~.l Another object is to provide a prism system for color dispersement and recombination in which dispersement occurs while introducing a minimum of polarization in the dispersed light.
Additional objects and advantages of the invention will be set forth in the des-cription which follows, and in part will be obvious from the description, or may be learned 20 by practice of the invention. The advantages of the invention may be realized and obtained by means of the instr.~ nt~lities and combinations particularly pointed out in the claims.
BRIEF SUMMARY OF THE INVENTION
In one aspect, the present invention is directed to a prism for color tli~p~r~ion and recombination. The prism comprises an a~e~ c for a light beam. The normal to the25 a~ellult; defines an optic axis. A first surface, intersecting the optic axis, is oriented at a first angle to the optic axis. The first angle is greater than 45~. The first surface disperses the light beam into a first con~pol enl and an intermediate component. First, second and third working faces are located along dirre,ell- segment~ of the pel;phel~ of the prism. A
second surface, inte~eclillg the optic axis, and oriented at a second angle to the optic axis, disperses the intermediate component of the ligh1: beam into a second component and a third component. At least one of the first, second or third components passes directly to the first, second or third working faces, respectively, from one of the first or second surfaces.
ImplemPnt~tions include the following features. The prism may further comprise first, second and third cells for hnpa~ g images to the first, second and third components, ,~,i,pe~ilively. The cells may be liquid crystal cells having a plurality of picture elements which change from a more scattering state to a ]ess scattering state upon application of an input such as an electric field. The first and second surfaces of the prism may be coated with multilayer dichroic reflective coatings. Each of the first and second angles to the optic lO axis may be in the range of about 55~ to 85~, and more particularly in the range of about 60~
to 70~, and even more particularly may be about 65~.
In another aspect, the invention is direcled to an system for color dispersion and recombination. The system comprises an apertlure for a light beam. The normal to the al~,.Lul~ defines an optic axis. A first coated glass plate intersects the optic axis and has a 15 surface oriented at a first angle to the optic axis. The first angle is greater than 45~. The surface of the first coated glass plate disperses the light beam into a first component and an interrn~ t~ component. A second coated glass plate intersects the optic axis and has a surface oriented at a second angle to the optic axis. The second coated glass plate ~ p~r~es the int~rrn~ te cc,lllponel,l of the light bearn into a second component and a third 20 component.
In another aspect, the invention is directed to a projection system. The system has a light source, a reflector adjacent the light source for directing the light to a steering mirror and a field lens for collecting light received from the steering mirror. A prism is provided to collect light from the field lens. The prism may be such as described above.
In another aspect, the invention is directed to a prism having at least one working face located along the periphery thereof for color dispersion and recombination. The prism compri.~e~ an ~llule for a light beam, where the normal to the al~c,lu~e defines an optic axis. A plurality of surfaces intersect the optic axis and at least one of the plurality of snrf~ces is oriented at a first angle to the optic axis. The first angle is greater than 45~ and 30 disperses the light beam into a first component and an interme~ te component. The first component passes directly to the working face from one of the plurality of surfaces. The plurality of surfaces includes dichroic surfaces.
An advantage of the invention is that the ratio of the light exiting the prism to the light entering the prism is high because light reflected inside the prism is only weakly 5 polarization dependent.
A further advantage of the invention is that the use of a prism structure makes the system rugged, easy to mount, and useful for beam superposition applications. Prisms deform less when subjected to stress than coated plates. Coatings used in prisms are resistant to degradation because they are usually sealed within the body of the cube.
BRIEF DESCRIPTION OF THE DRAWING(S) The accompanying figures, which are incorporated in and co~ ilule a part of the specification, schem~tically illustrate the invention and, together with the general description given above and the detailed description given below, serve to explain the principles of the invention.
Fig. 1 is a top plan view of a more detailed prior art projection system.
Figs. 2(a) and 2(b) are graphs of tr~n~mi~ivity and reflectivity, respectively, for plates 92 and 94 of Fig. 1.
Figs. 3(a) and 3(b) are graphs showing spectral differences between polarizationcomponents.
Fig. 4 is a top plan view of an embodiment of the present invention.
Fig. 5 is a top plan view of an embodiment of the present invention as used in aprojection system.
