METHOD AND APPARATUS FOR PRODUCING THREE-DIMENSIONAL PICTURES

Abstract: The three-dimensional television set comprises a closed apparatus (12) with a 3D video signal input and/or arial input, and a laser source (22), a modulator (24) and a deflecting system (30) arranged in the closed apparatus (12), and a light emitting surface (40) at the front face of the closed apparatus (12), said deflecting system (30) providing deflection of laser beam produced by said laser source (22) into pixels (42) of said light emitting surface (40), and a further deflection to direct laser ray emitted from said pixels (42) to various directions (i1, i2...in) defining a three-dimensional field of view, under control of synchronizing signal corresponding to direction information of a 3D video signal.

Description: METHOD AND APPARATUS FOR PRODUCING THREE-DIMENSIONAL PICTURES BACKGROUND OF THE INVENTION Technical Field The invention relates to a method and apparatus for producing three-dimensional picture, in particular to a three-dimensional television receiv¬ ing system. The invention is also useful for other purposes, such as industrial planning and design . Summary of the Prior .Art Video signals are recorded electronically or by other means, and may be displayed through a television system . The television receiver converts incoming television (video) signals into the original scenes or figures along with the associated sounds . The known two-dimensional television receivers comprise a picture tube having plane or arched fluorescent screen, producing a planar image by varying the electron-beam intensity as the beam, emitted by an electron gun, is deflected from side to side and up and down to scan a raster on the fluorescent screen at the other end of the tube . The fluorscent screen realizes a definite raster of segments, known as picture points or picture elements, arranged in scanning lines . The picture elements of the fluorescent screen are scanned point to point after each other by the electron beam, as the electron beam is moved by controlled horizontal and vertical deflection . The issue of displaying true 3D scenes is not yet solved properly up-to-date . According to the present state of television technique 3D image reconstruction is exhausted at the level of displaying stereoscopic or autostereoscopic images . In these systems the three-dimensional effect is based on the deception of human perception (e.g. using special glasses) causing bad physiological effect . There are experimental systems which employ lenticular-lenses . By principle, these systems realize a resticted field of view and poor resolution . A widely used method of three-dimensional optical image formation is the holography, a technique for recording and later reconstructing the amplitude and phase distributions of a wave disturbance . In optical image formation, the technique is accomplished by recording on a special photographic plate the pattern of interference between coherent light reflected from the object figure, and light coming directly from the same source or being reflected from a mirror. When the special photographic plate, known as hologram is developed and illuminated from behind by a coherent laser beam, it produces a three-dimensional image in space . Holography, however, is not a practical technique for producing three-dimensional picture from video signals. Objects of the invention An object of the invention is to provide a method which enables receiving three-dimensional video signals and producing real three-dimensional picture from them. A further object is to develop an apparatus to realize the above method, i .e . an apparatus producing three-dimensional picture from the received 3D video signal, said apparatus being realizable with reasonable form and expenditure . An essential object of the invention is to achieve a three-dimensional television system by means of the suggested method and apparatus . SUMMARY OF THE INVENTION An essential feature of all kind of two- -dimensional, planar images, e .g. paintings, photoes or picture of a usual television screen is that the intensity of light emitted or reflected from any point of the picture is independent, within a wide field of view, from the direction of the emitted or reflected light, i .e . a given picture point is the same viewed from every direction . On the other hand, a three-dimensional, spatial picture is characterized by picture points emitting or reflecting different light beams in every direction of the field of view, which means that the intensity (and colour) of a given picture point viewed from different directions depends on the viewing direction . It has been found that a three-dimensional picture can be provided by means of a light emitting surface in which light beams are emitted from the picture points of said light emitting surface to many directions, wherein the intensity and colour of the light beam emitted from any picture point is function of the viewing direction . Said viewing directions together define a three dimensional field of view. The quality of such three dimensional picture would depend on the density of the picture points and on the number of directions defining the field of view, and also on the width of said field of view. Set out from the above recognition, the method according to the invention comprises the