Abstract:
A system and method for separating and combining three spectrums of light has a polarizing beamsplitter, an input retarder or polarizer located adjacent a first side of the polarizing beamsplitter, a spacer that can also be a splitter located adjacent a second side of the polarizing beamsplitter and a dichroic beamsplitter located adjacent a third side of the polarizing beamsplitter.

Description:
CROSS REFERENCE TO RELATED APPLICATION  
       [0001]    The present application is a divisional of U.S. Ser. No. 09/291,752, filed Apr. 14, 1999. 
     
    
     
       FIELD AND BACKGROUND OF THE INVENTION  
         [0002]    The present invention relates to a spectral light division and recombination configuration as well as a process for the spectrally selective modulation of light.  
           [0003]    Definitions:  
                                       Light,   light with maximum energy in the spectral range 380       visible light:   nm - 720 nm       red light:   light with maximum energy in the spectral range 580           nm - 780 nm, in particular in the spectral range 600           nm - 680 nm       green light:   light with maximum energy in the spectral range 490           nm - 605 nm, in particular in the spectral range 500           nm - 600 nm       blue light:   light with maximum energy in the spectral range 380           nm - 510 nm, in particular in the spectral range 420           nm - 500 nm       yellow light:   light with maximum energy in the spectral range 475           nm - 605 nm, in particular at 482 nm ± 3 nm       white light:   light with red, blue and green light components       linearly polarized   light whose electric field vector oscillates in a plane.       light:       reflective light   image producing element which operates in reflection,       valve:   for example on the basis of liquid crystals with           polarization rotation (rLCD).       bright state rLCD:   With reflection of light on pixels of the reflective light           valve, the polarization is rotated by an odd-numbered           multiple of 90°.       dark state rLCD:   With reflection of light on pixels of the reflective light           valve the polarization is maintained.       F number:   Variable describing the angle opening-out of an           illumination optics system. It is given by the           reciprocal value of the twofold numerical aperture           NA, wherein NA = n sin α, and n is the refractive           index of the medium, α one half of the aperture angle           of the illumination cone. Therefore, the smaller the F           number, the wider the aperture angle. Typical F           numbers are in the range from 5 to 2.5; F numbers of           2 down to 1.4 are also used.                  
 
           [0004]    Optical light division and recombination configurations are used primarily in projectors in order to divide white light into red, green and blue light or to recombine the latter in order to form white light.  
           [0005]    It is known to divide, by means of such a configuration in projection apparatus, white light into light of said three spectral ranges, to modulate each via light valves operating in transmission, such as in particular LCD light valves, to be image producing and subsequently to recombine the modulated light of the three spectra to form an imaging beam. The light valves, as the image-producing structural elements, comprise a multiplicity of individually drivable pixels. Their number yields therein the resolution according to the formats EVGA, SVGA, EGA, XGA, etc. When using light valves operating in transmission a lower limitation of the pixel size exists which can only be overcome with difficulty due to the printed conductor tracks and the drive electronics. In addition, with a decrease of the pixel size, the optical aperture per pixel decreases.  
           [0006]    The present invention, in contrast, relates to a process for the spectrally selective modulation of light by means of light valves operating in reflection. The optical light division and recombination configuration, to which the invention relates further, consequently is preferably used in combination with light valves operating in reflection for the formation of a configuration according to the invention for the optical light division, spectrally selective modulation and subsequent recombination.  
           [0007]    When using light valves operating in reflection the restrictions regarding light valves operating in transmission cease to apply. Controlled light valves operating in reflection do not rotate in the dark state of a pixel the polarization of the light reflected thereon with respect to that of the incident light, while in the bright state the polarization of the reflected light is rotated by 90° with respect to the polarization of the incident light.  
           [0008]    In a process of the above described type, or an optical light division and recombination configuration of the above type, it is necessary, on the one hand, to ensure that white light is divided into light of said three spectra, and light of said three spectra, after reflective modulation and modulation-dependent or drive-dependent polarization rotation, is combined to white light, therewith, on the other hand, light from pixels operated in the bright state should be recombined to form a first light beam—the imaging beam—, light of pixels operated in the dark state not emerging on said beam, therewith in particular, should be recombined to form a second light beam —the dark reflection beam, wherein both said beams should leave the light division and recombination configuration in different directions. The first is preferably, and in view of the use on a projection arrangement, guided to its imaging optics system; the latter should, for example or preferably, be guided back to the white light source.  
