Abstract:
The invention relates to a holographic reconstruction system for the reconstruction of scenes having at least one video hologram modulated wave front, and an enlarged visibility region. The system utilizes two-dimensional coded light modulator cells of spatial light modulation means and optical focusing means, which realize a Fourier transformation of the modulated wave front in their focal plane. First optical deflection means deflect the parallel disposed partial light waves such that their Fourier transformations appear as cascading in the focal plane. A spatial frequency filter located on the focal plane, lets each of the same diffraction orders of all modulated partial light waves pass, and second optical deflection means arrange the wave front strips next to each other at the modulated wave front, which reconstructs the scene.

Description:
CROSS REFERENCE TO RELATED APPLICATIONS 
     This application claims the priority of PCT/EP2007/058097, filed on Aug. 3, 2007, which claims priority to DE 10 2006 036255.1, filed Aug. 3, 2006, the entire contents of which are hereby incorporated in total by reference. 
     BACKGROUND OF THE INVENTION 
     The present invention relates to a holographic reconstruction system for the reconstruction of scenes, said holographic reconstruction system having an enlarged visibility region and illuminating two-dimensionally encoded light modulator cells of spatial light modulator means with coherent light. 
     FIELD OF THE INVENTION 
     The invention can be applied to a holographic reconstruction system, for example of the type of a holographic projection device as disclosed by the applicant in the international publication WO 2006/119760, titled “PROJECTION DEVICE AND METHOD FOR HOLOGRAPHIC RECONSTRUCTION OF SCENES”. 
     The projection device preferably comprises in addition to a light modulator with a modulator surface of a cell matrix, light modulator cells and an illumination device for emitting coherent light, an imaging system with a first and a second imaging means. The first imaging means images the light modulator in an enlarged manner onto the second imaging means. The second imaging means images the spatial frequency spectrum, the Fourier spectrum of the light modulator, into a visibility region. The visibility region is thus the image of the used diffraction order in the Fourier plane of the video hologram. In order for the first imaging means to be able to image the entire light modulator onto the second imaging means, all contributions of a desired diffraction order must be covered by the first imaging means. This is achieved by focussing the modulated light on the first imaging means in which the spatial frequency spectrum is created. For this, the light modulator is illuminated by a wave which converges in the direction of light propagation. The first imaging means thus lies in the spatial frequency spectrum of the video hologram. Together with the observer window, the second imaging means defines a reconstruction volume. A scene is reconstructed in this reconstruction volume. The reconstruction volume also continues backwards to any extent beyond the second imaging means. The observer is thus able to see the reconstructed scene in the reconstruction volume through the observer window. 
     Light which is capable of generating interference typically illuminates two-dimensional spatial light modulator means in order to present video holograms. 
     A method for the holographic reconstruction with an enlarged visibility region is described in document Mishina T., Okui M., Okana F.: “Viewing zone enlargement method for sampled hologram that uses high-order diffraction”, Applied Optics, Vol. 4, No. 8, p. 1489-1499. A light source illuminates a light modulator in which a hologram is encoded. A lens creates a Fourier plane of the hologram, and a spatial frequency filter in the form of an aperture mask filters out diffraction orders from the Fourier plane. The aperture mask has an aperture pattern, which can be controlled temporally and spatially, and through which multiple diffraction orders of the Fourier transform of the hologram can be transmitted sequentially and be strung together such that the reproduced image—the reconstructed three-dimensional object—can be seen by the observer in an enlarged visibility region. 
     A problem is that for enlarging the visibility region the multiple diffraction orders having different intensities are filtered and joined sequentially. For this, the filter requires controllable openings in the Fourier plane of the hologram. Because the intensity of the diffraction orders in the visibility region differs, the intensity of the illuminating light must be controlled sequentially as well. Further, extensive software means are required, e.g. for switching and controlling the apertures. The sequential representation of the hologram and the filtering process must be performed at sufficient speed, so to prevent the reconstructed image from flickering. 