DETAILED DESCRIPTION OF THE INVENTION
Referring to Fig. 4, a color projection prism 120 includes an apcll~e 121. Aperture 121 is the area through which the white light enters the prism and through which the color-imaged light exits the prism. It may be as simple as the face of the prism itself, but is usually defined by the a~ Lul~ of the lens. The normal to the plane of aperture 121 generally defines an optic axis of the system. First, second and third reflection cells 122, W O 98/07061 PCTAUSg7/14438 127 and 129 are also provided and are denoted here as green (G) cell 122, blue (B) cell 127 and red (R) cell 129. Such cells, which may be oi the type using nematic curvilinear aligned phases (NCAP) liquid crystal materials or other types, are often used with the color projection prism of the present invention to form a color projection system, but this is not 5 necessary.
An NCAP liquid crystal cell uses a liquiàl crystal material which is ellr~rs~ ted in or dispersed in a col-t~in~ nt medium such as a polymer. Suitable enc~psul~ting media include, but are not limited to, gelatin, polyurethane, polyethylene oxide, polyvinyl pyrrolidone, cellulosic polymers, natural gums, acrylic and methacrylic copolymers, 10 epoxies, polyolefins, vinyl polymers, aqueous :lattices, and the like. In particular, the enc~psl-l~ting medium may be polyvinyl alcohol or a polyurethane latex. The liquid crystal m~t~ri~l may be nematic or operationally nematic, and may have a positive dielectric anisotropy. Alternately, the liquid crystal material may be smectic or chiral nematic. In addition, a pleochroic dye may be dissolved in the liquid crystal material.
Generally, such liquid crystal cells have a ]plurality of picture elements which change from a more sc~ttering state to a less scattering state upon application of an input, such as an electric field.
Prism 120 may be constructed of a number of prism segm~nt~ These prism segment~ have at least some surfaces which are coated with dichroic thin film reflectors such as a multilayer stack of al~ "~ g refractive index m~teri~l~. The precise design of the multilayer stack depends on the requirements of the ~lesigner. The segments are bonded together with an adhesive to form prism 120. In Fig. 4, two coated surfaces are formed:
first surface 123 and second surface 125. The coatings of these sl.rf~es are dichroic. The angle x between surfaces 123 and 125 is generally less than 90~.
White light enters the prism 120 along the direction of arrow 124 and is incident on surface 123 at an angle to the optic axis of greater than 45~. This white light beam may be ge~ d by an arc lamp, for example. A first component of the white light, in particular the blue bearn, is reflected from surface 123 and is directed towards a first working face 126 of the prism, a(ljac~nt to which is blue cell 127. The terrn ".working face" is defined herein as a face on which an active optic elem~nt would be placed or a face through which light may be directed to a cell. First working face, as well as second and third working faces described below, are generally located along dirrelelll portions of the periphery of the prism.
The choice of which color beam is reflected first is dependent on the nature of surface 123 and may be changed according to the preference of the user. Usually either blue or red is reflected first because l) they are nearer to the ends of the spectrum and 2) high and low pass reflectors are easier to form than band pass reflectors. In particular, the coating of surface 123 is a multilayer stack of altçrn~tine refractive index materials, e.g., silicon dioxide with a refractive index of about 1.5 and alumina with a refractive index of about 1.7. The thickness of each layer is designed to reflect substantially all light below a 10 certain wavelength, e.g., for blue, 490 nm is used. For red light, they are designed to reflect substantially all light above a certain wavelength, e.g., 570 nm. The reflection from surface 123 may cause some disparity between the s-polarized and p-polarized portions of the blue bearn, as described above in connection with Fig. 3(a). However, the closer surface 123 is to being 90~ to the optic axis, the less this difference will be.
Surface 123 is designed to increase the angle to the optic axis. It is oriented at a first angle to the optic axis of greater than 45~. This first angle may be in the range of about 55~
to 85~, and can be about 65~. In part, as this angle is closer to norrnal than, for example, a 45~ angle, the amount of polarization introduced into the beam, in this case the blue beam, is less than in prior systems.
Blue cell 127 imparts an image to the blue beam and reflects the same back towards surface 123. Blue cell 127 may have a partial depol~n~ing effect on the blue beam, as described above. However, in the present embodiment, the blue beam leaves surface 123 with less difference between its s- and p-polarizations (because of the angle to the optic axis) than, for example, if the angle to the optic axis was 45~. Therefore, there is less 25 chance of the blue beam being transmitted by surface 123 on its return.