           [0009]    Previously known solutions for processes, and for optical light division and recombination configurations of the above type, can be divided into formulations using glass plates and formulations with solid glass bodies. In both cases, again, geometries can be differentiated which operate on the basis of angular beam deflections of 45° or 90°, and those operating on the basis of angles which differ from beam deflections of 45° or 90°.  
           [0010]    Configurations realized with angles of 45° are described, for example, in DE 40 33 842, which describes a rectangular parallelepiped structural element composed of discrete prisms with dichroic layers. Such a structural element is customarily referred to as an X-cube. With respect to such X-cubes and their uses, further reference is made to U.S. Pat. No. 2,737,076, U.S. Pat.No. 2,754,718, JP 7-109443, U.S. Pat. No. 5,098,183, EP A 0 359 461, as well as WO98/20383 by the same applicant as the present application.  
           [0011]    Angles deviating from 45° as well as solid glass bodies are used, for example, according to U.S. Pat. No. 3,203,039 which lead to configurations generally known as “Philips prisms”.  
           [0012]    Furthermore are known diverse combinations of dichroic splitter configuration plates —spectrally selective splitters —combined with prism configurations, thus, for example, from U.S. Pat. No. 3,945,034, or combined with X-cubes.  
           [0013]    For a realization form known under the designation 3PBS system, reference can be made to R. L. Melcher “High Information—Content Protection Display Based on Reflective LC on Silicon Light Valves”, SID 98 Digest, pp. 25-28, 1998.  
           [0014]    As has been mentioned, in spectral light division and recombination light of different polarization states must be handled after the reflective modulation.  
           [0015]    An X-cube configuration, if appropriate in combination with a polarization-selective beam-splitting configuration, such as is described for example in said WO98/20383, presupposes dichroic layer systems, which have minimum polarization effects since they are acted upon by light of different polarization, which should only be handled with spectral selectivity.  
           [0016]    In this respect reference is made to A. Thelen “Nonpolarising interference films inside a glass cube”, Appl. Optics Vol. 15, No. 12, December 1976.  
           [0017]    Regarding problems concerning the dark-state transmission characteristics of light division and recombination techniques operating with reflective light valves, reference is made to A. E. Rosenbluth et al.: “Contrast properties of reflective liquid crystal light valves in projection displays”, IBM Journal of Research and Development, Vol. 42, No. 3/4 May/July, pp. 359-383, 1998. A solution of these problems is only possible with considerable design and fabrication expenditures.  
           [0018]    Realizations according to the above listed Philips prisms or similar approaches are based, as a rule, on total internal reflection at one or several air gaps. Apart from the difficulties in the production of such air gaps, the total reflection is the limiting factor for the F numbers possible in practice. In addition, such systems are very sensitive with respect to residual reflections which, for example, can occur if the transitions from one optical refractive index to the other are not optimally matched and which as ghosts can ‘haunt’ the system under diverse directions.  
           [0019]    In the case of approaches toward a solution using solid glass bodies, the problem of the mechanical birefringence in the glass or the substrate material must be taken into consideration whereby the polarization of the light is rotated uncontrollably with stochastic distribution. A contrast loss is generated in the process which is not constant over the illuminated surface.  
           [0020]    Structural parts in which dichroic plates in the imaging ray path are used, are, on the other hand, afflicted with the problem that an astigmatism is generated through the plates. The high requirements made of the planity of such substrates places limits on the transition to thinner substrates in which this astigmatism would become negligibly small.  
         SUMMARY OF THE INVENTION  
         [0021]    The present invention is based on the task of proposing a configuration as well as a process of the above described type, by means of which it becomes possible to combine in a driven state (bright state) of the light valves the recombined light with maximum intensity in a first beam while it emerges on this beam with minimum intensity if it originates from the light valves in the other driven state (dark state).  
           [0022]    Further, a high angle acceptance is to be realized, i.e. low F numbers are to be possible.  
           [0023]    This task is solved through the configuration and the processes of the above stated type, which are distinguished according to the claims.  
           [0024]    By using polarization-selective beam division and recombination it becomes possible to divide the recombined light as a function of the driven or modulation state of the light valves, i.e. to form an imaging beam from light of valves which are operated in the one modulation state, the bright state. When used in a projection apparatus, on the one hand, an imaging beam of light with high intensity is obtained, which is reflected on the valves or their pixels in the bright state, and, on the other hand, preferably a further beam of light reflected on the pixels in the dark state. The latter is preferably directed to the illumination source.  
           [0025]    Preferred embodiments of the configuration as well as of said process are specified in the corresponding dependent claims.  