     SUMMARY OF THE INVENTION 
     The present invention is based on a holographic reconstruction system for the reconstruction of scenes, where optical focussing means track a light wave front modulated by a video hologram to at least one eye position of an observer eye in a visibility region. Light which is capable of generating interference illuminates a two-dimensionally encoded modulator cell matrix of spatial light modulator means and thus modulates the light wave front. The modulator cells of the modulator cell matrix are arranged in modulator cell rows and modulator cell columns. Because it is irrelevant to the functionality of the present invention whether encoding means encode the modulator cell matrix structured in modulator cell rows or in modulator cell columns, the term ‘cell rows’ will be used for the arrangement of the encoded cell structure. 
     When the modulated wave front propagates on to the eye position, the optical focussing means perform an optical Fourier transformation of the modulated wave front in its focal plane, such that a Fourier transform of the modulated light wave front is created in the Fourier plane. 
     It is the object of the present invention to provide technical means which enlarge the visibility region optically in an inexpensive manner. When modulating the light wave front, which reconstructs a three-dimensional scene, the effective number of cells in one dimension shall in particular be multiplied in comparison to the respective number of cells in that dimension of the modulator matrix. 
     This is achieved in the holographic reconstruction system according to this invention by using a specific method of encoding the spatial light modulator means for modulating the light front which is capable of generating interference in conjunction with a spatial division of the light wave front, deflection and spatial filtering of the divided light wave front. 
     According to this invention, hologram computation means associate the information of the total light wave front which is required for the holographic reconstruction to multiple wave front strips, and compute for each video hologram of the video sequence strip holograms which comprise multiple hologram segments. 
     The hologram computation means are connected to encoding means which encode the spatial light modulator means using a combination of both time division multiplexing and spatial division multiplexing modes. The encoding means encode the spatial light modulator means with the content of a strip hologram in the time division multiplex mode and with its hologram segments in the spatial division multiplex mode. All hologram segments of each strip hologram together have such a number of hologram pixels that the strip holograms are disposed side by side in cell rows on the modulator cell matrix as spatial division multiplex structure of the corresponding hologram segments. 
     As a result of the illumination of the modulator cell matrix with a light wave front which is capable of generating interference, the modulator cell matrix modulates partial light waves propagating parallel which comprise the information of a hologram segment and which are assigned to a strip hologram. 
     To solve the object of the present invention, the following elements are disposed in the light path of the light wave front, in addition to the modulator cell matrix and the focussing means:
         First optical deflection means which deflect the partial light waves propagating parallel of the modulated wave front in different directions such that their Fourier transforms appear in a step-like manner in the focal plane,   A spatial frequency filter which lies in a focal plane of the focussing means and which lets pass the same diffraction order of all modulated partial light waves,   Second optical deflection means which string together the passing diffraction orders of the partial light waves so to form a wave front strip,   A time division multiplex control system, which works in synchronism with the time division multiplex mode of the hologram computation means, and which discretely adjusts adjustable third optical deflection means such that these deflection means dispose the wave front strips side by side, such that the modulated wave front appears and all wave front strips holographically reconstruct the desired scene in the time division multiplex mode.       

     In other words, all hologram segments which are encoded during a signal frame of the video signal belong to one strip hologram and modulate partial light waves, propagating parallel, of a wave front strip with the hologram segments. The modulator cell matrix modulates the remaining strip holograms by way of time division multiplexing, such that the strip holograms holographically reconstruct the scene by way of time division multiplexing. 
     It is a known disadvantage that the cell structure of the modulator cell matrix modulates in addition to a desired diffraction order parasitic diffraction orders, for which a Fourier transformation is performed by the optical focussing means. The Fourier transformation causes a spatial frequency spectrum to be generated in the focal plane of the focussing means for each partial light wave. 
     In order to optically enlarge the visibility region according to the object of this invention, first optical deflection means laterally deflect the partial light waves of a strip hologram in one dimension such that the partial light waves appear in a step-like offset manner in the focal plane of the optical focussing means. These deflection means have static angle settings. This has the advantage that a simple spatial frequency filter with a step-like structure of fix apertures can be used in order to separate with high efficiency the same respective diffraction order, which is desired for reconstructing, of each modulated partial light wave from the disturbing parasitic diffraction orders. 