The blue beam emerges from blue cell 127, passes through the first working face 126 of the prism, and is directed towards surface 123. Surface 123 reflects the blue beam back in a direction parallel but opposite to arrow 124.
Light transmitted through surface 123 is composed of an int~nne~ te component:
30 the white light minus the blue beam. This light is incident on surface 125 at an angle to the optic axis which is again greater than 45~. This surface disperses the intermediate component into second and third components, i.e., into a reflected red beam and a transmitted green beam.
A polarization effect similar to that above occurs for the red beam. The reflection S from surface 125 partially polarizes the red beam. However, surface 125 provides an angle to the optic axis which is closer to normal, i.e., 90'', than in prior systems. Therefore, for the same reasons as above, surface 125 introduces less of a dirr~lcnce between the polarizations of the beam, i.e., less polarization dep~n~ence, than if the angle to the optic axis were, for example, 45~.
Surface 125 reflects the red beam towards, a second working face 128 and red cell 129, and transmits the rem~ining light, the green beam, towards a third working face 130 and green cell 122. Red cell 129 imparts an ima;ge to the red beam and reflects the same back towards surface 125. Surface 125 directs the beam in a direction parallel but opposite to arrow 124. Any light is which ~ sllliLled lthrough surface 125 is lost by multiple 15 reflection and scattering. Any depolarizing effects of red cell 129 will produce, at most, only minim~l effects on the red beam because of the dichroic surface's weak polarization depçn~n.~e The green beam lcprcsellts the rern~in-lçr of the light after the blue and red beams are removed by reflections from surfaces 123 and 125. The green beam is transmitted 20 directly through the prism with little change in ~mgle and is incident on green cell 122 because the dichroic surfaces do not reflect green light. Rather, they allow it to pass through without angular deviation. Green cell 122 imparts an image to the green beam and reflects the green beam back towards surface 125. The green beam passes through surface 125 and is recombined with the reflected red bearm. The combination then passes through 25 surface 123 where it is also recombined with the blue bearn. The combination of the red, green and blue beams then emerges from a~c~ e ]121 in a direction parallel but opposite to arrow 124.
In the above system, the dirr~.~,lll co~llpollents of the light generally pass directly from surface 123 or surface 125 to working face 126, 128 or 130, where a direct passage 30 refers to a passage without reflection. Of course, it is understood that such light may pass ~ , . . .
directly through a lens, without undergoing reflection, and the inclusion of such optical elements as lenses are fillly contemplated by the present invention. Depending on the requirements of the optical designer, a certain subset of the components may undergo a reflection, but preferably not all.
Reflections are mini,.. i~Pd in the present invention because any extra deviations introduce aberrations, and aberrations by mirrors are often twice as bad as those caused by refractive deviations. Of course, the more aberrations, the poorer the image. Therefore, it is r~lled that the number of reflections be minimi7~1 The prism of the present invention may be used as part of an overall projection 10 system, as shown in Fig. 5. In this system, a light source 154, which may be an arc lamp, is collim~ted by a parabolic reflector 155, causing light to be focused and incident on a steering mirror 153. Steering mirror 153, which is located slightly off an optic axis 157, diverges and directs the light to field lens 156, which may be identified as serving a similar purpose to ape~ e 121 (see Fig. 4).
The path of the light within prism 120 is the same as that described before. Of course, the choice of order in which the colors are separated is not limited by that described above. By a suitable choice of filters, the colors could be separated. If band-pass filters are employed, for example, the green beam could be separated first. Moreover, the light need not be separated into 3 colors of red, green and blue. For example, a suitable choice of 20 filters, which may include a plurality of dichroic s..rf~ces, may separate the white light into four or even more beams. When the light emerges from prism 120, it is directed to a projection lens 152, this lens being located on optic axis 157, and finally is projected on projection screen 151.
The present invention has been described in terms of pfer~ d embodiments. The 25 invention, however, is not limited to the emborliment~ depicted and described. Rather, the scope of the invention is defined by the appended claims.