           [0026]    The present invention relates furthermore to a projection arrangement with said optical light division and recombination configuration according to still further claims. 
       
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0027]    In the following, the invention will be explained by example with reference to Figures. Therein depict:  
         [0028]    [0028]FIG. 1 schematically a configuration according to the invention toward an explanation of the process according to the invention,  
         [0029]    [0029]FIG. 2 schematically a first embodiment of the configuration according to the invention operating after the inventive process,  
         [0030]    [0030]FIG. 3 in detail a configuration according to the invention which operates after the process according to the invention, in preferred embodiment,  
         [0031]    [0031]FIG. 4 by example the transmission behavior of a spectrally selective layer system for s-polarized and p-polarized light, used for example in the approach according to the invention,  
         [0032]    [0032]FIG. 5 the transmission behavior of a polarization-selective layer system, such as used, for example, for s-or p-polarized light,  
         [0033]    [0033]FIG. 6 the ray path for green light in the process according to the invention, in a representation according to FIG. 2,  
         [0034]    [0034]FIG. 7 in a representation analogous to FIG. 6 the ray path realized according to the invention for blue light,  
         [0035]    [0035]FIG. 8 in analogy to the representations according to FIGS. 6 and 7 the ray path realized according to the invention for red light,  
         [0036]    [0036]FIG. 9 a further embodiment of a configuration according to the invention, in plate embodiment in part,  
         [0037]    [0037]FIG. 10 a further embodiment of the configuration according to the invention which differs from beam deflections of 45° or 90° angles,  
         [0038]    [0038]FIG. 11 in a representation analogous to FIG. 10 the same embodiment with respect to difference from angles of 45°, in plate embodiment in part. 
     
    
     DESCRIPTION OF THE PREFERRED EMBODIMENTS  
       [0039]    The fundamental structure and function of the configuration according to the invention or the process according to the invention will be explained with reference to FIG. 1.  
         [0040]    White light L w  is directed with spectrally selective polarization, for example for red light (R) of polarization P 0 , for blue light (B), P 0 , and, in this respect rotated by 90°, for example for green light (G), P 90,  onto a polarization-selective splitter configuration  1 . The spectrally selective polarization in P 0,  for example for red, Δλ 2 , and blue, Δλ 1 , or P 90  for green light, Δλ 3 , is obtained through an additional preceding optical element, not shown in FIG. 1, for example through a film laminate such as is described in U.S. Pat. No. 5,751,384. In this respect this document is declared to be an integrated component of the present specification as an example of the realization of spectrally selective polarization.  
         [0041]    On the polarization-selective splitter configuration  1  light of polarization P 90  is transmitted into a first direction I, light of polarization P 0 is reflected into a second direction II.  
         [0042]    Succeeding the polarization-selective splitter configuration  1  in the first direction I is a light valve  3   a  operating in reflection.  
         [0043]    Succeeding the polarization-selective splitter configuration in the second direction II a spectrally selective splitter configuration  5  is provided. The latter splits the light incident in the second direction II of the two spectra Δλ 1 , Δλ 2 still polarized with P 0 , into a third III and fourth IV direction, but now represented spectrally selectively with Δλ 1 , Δλ 2 .  
         [0044]    Under the broadest aspect of the present invention, the third—III —and fourth—IV—directions, not needing to be parallel, correspond to the second II and first directions I. It is not mandatory that a configuration based on 45° of the selective splitter configurations  1 ,  5  is realized.  
         [0045]    Succeeding the spectrally selective splitter configuration  5  in the third III and fourth IV directions is provided one light valve  3   b  or  3   c  each, operating in reflection.  
         [0046]    The light L w , now divided polarization-selectively as well as also spectrally selectively, is reflected on said light valves  3  operating in reflection.  
         [0047]    The course of the reflected light is represented in FIG. 1 with solid arrow tips or arrows, alternatively.  
         [0048]    From the two light valves  3   b  and  3   c  succeeding the spectrally selective splitter configuration  5  the light in the configuration according to the FIG. 1 is correspondingly reflected in the third III and fourth IV directions. However, dependent on the operating state of said light valves or their pixels, this takes place still with polarization P 0 —dark state—or rotated to polarization P 90  —bright state.  
         [0049]    Consequently, from the second direction impinges onto the polarization-selective splitter configuration  1  light of the two spectral ranges Δλ 1 and Δλ 2 after recombination on the spectrally selective splitter configuration  5 , but, depending on the operating state of said light valve pixels, with the polarization P 0 or P 90  independently of the spectrum.  