     Second optical deflection means string together the passing diffraction orders of all modulated partial light waves such that a modulated light wave strip is generated, which is made up of the joined partial light waves. The second optical deflection means thus compensate the optical deflection of the partial light waves which are organised in a spatial division multiplex process in order to make up for the spatial multiplexing. 
     As a result of the lateral deflection in one dimension, this modulated light wave strip exhibits a hologram pixel resolution which is a multiple of the number of the hologram segments. A multiplication of the diffraction angle of the modulator cell matrix is thus achieved in one dimension of the modulator cell matrix, which corresponds to an enlargement of the visibility region according to the object of the present invention. 
     The first optical deflection means can be a prism array which is disposed in the optical path of the wave front and which displaces the modulated partial light waves in one dimension, i.e. horizontally or vertically against one other, such that the modulated partial light waves are disposed side by side in the focal plane of the focussing means in a step-like manner and offset by one diffraction order. 
     The encoding means preferably assign each hologram segment on the cell structure of the modulator cell matrix with multiple adjacent horizontal modulator cell rows, such that only few, for example three, hologram segments lie on the modulator cell matrix. According to the number of hologram segments, the first optical deflection means comprise multiple, for example three, prisms which stretch entirely across the modulator cell matrix in one dimension. The longitudinal sides of the prisms adjoin to one another, and the prisms exhibit different inclinations. The inclinations are chosen such that the same diffraction orders of the adjacent partial light waves are adjoined in the focal plane after the deflection such that a seamless connection of the step-like offset same diffraction orders is achieved. This can be achieved if the maximum diffraction angle of the light modulator means in the direction of deflection defines the inclinations of the prisms. 
     According to a preferred embodiment of this invention, the first optical deflection means can be a prism array with micro prisms, where each matrix section is assigned with a multitude of micro prisms, which direct the partial light waves in a step-like manner according to the structure of the spatial frequency filter. This facilitates a more light-weight design of the projection system and reduces the volume of the hologram projector. 
     The spatial frequency filter may preferably be an aperture mask with apertures each of which letting pass a single diffraction order of the modulated partial light wave. However, a different mask with transparent and light-impermeable areas, for example a photographic film copy or the like, can be used instead of an aperture mask. This mask then comprises step-like offset transparent areas which correspond to the form and position of the same diffraction orders in the plane where the spatial frequency filter is disposed. 
     The second optical deflection means is also a prism array. The prisms lie in the optical path in order to string together the modulated, filtered and step-like offset partial light waves in one dimension so to form one light wave strip. 
     The second optical deflection means are preferably also micro prisms, a multitude of which being assigned to each matrix section. These micro prisms can also be adjusted as regards their angular range and be connected to a position controller which is adjusted by an eye finder such that the light wave strips with their partial light waves are directed according to an eye position. This way, if the adjustable optical deflection means are enlarged, the modulated partial light waves can be tracked at least in one dimension according to the changes of eye positions. 
     In order to save room inside the device, the second optical deflection means can be disposed directly on the spatial frequency filter. 
     The discretely adjustable third optical deflection means are well known from beam-projection display devices. Such a device has movable mirrors or rotating polygonal mirrors for reproducing an image on a display surface, and deflects the light for example row by row. The international publication WO 2006053793, titled “BEAM-PROJECTION DISPLAY DEVICE AND METHOD FOR OPERATING A BEAM-PROJECTION DISPLAY DEVICE” may be referred to as an example. The third optical deflection means can also be controllable micro prisms. 
     It appears to a person skilled in the art, that it is not relevant for the practical embodiment of this invention whether the modulator cells of each cell row are disposed horizontally or vertically. 
     Considering this, the visibility region can for example be broadened in the spatial division multiplex mode by horizontally stringing together multiple hologram segments, i.e. by increasing the horizontal resolution. In this context, the hologram computation means can compute a larger number of strip holograms for each video hologram in order to increase with the help of the encoding means the vertical resolution in the time division multiplex mode. 