-1~
Claims (17)
1. A prism for color dispersion and recombination, comprising:
an aperture for a light beam, the normal to said aperture defining an optic axis;
a first surface, intersecting the optic axis, oriented at a first angle to the optic axis, said first angle greater than 45° for dispersing the light beam into a first component and an intermediate component;
first, second and third working faces located along different segments of a periphery of the prism;
a second surface, intersecting the optic axis, oriented at a second angle to theoptic axis, for dispersing the intermediate component of the light beam into a second component and a third component; and such that at least one of the first, second or third components passes directly to the first, second or third working faces, respectively, from one of the first or second surfaces.
an aperture for a light beam, the normal to said aperture defining an optic axis;
a first surface, intersecting the optic axis, oriented at a first angle to the optic axis, said first angle greater than 45° for dispersing the light beam into a first component and an intermediate component;
first, second and third working faces located along different segments of a periphery of the prism;
a second surface, intersecting the optic axis, oriented at a second angle to theoptic axis, for dispersing the intermediate component of the light beam into a second component and a third component; and such that at least one of the first, second or third components passes directly to the first, second or third working faces, respectively, from one of the first or second surfaces.
2. The prism of claim 1, further comprising first, second and third cells for imparting images to the first, second and third components, respectively.
3. The prism of claim 2, wherein said cells are liquid crystal display cells having a plurality of picture elements which change from a more scattering state to a less scattering state upon application of an input.
4. The prism of claim 1, wherein said first and second surfaces are coated with multilayer dichroic reflective coatings.
5. The prism of claim 1, wherein the first angle is in the range of about 55° to 85°.
6. The prism of claim 5, wherein the first angle is in the range of about 60° to 70°.
7. The prism of claim 6, wherein the first angle is about 65°.
8. The prism of claim 1, wherein the second angle is in the range of about 55° to 85°.
9. The prism of claim 8, wherein the second angle is in the range of about 60° to 70°.
10. The prism of claim 9, wherein the second angle is about 65°.
11. A system for color dispersion and recombination, comprising:
an aperture for a light beam, the normal to said aperture defining an optic axis;
a first coated glass plate intersecting the optic axis and having a surface oriented at a first angle to the optic axis, said first angle greater than 45° for dispersing the light beam into a first component and an intermediate component;
first, second and third working faces associated with different segments along the periphery of the system;
a second coated glass plate intersecting the optic axis and having a surface oriented at a second angle to the optic axis, for dispersing the intermediate component of the light beam into a second component and a third component; and such that at least one of the first, second or third components passes directly to the first, second or third working faces, respectively, from one of the first or second coated glass plates.
an aperture for a light beam, the normal to said aperture defining an optic axis;
a first coated glass plate intersecting the optic axis and having a surface oriented at a first angle to the optic axis, said first angle greater than 45° for dispersing the light beam into a first component and an intermediate component;
first, second and third working faces associated with different segments along the periphery of the system;
a second coated glass plate intersecting the optic axis and having a surface oriented at a second angle to the optic axis, for dispersing the intermediate component of the light beam into a second component and a third component; and such that at least one of the first, second or third components passes directly to the first, second or third working faces, respectively, from one of the first or second coated glass plates.
12. The system of claim 11, further comprising first, second and third color cells for imparting images to the first, second and third components, respectively.
13. The system of claim 12, wherein said cells are liquid crystal display cells having a plurality of picture elements which change from a more scattering state to a less scattering state upon application of an input.
14. A projection system, comprising:
a light source;
a reflector adjacent said light source for directing the light to a steering mirror;
a field lens for collecting light received from said steering mirror;
a prism for collecting light from said field lens, the prism including:
(i) an aperture for the light, the normal to said aperture defining an optic axis, (ii) a first surface, intersecting the optic axis, oriented at a first angle to the optic axis, said first angle greater than 45° for dispersing the light beam into a first component and an intermediate component, and (iii) a second surface, intersecting the optic axis, oriented at a second angle to the optic axis, for dispersing the intermediate component of the light beam into a second component and a third component;
first, second and third cells for imparting images to the first, second and third components, respectively; and such that at least one of the first, second or third components passes directly to the first, second or third cells, respectively, from one of the first or second surfaces.
a light source;
a reflector adjacent said light source for directing the light to a steering mirror;
a field lens for collecting light received from said steering mirror;
a prism for collecting light from said field lens, the prism including:
(i) an aperture for the light, the normal to said aperture defining an optic axis, (ii) a first surface, intersecting the optic axis, oriented at a first angle to the optic axis, said first angle greater than 45° for dispersing the light beam into a first component and an intermediate component, and (iii) a second surface, intersecting the optic axis, oriented at a second angle to the optic axis, for dispersing the intermediate component of the light beam into a second component and a third component;
first, second and third cells for imparting images to the first, second and third components, respectively; and such that at least one of the first, second or third components passes directly to the first, second or third cells, respectively, from one of the first or second surfaces.