         [0050]    Analogously, the light incident on light valve  3   a  of the spectral range Δλ 3 , depending on the operating state of its pixels still in polarization P 90  or with polarization P 0 , is reflected in the first direction I and is incident on the polarization-selective splitter configuration  1 . The light of the three spectra Δμ 1 , Δλ 2 , Δλ 3  is polatization-selectively recombined on the polarization-selective splitter configuration  1 :  
         [0051]    Light of the spectral range Δλ 3 , in the bright state of the pixels of light valve  3   a  rotated to polarization P 0 , due to the effect of the polarization-selective splitter configuration  1 , in analogy to its effect on incident light, emerges in the second direction II.  
         [0052]    Light of the two spectral ranges Δλ 1  and Δλ 2  impinges from the second direction onto the polarization-selective splitter configuration  1 , in the bright state of the corresponding pixels rotated into polarization P 90  on light valves  3   b  and  3   c , and propagated in the second direction II: an imaging beam A is formed in said second direction II with light of the three spectra modulated through the associated light valve pixels in the bright state H.  
         [0053]    Light of spectral range Δλ 3  in the first direction I, thus reflected from light valve  3   a , in the dark operation state of the associated pixels, is incident with unchanged polarization P 90  on the polarization-selective splitter configuration  1  and emerges in the first direction I.  
         [0054]    Light from the second direction II with polarization P 90 , such as is generated through the dark state of the associated pixels on light valves  3   b  and  3   c , also emerges in the first direction I from the polarization- selective configuration I: a second beam B with light of the three spectra is formed, reflected on the light valves with the driving of the associated pixels into the dark state D.  
         [0055]    According to FIG. 1 the configurations  1  and  5 , with respect to the light entry and the spectral exits at the light valves, when viewed as a black box, form a spectrally selective division and recombination unit.  
         [0056]    In FIG. 2 is shown the fundamental structure of the configuration operating according to FIG. 1, and here also, as preferred, pairwise parallelism of the four directions I-IV is realized. The structural parts already explained in conjunction with FIG. 1 carry the same reference symbols in FIG. 2.  
         [0057]    In FIG. 3 a preferred embodiment of a light division and recombination configuration operating after the process according to the invention is depicted together with the light valves preferably combined with the configuration as well as of parts such as are preferably provided in realizing a projection arrangement according to the invention.  
         [0058]    The incident white light L′ w  is polarized under P 0 . The generation of such light by means of polarizers and/or polarization conversion systems is generally known.  
         [0059]    A spectrally selective polarization rotator  10  now has the task of rotating the polarization of a spectral range of the visible light L w  relative to the other two by 90°, P 90  . The rotator can comprise, for example, a laminate of birefringent films, such as, as stated, is described in U.S. Pat. No. 5,751,384. Therewith the white light L w , according to FIG. 1, is available.  
         [0060]    L w  is incident on the entry face  12  of the configuration according to the invention, preferably substantially perpendicularly, as shown. Depending on whether or not the polarization rotator  10  is disposed directly on face  12 , it requires a corresponding refractive index matching layer system or an antireflection layer system (not shown) on rotator  10  and/or on face  12 .  
         [0061]    The light L w  passes through the substrate material of the polarization-selective splitter configuration  15  which, according to FIG. 3, is preferably square in cross section. As the substrate material, preferably for both sub-bodies bilaterally of a diagonal face F, identical material, preferably glass, is used. The refractive index of the substrate material on both sides of face F should as much as possible be identical. The optical properties of the substrate material are also one of the determinants of the spectral characteristic of the polarization-selective splitter configuration  15 . Essential is further that the material absorbs little light, in particular in the blue spectral range Δλ B . The optical design of the polarization-selective layer system  17  is simple in face F if the refractive index of the substrate material is high. Therefore SF2 material is, for example, suitable which has an index of refraction of n=1.65. To be taken into consideration are also the birefringent properties of the substrate material.  
         [0062]    Light L w  of the one polarization P 0  which, with respect to the splitter configuration  15 , is also denoted as s-polarization, should, as much as possible, be reflected completely on layer system  17 , while light of the other polarization P 90 , which, with respect to the splitter configuration  15 , is also denoted as p-polarization, should, as much as possible, be transmitted completely. A wide angle acceptance is, furthermore, essential if the configuration according to the invention, as preferred, also be used for divergent white light illumination arrangements. These have typically an angle of aperture of α=±12° or more. If, for example, a known MacNeille polarizer is used (see, for example, H. A. MacLeod “Thin Film Optical Filters”, Second Edition, pp. 328-332, Adam Hilger, 1986), the angle dependence for reflection in s-polarization does not present a problem while the p-transmission has a strong angle dependence. With an illumination aperture angle α of the above order of magnitude typically a loss of approximately 15% in this transmission results.  