     If the holographic reconstruction system exhibits such a structure, micro prisms in the second deflection means which are adjustable as regards their angular range and which are connected to a position controller, can direct the generated modulated light wave strips in accordance with horizontal changes of the eye position. 
     According to a preferred embodiment of the present invention, the focussing means exhibit horizontally and vertically different focal planes such that both a Fourier plane and an image plane can be created in the same plane. A focal plane is therein disposed as close as possible to the spatial frequency filter, such that a Fourier transform of the partial light waves appears on the spatial frequency filter in the direction of deflection of the first deflection means. The second focal plane lies such that the focussing means vertically project the illuminated modulator cell matrix on to the second deflection means. 
     In the present case, the focussing means realise in the horizontal direction a Fourier transformation of the modulated wave front near the spatial frequency filter, and in the vertical direction an imaging of the light modulator means near the second deflection means. 
     In a specific embodiment, the focussing means have a focal length f x  in one direction and are disposed at that distance f x  after the light modulator means, such that the Fourier transform of the partial light waves is generated on the spatial frequency filter at that distance f x  after the focussing means, such that the diffraction orders of the modulated partial waves, which are emitted by the light modulator means at different angles, appear spatially separated on the spatial frequency filter. 
     The focussing means have for example a vertical focal length f y , where f y =f x /2 and where the distances between the light modulator means and focussing means, and between the focussing means and the spatial frequency filter plane are 2f y . An image of the hologram segments on the modulator cell matrix then is generated in the spatial frequency filter plane. 
    
    
     
       SHORT DESCRIPTION OF FIGURES 
       The present invention will be described in more detail below with the help of a number of embodiments and drawings, wherein 
         FIG. 1  is a perspective view of a part of the holographic reconstruction system according to the present invention, 
         FIG. 2  is a schematic view of a modulator cell matrix of spatial light modulator means, 
         FIG. 3  shows an example of a deflection means in the form of a prism array in a projection system according to the present invention, 
         FIG. 4  is an example of the step-like offset of the modulated partial light waves with the help of the prism array according to  FIG. 3 , 
         FIG. 5  is a schematic view illustrating the function of the focussing means, where 
         FIG. 5   a  is a top view of the modulated and Fourier-transformed wave front and 
         FIG. 5   b  is a side view of the wave front which images the video hologram in the vertical direction into a plane, 
         FIG. 6  illustrates the structure of the spatial frequency filter, 
         FIG. 7  is a schematic view showing a side view of the optical path of a device according to the present invention, 
         FIG. 8  is a top view of the device according to this invention with a one-dimensional diffuser, 
         FIG. 9  is a side view of one embodiment of the device according to this invention according to  FIG. 7  with an adjustable third optical deflection means in the form of a rotating mirror having a rotation axis, 
         FIG. 10  shows the graph of the desired diffraction orders for the modulated partial light waves, and 
         FIG. 11  illustrates a deflection pattern generated when rotating the rotating mirror, with the modulated partial light waves which are deflected in vertical steps being arranged next to each other in rows. 
     
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
       FIG. 1  illustrates a detail of a holographic reconstruction system  1  for the holographic reconstruction of scenes with a light modulator  2  on which a sequence of video holograms is encoded. Light which is capable of generating interference (not shown) illuminates the modulator cell matrix  4  of a spatial light modulator  2  with m modulator cell rows at n modulator cells each, focussing means, here in the form of a lens  7 , and a spatial frequency filter  8 . 