15. The projection system of claim 14, wherein said cells are liquid crystal display cells having a plurality of picture elements which change from a more scattering state to a less scattering state upon application of an input.
16. A prism having at least one working face located along the periphery thereof for color dispersion and recombination, comprising:
an aperture for a light beam, the normal to said aperture defining an optic axis;
a plurality of surfaces intersecting the optic axis, at least one of said plurality of surfaces oriented at a first angle to the optic axis, said first angle greater than 45°
for dispersing the light beam into a first component and an intermediate component;
and such that the first component passes directly to the working face from one of the plurality of surfaces.
an aperture for a light beam, the normal to said aperture defining an optic axis;
a plurality of surfaces intersecting the optic axis, at least one of said plurality of surfaces oriented at a first angle to the optic axis, said first angle greater than 45°
for dispersing the light beam into a first component and an intermediate component;
and such that the first component passes directly to the working face from one of the plurality of surfaces.
17. The prism of claim 16, wherein said plurality of surfaces include dichroic surfaces.
Applications Claiming Priority (7)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US69989296A | 1996-08-16 | 1996-08-16 | |
| US08/699,892 | 1996-08-16 | ||
| US81291497A | 1997-03-10 | 1997-03-10 | |
| US08/812,914 | 1997-03-10 | ||
| US08/869,308 | 1997-06-04 | ||
| US08/869,308 US6082863A (en) | 1996-08-16 | 1997-06-04 | Color projection prism |
| PCT/US1997/014438 WO1998007061A1 (en) | 1996-08-16 | 1997-08-15 | Color projection prism |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA2263643A1 true CA2263643A1 (en) | 1998-02-19 |
Family
ID=27418697
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA002263643A Abandoned CA2263643A1 (en) | 1996-08-16 | 1997-08-15 | Color projection prism |
Country Status (5)
| Country | Link |
|---|---|
| US (1) | US6082863A (en) |
| EP (1) | EP0919008A1 (en) |
| JP (1) | JP2001523351A (en) |
| CA (1) | CA2263643A1 (en) |
| WO (1) | WO1998007061A1 (en) |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6010221A (en) * | 1997-05-22 | 2000-01-04 | Nikon Corporation | Projection type display apparatus |
| US5951135A (en) * | 1997-10-14 | 1999-09-14 | Raychem Corporation | Color image projection system |
| DE19842216A1 (en) * | 1998-09-15 | 2000-04-06 | Agfa Gevaert Ag | Device and method for splitting or combining light |
| JP2000227578A (en) * | 1998-11-12 | 2000-08-15 | Fujitsu Ltd | Projection type display device |
| US6215597B1 (en) * | 1999-11-17 | 2001-04-10 | Duncan Technologies, Inc. | Apparatus for forming a plurality of subimages having different characteristics |
| US20030218590A1 (en) * | 2002-05-23 | 2003-11-27 | Kiser David K. | Optics engine having multi-array spatial light modulating device and method of operation |
| US6947020B2 (en) | 2002-05-23 | 2005-09-20 | Oregonlabs, Llc | Multi-array spatial light modulating devices and methods of fabrication |
| US20040108973A1 (en) * | 2002-12-10 | 2004-06-10 | Kiser David K. | Apparatus for generating a number of color light components |
| US20040109138A1 (en) * | 2002-12-10 | 2004-06-10 | Kiser David K. | Apparatus for generating a number of color light components |
| US20040109139A1 (en) * | 2002-12-10 | 2004-06-10 | Kiser David K. | Apparatus for combining a number of images into a single image |
| US20040109140A1 (en) * | 2002-12-10 | 2004-06-10 | Kiser David K. | Apparatus for combining a number of images into a single image |
| JP4796443B2 (en) * | 2006-06-08 | 2011-10-19 | シスメックス株式会社 | Reagent for sample analysis, reagent kit for sample analysis, and sample analysis method |