         [0063]    Of L w  the spectral range Δλ R  and Δλ B in s-polarization is incident on layer system  17  and completely reflected on it in the second direction II. The third spectral range Δλ G in p-polarization is transmitted in the first direction I. Thus, as already explained, through the combination of the spectrally selective polarization rotator  10  as well as of the polarization-selective splitter  15  a spectral range separation takes place on the basis of the polarization criterion. It should be noted that the polarization rotator  10  has substantially no angle dependence and that the polarization-selective splitter  15  can be optimized such that it hardly has any wavelength dependence. It is therewith attained that the system has substantially no undesirable coloration effects which can be traced to angle dependencies.  
         [0064]    Light of spectral ranges Δλ B and Δλ R  propagating in direction II enters a spectrally selective splitter  16 . If the configuration according to the invention is to be structured modularly, then the rectangular parallelepipeds of configurations  15  and  16  are each separate parts and, in any case, an interfacial surface  14  results. It is therefore entirely possible to realize the configurations  15 ,  16  integrally without an interfacial surface  14 . If on the interfacial surface  14  an air gap is provided, it is of advantage to provide on the one and/or on the other of faces  14   a ,  14   b  an antireflection coating.  
         [0065]    In the case of direct contacting of the configurations  15 ,  16  free of air gap, an intermediate layer can be of advantage for the matching of the refractive indices of the two materials on the one and/or the other face  14   a ,  14   b.    
         [0066]    The dichroic or spectrally selective layer system  18  of the spectrally selective splitter configuration  16  is, as shown, again laid out preferably with a 45° prism geometry. Since here a splitter system is necessary which, as much as possible, is independent of polarization, a substrate material is preferably used which has a low index of refraction. Therewith the substrate material of the splitter configurations  16  and  15  is preferably selected to be different and the previously mentioned antireflection and index matching measures on the interfacial surface  14  must be taken. For splitter  16  preferably as the substrate material BK7 is used which has a refractive index n=1.52 and, again, attention should be paid to a low mechanical birefringence.  
         [0067]    It is not absolutely required but preferred that the same substrate material is used on both sides of layer system  18 . With respect to the dichroic color splitter layer system  18  it is essential that the transmission and reflection characteristics for the remaining two spectral ranges Δλ B  and Δλ R  are substantially independent of polarization. Since for the green spectral range Δλ G  the realization of polarization independence and angle independence is far more critical than for the blue range Δλ B  and the red range Δλ R , it is evident why the last mentioned spectral ranges are preferably supplied to the spectrally selective splitter configuration  16 .  
         [0068]    [0068]FIG. 4 shows the transmission behavior of a dichroic layer system  18 , used by example, in BK7 substrate material for angles of incidence of 45° for the s-polarization as well as also for the p-polarization.  
         [0069]    The spectrally selective layer system  18  was produced according to the characteristic to be brought into effect as long pass filter, as optical multilayer system  67  layers, alternately of high and low-refracting materials (TiO 2 , Y 2 O 3 ). Other materials and layer sequences suitable for this filter type are possible in known manner.  
         [0070]    In FIG. 5 is shown the transmission behavior of a polarization-selective layer system  17  for p-and s-polarized white light. The layer system was implemented as a typical MacNeille polarizer comprising 45 optical alternating layers of SiO 2 /Ta 2 O 5 . It is understood that here other layer sequences and/or materials are also possible.  
         [0071]    The emergent faces  20  or  22  of the spectrally selective splitter configuration  16  for the corresponding spectral ranges Δλ R  and Δλ B  can, if appropriate, be provided with an antireflection coating. If onto these faces further optical elements are directly cemented, such as light valves  25  and  24 , layer systems are preferably installed for refraction index matching.  
         [0072]    Considering retrospectively the effect of the polarization-selective splitter configuration  15 , light in p-polarization propagates in direction I. Preferably in addition to the explanations according to FIG. 1 and  2 , according to FIG. 3 a compensation body  26  is preferably provided. If the configuration depicted in FIG. 3 is modularly constructed with parts  15 ,  16  and  26 , an interfacial surface  28  between splitter  15  and compensation body  26  results. This occurs in particular if the materials of the substrate of splitter  15  differ from the material of body  26 . If in the interfacial surface region  28  an air gap is provided, it is of advantage to provide on the one and/or the other of these surfaces  28   a  and/or  28   b  an antireflection layer system. If the transition is realized free of air gap, it can be advantageous to carry out a matching of the refractive index depending on the selection of the substrate materials bordering on each other.  