     According to the present invention, a first optical deflection means, here in the form of a prism array  11 , is disposed between the light modulator  2  and the lens  7 . Hologram computation means  3  compute for each video hologram strip holograms S 1  . . . S 3  with hologram segments H 11  . . . H 33 . An encoding device (not shown) encodes one after another the modulator cell matrix  4  with hologram segments of the strip holograms S 1  . . . S 3 .  FIG. 1  thus shows different sequentially encoded modulator cell matrices  4 ,  4 ′ and  4 ″ in assigned cell regions  12 ,  13 ,  14  with the hologram segments H 11  . . . H 33 , the horizontally deflecting static prism array  11 , focussing means in the form of a lens  7  and a spatial frequency filter in the form of an aperture mask  8  with attached second optical deflection means, the vertically deflecting prisms  51 ,  52  and  53 . The prism array  11  realises a horizontal, step-like displacement  9  of the partial light waves which are modulated by the cell regions  12 ,  13 ,  14 . The aperture mask  8  has step-like offset openings  15 ,  16 ,  17  which are disposed below the prisms  51 ,  52 ,  53  and which filter only one chosen diffraction order out of the Fourier transform of the partial light waves of the hologram segments. The prisms  51 ,  52  and  53  vertically deflect the filtered partial light waves such that the latter hit a third deflection device  54 , which can be pivoted around a horizontal axis, such that the hologram segments of each strip hologram S 1 , S 2  or S 3  appear one after another as light wave strips. The deflection device  54  is synchronised by a time division multiplex controller  55  with the time multiplex mode of the hologram computation means, such that an entirely modulated light wave front with the structure and modulation of all strip holograms S 1  . . . S 3  is made available for a holographic reconstruction through an exit pupil  56 . 
       FIG. 2  shows the modulator cell matrix  4  of the light modulator  2 , which exhibits n modulator cells  6  and m cell columns  5  in a cell row, where, in the present case, three cell columns  5  form one cell row  12 ,  13 ,  14 . 
     As shown in  FIG. 3 , the prism array  11  comprises three prisms  21 ,  22 ,  23 , which are disposed side by side vertically, and which exhibit different inclinations  24 ,  25 ,  26  with different inclination angles −α, 0°, +α, said inclinations  24 ,  25 ,  26  being chosen such that the corresponding diffraction angle ranges Θ x1 , Θ x2 , Θ x3  of adjacent prisms  21 ,  22 ,  23  are adjoined such that horizontally a seamless connection of the step-like offset  9  of the modulator rows  12 ,  13 ,  14  can be achieved, as shown in  FIG. 4 . 
     The maximum number of the adjoined diffraction angle ranges corresponds to the number m of the cell rows  5  into which the light modulator  2  is structured during the encoding process. However, the prism array  11  would comprise very many very narrow prisms, and the subsequently disposed movable deflection means would have to position very finely. The narrow prisms would be prone to great diffraction effects. It is therefore sensible not to adjoin the maximum number of angular ranges that corresponds with the number m of cell rows  5 . 
     In  FIG. 1 , for example, only three prisms  21 ,  22 ,  23  are thus used, i.e. each prism  21 ,  22  and  23  is assigned with one third of the cell rows  5 , where that third may then be a modulator row  12  or, as will be explained below, may comprise a hologram. 
     The maximum horizontal diffraction angle of the light modulator  2  defines the diffraction angle ranges Θ x1 , Θ x2 , Θ x3  of the prisms  21 ,  22 ,  23 . 
     As shown in  FIG. 3 , the light modulator  2  with a cell pitch of 10 μm exhibits a maximum diffraction angle Θ x  of 3.6° at a wavelength λ of 633 nm. The value of 3.6° also represents the angular range of a diffraction order. In order to also select the corresponding diffraction order of an adjacent partial light wave, the adjacent prism  24  or  26  must deflect the light by +3.6° or −3.6°, respectively. 
       FIG. 3  shows the prism  21  with an incident partial light wave  27  and the modulated partial light wave  33  which is deflected by the angle δ. The prism angle is the angle α of the inclination  24 . A partial light wave  27  which enters the lower face of the prism  21  is deflected by the angle α when it exits the upper face. The relation between α and δ is given as δ=arcsin (n*sinα)−α(I), where n is the refractive index of the prism  21 . For small angles α, the linear approximation δ≈(n−1)*α can be derived from equation (I). 