| JP4914656B2 (en) | 2006-06-26 | 2012-04-11 | シスメックス株式会社 | Reagent for sample analysis, reagent kit for sample analysis, and sample analysis method |
| KR102262215B1 (en) * | 2014-09-01 | 2021-06-08 | 삼성전자주식회사 | Backlight unit and holographic display having the same |
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| GB1401476A (en) * | 1972-09-19 | 1975-07-16 | Rank Organisation Ltd | Optical beam splitting systems |
| US4715684A (en) * | 1984-06-20 | 1987-12-29 | Hughes Aircraft Company | Optical system for three color liquid crystal light valve image projection system |
| US4687301A (en) * | 1985-07-12 | 1987-08-18 | Hughes Aircraft Company | Full-color projector system with a tricolor-separating prism |
| US4726662A (en) * | 1985-09-24 | 1988-02-23 | Talig Corporation | Display including a prismatic lens system or a prismatic reflective system |
| US4913528A (en) * | 1987-05-30 | 1990-04-03 | Pioneer Electronic Corporation | Optical prism, and projection television set using same |
| JPS63311892A (en) * | 1987-06-12 | 1988-12-20 | Sharp Corp | Liquid crystal projection device |
| US4943155A (en) * | 1987-12-22 | 1990-07-24 | Hughes Aircraft Company | Color projection system with a color correction wedge |
| US5105265A (en) * | 1988-01-25 | 1992-04-14 | Casio Computer Co., Ltd. | Projector apparatus having three liquid crystal panels |
| US4943154A (en) * | 1988-02-25 | 1990-07-24 | Matsushita Electric Industrial Co., Ltd. | Projection display apparatus |
| JPH0274903A (en) * | 1988-09-12 | 1990-03-14 | Seiko Epson Corp | Dichroic optical element and projection type display device |
| US5150232A (en) * | 1988-10-04 | 1992-09-22 | Asahi Glass Company Ltd. | Active matrix liquid crystal display element and projection type active matrix liquid crystal display device |
| NL8802517A (en) * | 1988-10-13 | 1990-05-01 | Philips Nv | IMAGE PROJECTION DEVICE. |
| JPH02153336A (en) * | 1988-12-05 | 1990-06-13 | Sharp Corp | Projection type liquid crystal display device |
| FR2642927B1 (en) * | 1989-02-07 | 1993-12-24 | Thomson Csf | HIGH DEFINITION, COLOR DISPLAY DEVICE |
| NL8902205A (en) * | 1989-09-01 | 1991-04-02 | Philips Nv | PROJECTION SYSTEM. |
| JPH03288124A (en) * | 1990-04-04 | 1991-12-18 | Victor Co Of Japan Ltd | Optical system of color image display device |
| JP2985906B2 (en) * | 1991-07-17 | 1999-12-06 | 日本ビクター株式会社 | Projection display device |
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| US5648860A (en) * | 1992-10-09 | 1997-07-15 | Ag Technology Co., Ltd. | Projection type color liquid crystal optical apparatus |
| US5309188A (en) * | 1993-05-21 | 1994-05-03 | David Sarnoff Research Center, Inc. | Coupling prism assembly and projection system using the same |
| US5398081A (en) * | 1993-06-07 | 1995-03-14 | Raychem Corporation | Apparatus for projecting colored images |
| WO1996013943A1 (en) * | 1994-11-01 | 1996-05-09 | Raychem Corporation | Hole eliminator for lamp with reflector |
| EP0722253A3 (en) * | 1995-01-10 | 1996-10-30 | Ibm | Arrangements for projection displays employing reflective light valves |
| US5621486A (en) * | 1995-06-22 | 1997-04-15 | International Business Machines Corporation | Efficient optical system for a high resolution projection display employing reflection light valves |
-
1997
- 1997-06-04 US US08/869,308 patent/US6082863A/en not_active Expired - Fee Related
- 1997-08-15 CA CA002263643A patent/CA2263643A1/en not_active Abandoned
- 1997-08-15 EP EP97937290A patent/EP0919008A1/en not_active Withdrawn
- 1997-08-15 JP JP51008098A patent/JP2001523351A/en active Pending
- 1997-08-15 WO PCT/US1997/014438 patent/WO1998007061A1/en not_active Application Discontinuation
Also Published As
| Publication number | Publication date |
|---|---|
| JP2001523351A (en) | 2001-11-20 |
| EP0919008A1 (en) | 1999-06-02 |
| WO1998007061A1 (en) | 1998-02-19 |
| US6082863A (en) | 2000-07-04 |
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