         [0073]    The compensation body  26  is especially preferably provided in order to carry out a color trimming as well, yet be described. For this purpose, further advantageously a so-called halfwave retarder plate  30  is installed between surfaces  28   a  and  28   b  with which the polarization of the light in the spectral range Δλ G  can be rotated.  
         [0074]    If such a halfwave retarder plate  30  is used with or without air gaps, it is preferred to provide again a refractive index matching layer system or an antireflection system on the interfacial surfaces  28   a  and/or  28   b  and/or the corresponding surfaces of the retarder plate  30 .  
         [0075]    Apart from the possibility to provide a color triming on the compensation body  26 , with it the optical path of the light Δλ G  propagated therein is adapted to that of the light of the two other spectral ranges Δλ B  and Δλ R . On both sides of the layer system  32 , yet to be described, preferably in the 45° diagonal face of body  26 , the substrate material is preferably identical and, further preferred, identical to that of the splitter configuration  15 .  
         [0076]    The color trimming layer system  32  preferably provided in the 45° diagonal face of the compensation body  26  reflects selectively spectral ranges of the light away from the optical path, direction I. Therewith the compensation body  28  is also a spectrally selective splitter configuration. If no halfwave retarder plate  30  is provided, the light Δλ G  is first incident in p-polarization on system  32 , and is typically transmitted. If the light Δλ G , in the bright state of succeeding light valve pixels, returns in s-polarization, the layer system  32  can function very well as trimming filter; it affects the spectral characteristic in the bright state while the latter in the dark state of the pixels is substantially not affected; the light Δλ G  remains in this case p-polarized. The light reflected away by system  32  of given spurious spectral ranges, for example, emerges through a face  36  from the system or the compensation body.  
         [0077]    One possibility of trimming the behavior of the system also for the dark state of the pixels is given in the combined use of layer system  32  and retarder plate  30 . If by means of the retarder plate  30  the initially p-polarized light is rotated into s-polarization by the polarization-selective splitter configuration  15 , a color trimming can already take place on the path to the light valve  34 . The light subsequently reflected away on layer system  32  leaves the system at the emergent face  38 . Since in the dark state of the pixels no polarization change of the reflected light Δλ G  occurs, reflected light on its return path again after s-polarization, is incident for a second time on layer system  32 , and is trimmed for a second time thereby that undesirable spectral components were reflected away via face  36 . This results in an improvement in the dark state and thus an improvement of the realized image contrast.  
         [0078]    As already described for other interfacial surfaces, at the emergent face  40 , depending on whether or not an air gap to the succeeding light valve  34  is provided, as well as the materials abutting it, an antireflection coating and/or a layer system is preferably installed for the matching of the refractive indices. This applies also to the emergent faces  38  as well as  36  as a function of the structure of a total system in practice.  
         [0079]    A further improvement of the transmission properties can be provided, if appropriate, by provision of a further spectrally selective polarization rotator  50  in combination with an analyzer  52 .  
         [0080]    Via the emergent face  49  implemented with or without air gap and correspondingly preferred with antireflection and/or refractive index matching layer systems, the imaging beam A according to FIG. 2 emerges. If, potentially, light emerges in the imaging beam A from pixels switched in the dark state, its fraction can be minimized with said spectrally selective polarization rotator  50  and the succeeding analyzer  52 .  
         [0081]    Light of spectral range Δλ R  and Δλ B , which is combined correspondingly from the light valves  24  or  25  in the pixel bright state to form the imaging beam A, is p-polarized with respect to the polarization-selective layer system  17 . In contrast, light Δλ G  reflected by light valve  34  in the pixel bright state and is recombined to form imaging beam A, is there s-polarized. On the polarization-selective layer system  17 , or generally on the polarization-selective splitter configuration  15 , a portion, typically approximately 10%, of the light incident in the dark state of the pixels is also reflected into the imaging beam A. With the aid of the spectrally selective polarization rotator element  50 , this fraction can be repolarized into s-polarized light which subsequently makes all components of the light reflected in the pixel bright state p-polarized by placing the effective spectrum of this rotator into the spectral range Δλ G . All components of the light, reflected erroneously in the pixel dark state, in the imaging beam A are subsequently s-polarized. It is subsequently simple to block out with the aid of the analyzer  52  the component in the total spectrum brought about by the dark state.  