     Given a refractive index n of 1.5, a prism angle α of 7.2° is thus required in order to deflect an incident partial wave  27  by 3.6°. Because according to the linear approximation the deflection angle δ does not depend on the angle of incidence on the lower face of the prism, the angular range of one diffraction order is deflected by 3.6°. If the central prism  22  has a prism angle of 0°, according to the above-mentioned linear approximation, the adjacent prisms  21  and  23  must have prism angles of +7.2° and −7.2°, respectively, and the next but one prism must have prism angles of +14.4° and −14.4°, respectively. 
     In contrast to  FIG. 1 , where the prism array  11  is disposed behind the light modulator  2 , it is also possible to dispose the prism array  11  in front of the light modulator  2 . 
     The combined arrangement of light modulator  2  and prism array  11  can also be considered as a single-row light modulator with n*m cells, where one row comprises n*k cells. The prism array  11  is therein used for spatial division multiplexing, i.e. the hologram segments H 11 , H 12 , H 13 , which correspond to the adjoined angular ranges Θ x1 , Θ x2 , Θ x3 , are encoded simultaneously, but spatially separated on the light modulator  2 . 
     The maximum diffraction angle Θ x  of the light modulator  2  is λ/p, where p is the cell pitch of the light modulator  2  and λ is the wavelength of the incident light. The maximum diffraction angle Θ x  also limits a diffraction order. In one diffraction order, the diffraction pattern can be controlled by encoding the light modulator  2 . The diffraction pattern is repeated in higher diffraction orders. The higher diffraction orders adjoin the angular range Θ x  of the zeroth diffraction order on both sides. 
     The spatial frequency filter according to this invention prevents parasitic diffraction orders from entering the used diffraction orders of the partial light waves of the prisms  21 ,  22  and  23 . This is important because a parasitic diffraction order is only a periodic continuation of the used diffraction order, and parasitic diffraction orders which enter the visibility region would substantially disturb the holographic reconstruction. This is why the spatial frequency filter may only let pass the used diffraction order of the partial wave front, which is divided by each prism  21 ,  22 ,  23 . 
     One possibility for this is shown in  FIG. 5  with  FIG. 5   a  and  FIG. 5   b  in combination with  FIG. 6 . The focussing means which lie in the optical path, and which are illustrated as lens  7  here, exhibit vertically and horizontally different focal planes. It is thus achieved that both a Fourier transform of the video hologram and an imaging of the light modulator are disposed in the same plane  28 . This means that the Fourier plane is identical to the image plane. 
       FIG. 5   a  is a side view. The lens  7  (L x ) is disposed behind the illuminated light modulator  2 . That lens has the focal length f x  in the horizontal direction and is disposed behind the light modulator  2  at that distance f x . A Fourier transform of the modulated light wave front is generated in the horizontal direction in the filter plane  28  at the distance f x  behind the lens  7 . The diffraction orders which, starting from the light modulator  2 , run at different angles are spatially separated in the filter plane  28  as a result of the Fourier transformation. 
       FIG. 5   b  is a side view. The lens  7  has the vertical focal length f y , where f y =f x /2. The distance of 2f y  both between the light modulator  2  and the lens  7 , and between the lens  7  and the filter plane  28 , causes the holograms segments on the light modulator to be projected vertically into the filter plane  28 . 
     Because the filter plane  28  is a Fourier plane horizontally and an image plane vertically, the spatial frequency filter  8  is disposed in the filter plane  28  in the present invention. This is shown in  FIG. 6 . The numbers entered on the spatial frequency filter  8  describe the diffraction orders of the Fourier transforms. In the Figure, the central section  30  of the spatial frequency filter  8  comprises the −1 st , 0 th  and 1 st  diffraction order of a prism  22 . In the upper segment  31 , the diffraction orders of the adjacent prism  21  are displaced to the left by one diffraction order, because the angle of the prism  21  is chosen such that there is a deflection by one diffraction order. The same applies to the lower section  32 , which corresponds to the prism  23 , but with an offset by one diffraction order to the right. Because the vertical and horizontal focal lengths of the lens  7  differ, a Fourier transform of the light wave front lies in the filter plane  28  and the diffraction orders are spatially separated while the lens  7  images the encoded light modulator  2  vertically. 