         [0082]    The analyzer  52  can therein comprise a polarization film.  
         [0083]    Subsequently, in summary again the ray path of the discrete spectral ranges will be described. For reasons of clarity and conformance with the preferred embodimnent, according to FIG. 1, Δλ 1  will be referred to as blue light B, Δλ 2  as red light R, and Δλ 3  as green light G.  
         [0084]    The description follows the representation according to FIG. 2.  
         [0085]    Ray Path G:  
         [0086]    White light, s-polarized with respect to the polarization-selective splitter configuration  1 , is incident on green rotator  10 . S-polarization is depicted in FIG. 6 as well as also the following Figures with a ray path drawn in solid lines.  
         [0087]    G leaves the rotator  10  in p-polarized form (dashed lines). Consequently, G is transmitted on the polarization-selective splitter  1  and is incident on the light valve configuration  3   a.    
         [0088]    In the bright state of its pixels, the polarization of the reflected G is rotated into s-polarization. On the polarization-selective configuration  1  the s-polarized G is output in the direction of the imaging optics system, i.e. as spectral part of the imaging beam A. In the dark state of the pixels, the polarization of the reflected light G with respect to that of the incident light is not changed. Consequently, G is reflected in p-polarization and is incident on the polarization-selective splitter configuration  1 , where it is transmitted as a portion of beam B back to the illumination optics system.  
         [0089]    Ray Path B:  
         [0090]    B is not changed on the spectrally selective rotator  10  with respect to its polarization and thus is incident s-polarized on the polarization-selective splitter configuration  1 . According to its polarization, B is reflected there and is incident, still s-polarized, on the spectrally selective splitter configuration  5  where it is reflected according to its spectral range and, still s-polarized, is incident on the light valve configuration  3   b.    
         [0091]    In the bright state of the pixels a polarization rotation takes place, B is p-polarized and reflected back onto the spectrally selective splitter configuration  5  where it is reflected according to its spectral range. B, still p-polarized, is incident on the polarization-selective splitter configuration  1  where it is transmitted as spectral range B of the imaging beam A in the direction to the imaging optics system.  
         [0092]    In the dark state of the pixels no polarization rotation takes place, B is still s-polarized and reflected back onto the spectrally selective splitter configuration  5  where it is reflected according to its spectral range. B, still s-polarized, is incident on the polarization-selective splitter configuration  1  where it is reflected as spectral component B of beam B in the direction toward the illumination optics system.  
         [0093]    Ray Path R:  
         [0094]    R is changed on the spectrally selective rotator  10  with respect to its polarization and thus is incident s-polarized on the polarization-selective splitter configuration  1 . According to its polarization, R is reflected there and is incident, still s-polarized, on the spectrally selective splitter configuration  5  where it is transmitted according to its spectral range and, still s-polarized, is incident on the light valve configuration  3   c.    
         [0095]    In the bright state of the pixels a polarization rotation takes place, R is reflected back in p-polarization onto the spectrally selective splitter configuration  5  where, according to its spectral range, it is transmitted. R, still p-polarized, is incident on the polarization-selective splitter configuration  1  where it is transmitted as spectral component R of the imaging beam A in the direction of the imaging optics system.  
         [0096]    In the dark state of the pixels no polarization rotation takes place. R is, still s-polarized, reflected back onto the spectrally selective splitter configuration  5  where it is transmitted according to its spectral range. R, still s-polarized, is incident on the polarization-selective splitter configuration  1  where it is reflected as spectral range R of beam B in the direction toward the illumination optics system.  
         [0097]    The depicted embodiment is customarily referred to as green or Δλ 3  stand-alone version since the ray path of this spectrum is relatively early separated and thus isolated. It is understood that it is also possible to realize a red or Δλ 2 stand-alone version or a blue or Δλ 1  stand-alone version.  
         [0098]    Furthermore, with respect to the light incident from the illumination source on the polarization-selective splitter configuration  1  the following two variants are possible:  
         [0099]    one spectral range p-polarized, two s-polarized, as described, or  
         [0100]    one spectral range s-polarized, two p-polarized.  
         [0101]    Furthermore, the following variants are possible:  
         [0102]    green stand-alone, transmitted red on the spectrally selective splitter, reflected blue, as described  
         [0103]    green stand-alone transmitted blue and reflected red on the spectrally selective splitter,  
         [0104]    red stand-alone, transmitted green and reflected blue on the spectrally selective splitter,  
         [0105]    red stand-alone, transmitted blue and reflected green on the spectrally selective splitter,  
         [0106]    blue stand-alone, transmitted red and reflected green on the spectrally selective splittet,  
         [0107]    blue stand-alone, transmitted green and reflected red on the spectrally selective splittet.  