     The spatial frequency filter  8  exhibits openings  15 ,  16 ,  17 , which only let pass the selected diffraction order of each hologram segment  12 ,  13 ,  14 . This results in a structure of step-like offset rectangular apertures  15 ,  16 ,  17 , and the selected diffraction orders of the hologram segments are adjoined while the spatial frequency filter  8  absorbs all undesired diffraction orders. This prevents mutual interference of the various diffraction orders. The horizontally adjoined selected diffraction orders multiply the diffraction angle of a light modulator  2 . 
       FIG. 6  illustrates a step-like offset of the adjoined angular ranges Θ x1 , Θ x2 , Θ x3 . Whether or not the offset  9  must be compensated in the vertical direction, and how this is done, depends on the subsequent optical arrangement or a subsequent optical system, according to the intended use of the device. The light filtered in the filter plane  28  can be directed into a subsequent optical arrangement, as shown in  FIGS. 7 ,  8  and  9 , e.g. for a holographic illumination device or for a holographic projection system. 
       FIG. 7  is a side view of the device  1  according to this invention for adjoining diffraction orders of an encoded light modulator  2  for use in a subsequent arrangement  34 . The compensation of the step-like offset  9  with a deflection device  40  in the form of a one-dimensional diffuser is shown in  FIG. 8 . In the embodiment, the prism array  11 , which comprises the three prisms  21 ,  22 ,  23 , is disposed behind the light modulator  2 . The drawn bundles of rays  18 ,  19 ,  20  represent the selected diffraction orders of the prism  21 , prism  22  and prism  23 . The used diffraction orders of the partial light waves are offset as regards their angles Θ x1 , Θ x2 , Θ x3 , and are thus spatially separated in the filter plane  28  behind the lens  7 . A lens  38  horizontally images the filter plane  28  into an exit plane  39 . This is why the diffraction orders, which are spatially separated in the filter plane  28 , are spatially separated there again. The prisms  21 ,  22 ,  23  of the prism array  11  horizontally direct the modulated bundles of rays  18 ,  19 ,  20  into different adjacent angular ranges Θ x1 , Θ x2 , Θ x3 . The diffraction angle range Θ x =Θ x1 +Θ x2 +Θ x3  of the light modulator  2  is thus enlarged in the horizontal direction. 
       FIG. 8  is the corresponding side view. The prism array  11 , which vertically deflects the light waves, is disposed behind the light modulator  2 . The lens  7  images the prisms  21 ,  22 ,  23  into the filter plane  28 , where the spatial frequency filter  8  is disposed. The lens  38  vertically realises a Fourier transformation into the exit plane  39 , where the Fourier transforms of the partial light waves lie. However, the modulated light of the hologram segments runs into different angular ranges Θ y1 , Θ y2 , Θ y3 . 
     Because in the horizontal direction the light is radiated into different angular ranges Θ x1 , Θ x2 , Θ x3 , only an offset total angular range (Θ x , Θ y ) as shown in  FIG. 10  can be covered. The individual angular ranges  43 ,  44 ,  45  with Θ x1 , Θ y1 ; Θ x2 , Θ y2 ; Θ x3 , Θ y3  are adjoined in a step-like offset manner. As shown in  FIG. 8 , a one-dimensional diffuser  40  which acts in the vertical direction diffuses the light in the arrangement  34 , and so a continuous angular coverage is achieved over a total angular range Θ y  of at least Θ y1 +Θ y2 +Θ y3 . 
     If the encoded information of the light modulator  2  is constant in the vertical direction, the vertical diffuser  40  will be sufficient for compensating the offset  9 , where, however, any vertical information will be lost. This is why only a horizontal diffraction pattern with horizontal structure can be used, such as a sequence of parallel lines in the vertical direction. Such a projection device can serve in a holographic reconstruction device to realise a backlight with virtual light sources. In this case, the light modulator  2  is encoded with a computer-generated hologram which reconstructs light points or light lines which serve to illuminate a second light modulator on which the video hologram is encoded. 