         [0108]    In the following still further embodiments of the configuration according to the invention or the process according to the invention will be described.  
         [0109]    According to FIG. 9, in which the same reference symbols are used for the same elements as are explained in conjunction with FIG. 3, the spectrally selective splitter configuration  16 ′ is implemented as a glass plate as well as the compensation body  26 ′.  
         [0110]    The embodiment, for example according to FIG. 3, but also according to, for example, FIG. 2, with solid bodies has primarily the advantage that light-incident faces can be simply realized in substrate naterials perpendicularly to the direction of light incidence and thus few problems involving ray offset and astigmatism occur. But it must be noted that the design of the spectrally selective splitter layer system in solids is more difficult since the difference in the polarization is greater than on the plate version depicted in FIG. 9. Furthermore, in the solid version the light must travel a relatively long way in the substrate material which results in a stronger effect of the occurring mechanical birefringence.  
         [0111]    In the case of the plate structure according to FIG. 9, it needs to be considered that the optical path length for the three spectral components of the light must be identical. That means the layer system functioning spectrally selectively on the configuration  16 ′ must be packed in the manner of a sandwich between two glass substrates and in the “stand-alone” path an analogous geometric configuration should adapt the length of the optical path.  
         [0112]    [0112]FIG. 10 shows an embodiment in which a polarization-selective splitter configuration  15  is used with angles deviating from 45°. It is known to a person skilled in the art that polarizing splitter configurations, depending on the type used, have optimum efficiency at differing angles of incidence. Examples are the already mentioned MacNeille polarizer; polarizing beam splitters which operate above the critical angle (see for example Li Li et al. “High Efficiency LCD Projection Displays with Novel Thin-Film Polarizing Beam Splitters”, SID 98 Digest, pp. 686-689, 1998); polarizing beam splitters based on liquid crystals (see for example K. Vinokur et al., “High-Contrast-Ratio Broad-Angle LC Polarizing Beam Splitter”, SID 98, Digest, pp. 690-693, 1998).  
         [0113]    In FIG. 11 is shown the configuration according to the invention conformably with FIG. 10 in “Plate Construction.” Relatively expensive measures against the introduced astigmatism become necessary. Concomitant with losses in contrast, furthermore fundamentally the reflection angles on the polatization-selective splitter configuration as well as the spectrally selective omitted can be different and has no absolute need to be 45°.  
         [0114]    The process according to the invention can be realized with respect to material and production by using relatively simple structural parts, in particular if the (not absolutely necessary) basis is 45°.  
         [0115]    The spectrally selective polarization rotators  10  used preferably within the scope of the present invention comprise a very low angle dependence. Since the splitting-off of the first spectral range (in particular, as has been explained in detail, of the green range) takes place in combination with a largely wavelength-neutral structural element, namely the polarization-selective beam splitter  17  to be provided, an extremely low angle dependence in the spectral characteristic can be expected. Thereby small F numbers, i.e. large angular ranges become possible without disturbing color effects on the margin and in corner zones of the optically effective structural elements.  
         [0116]    In particular in the preferred green stand-alone version, the spectrally selectively dividing layer system can be selected such that polarization shift and angle shift show an effect largely only in the green spectral range. Consequently, on the one hand, the transmission of blue and red light becomes noncritical and, no disturbing color effects nor losses occur there, on the other hand, the stand-alone channel, as has been explained, can be trimmed relatively simply.  
         [0117]    In the preferred embodiment, furthermore, the light is only incident on layer systems disposed in parallel with respect to one another. This has the advantage that the “compound angle depolarization”, mentioned in the introduction and described in Rosenbluth, can be kept extremely low without further expensive measures. Therefore a special phase optimization of the thin-film layer systems does not need to be carried out in order to attain optimally good contrast.  
         [0118]    Furthermore, the optical path, which the light travels after reflection on the light valves in the substrate material, can be kept relatively short which minimizes problems based on depolarization through mechanical bireftingence.  
         [0119]    In the preferred 45°-based embodiment light produced by residual reflection and, if it reaches the imaging beam A, negatively influencing the contrast, is subsequently substantially incident perpendicularly on the emergent faces of the configuration, which makes it simplet to eliminate it through suitable measures (for example black surfaces which can absorb light) than in configurations with angles not equal to 45°.