     However, if the projection system is provided primary for generating a holographic reconstruction, a one-dimensionally deflecting rotating mirror  41  will be required instead of the one-dimensional diffuser  40 , as shown in  FIG. 9 . The rotating mirror  41  deflects the light of the light modulator  2  in the vertical direction. The arrangement  35  is more flexible than that with the one-dimensional diffuser  40 , because the light modulator  2  is encoded with a new strip hologram while the rotating mirror  41  is in motion. Thereby, a visibility region is generated which comprises sub-regions which are adjoined vertically in a step-like manner. It thus becomes possible to structure and enlarge the visibility region in the vertical direction as well. 
     Because the Fourier transformation with the help of the lens  38  also produces vertical parasitic diffraction orders, these parasitic diffraction orders must be blocked by a horizontal aperture gap filter in the exit plane  39  (not shown). The top view is the same as shown in  FIG. 7 . 
     The rotating mirror  41  disposed in the exit plane  39  (not shown) has a horizontal rotation axis  42 . The beams from the angular ranges  43 ,  44 ,  45  are thus deflected vertically. 
       FIG. 10  shows the angular ranges  43 ,  44 ,  45 , which are covered if the mirror is not in motion. Horizontally, the angular ranges of the used diffraction order are adjoined. Vertically, encoding the modulated cells in adjacent modulator rows  12 ,  13 ,  14  causes step-like offset angular ranges  43 ,  44 ,  45  to appear in the filter plane  28 . This is why no rectangular angular range, which would be parallel to the axes of the coordinate system, can be covered if the rotating mirror  41  is at a fix position. 
       FIG. 11  shows a deflection pattern when rotating the rotating mirror  41  with step-like offset angular ranges  43 ,  44 ,  45  in the vertical direction, where the angular ranges are seamlessly adjoined by the rotating mirror  41 . The angular ranges  43 ,  44 ,  45  with same hatching are displayed simultaneously. If the light modulator  2  is re-encoded in synchronism with the movement of the rotating mirror, the hologram can also be structured in the vertical direction. The angular ranges with the same Θ y  and different Θ x  are generated at different times in the modulator, as can be seen in the Figure (different hatching). Thanks to the vertical deflection, a rectangular angular range  46  can be covered, which is shown as a dotted area in  FIG. 11 . The appendices  47 ,  48  at the upper  36  and lower edges  37  can be gated out or hidden through an empty light modulator content. 
     This is achieved when reconstructing the hologram  4  either by illuminating each sub-hologram  12 ,  13 ,  14 , . . . of the light modulator  2  under different angles, where the illumination angle changes in steps which correspond to the maximum diffraction angle Θ x1 , Θ x2 , Θ x3 , . . . , Θ xk  of a modulator row  12 ,  13 ,  14 , . . . , or by illuminating them under a fix angle, e.g. in the normal direction (the z direction). The light of the hologram  4 , which is diffracted by each sub-hologram  12 ,  13 ,  14 , . . . , will then be deflected under an angle which is also step-wise enlarged according to the maximum diffraction angle Θ x1 , Θ x2 , Θ x3 , . . . , Θ xk . Both variants can be realised e.g. with the light modulator  2  and the prisms  21 ,  22 ,  23 , . . . which each cover a sub-hologram  12 ,  13 ,  14 , . . . of the hologram  4 . Their respective inclinations  24 ,  25 ,  26 , . . . are enlarged in steps according to the diffraction angles Θ x1 , Θ x2 , Θ x3 , . . . , Θ xk . 
     In contrast to prior art solutions, a major advantage of the present invention is that the spatial frequency filter is static, fitted with fix, localised openings in the mask, and that it works without a shutter device. 
     Depending on the application, the present invention makes it possible either to virtually enlarge the resolution of spatial light modulator means or to enlarge the visibility region for a holographic reconstruction.