steps of: modulating the intensity of a spatially coherent light ray, preferably a laser ray by a 3D video signal (video signal containing three-di¬ mensional picture information) , - directing the modulated laser ray by controlled deflection into pixels defining a light emitting surface, and - deflecting the modulated laser ray to be emitted from every pixel of the light emitting surface to a number of directions, said directions defining a given field of view, the intensity of said laser ray components emitted from said pixels in various directions of the field of view corresponding to the direction information of the concerning direction of the 3D video signal. According to the invention the laser ray modulated with the 3D video signal containing intensity and colour information is directed to the picture points (pixels) in a defined order, which order is preferably controlled by the synchronizing components of said 3D video signal . The light ray emitted from any pixel to any direction has an intensity and colour corresponding to the intensity and colour information of the 3D video signal component associated with said pixel and said direction . The coordinates of an emitted laser ray is defined as a result of the horizontal, vertical and viewdirectional deflections . Baεicly there are two modes of achieving the above deflections of modulated laser ray according to picture points and directions . The one mode is deflecting the laser ray according to said directions before reaching the pixels so that the incident components of laser ray striking into the pixels are deflected in angle of arrival or displaced parallel in association with the direction they belong to . The further deflection shall be achieved without any further controlled step, pre¬ ferably by use of passive optical means . According to the other mode of deflecting the laser ray strikes into the pixels without being de¬ flected according to the view directions, and is de- ujnb fleeted and emitted through active, controlled optical elements placed in the pixels to said various directions defining said field of view. The modulated laser can be directed into said pixels by means of mechanical or acousto-optical deflecting means controlled in accordance with said directions of the field of view, too, wherein said mechanical or acousto-optical deflection is preferably controlled by horizontal and vertical deflection information contained in the synchorinizing component of said 3D video signal . Preferably, the modulated laser ray is directed into said pixels by use of horizontal and vertical (frame) deflection according to TV standards, said pixels being arranged so that their configuration conforms with the standard TV picture point configur¬ ation . In an advantageous practical mode of realizing the invention a laser beam is modulated by a 3D video signal having no vertical parallax information content, wherein said laser beam emitted from a pixel horizontally sweeps along said field of view, said laser beam having a definite vertical dispersion . Since the human eyes are normally in the same horizon¬ tal plane, omitting the vertical parallax does not mean practically any essential loss of quality in the three-dimensional view. The modulated laser ray striking into said pixels preferably can be deflected and directed through holographic optical elements or through periodical spheric-symmetrical optical elements to the directions of the field of view. According to the invention the modulated laser ray can be achieved by direct modulation of a laser source with said 3D video signal . The modulated laser ray can also be achieved by modulating an acousto-optical crystal through which the laser ray passes by said 3D video signal . A sufficiently wide spatial view can be achieved by realizing a field of view of 30 to 150°, wherein the number of said various directions defining said field of view is 30 to 150, which presumes a horizontal dispersion of emitted light beam of about 1°. Our experiments show that three-dimensional spatial picture of satisfactory quality is achieved even with a horizontal viewing field of 30 to 40 degrees, and view direction steps of 1 to 3 degrees . As mentioned above, the vertical parallax of the three-dimensional view can be omitted. In this case the laser beam of any horizontal direction should have an appropriate vertical dispersion, which can be achieved by using e .g. holographic or vertical cylindric-symmetrical optics combined with one dimensional dispersion elements . According to the invention colour three- dimensional picture can be produced by modulating a multicoloured laser beam or more laser rays, preferably three laser rays of different basic wavelength (red, green and blue) , deflecting and directing them into said pixels, and directing a modulated laser beam containing said three laser rays of different basic wavelength from each pixel to each direction of said field of view. Three dimensional moving picture may be achieved according to the invention by a definite number, preferably at least twenty picture repetitions per seconds . The bandwidth of the 3D video signal can be reduced if necessary by use of any data- or information-compressing process . Such processes are known per se so the don ' t need further discussion . The 3D video signal by which the laser beam is modulated can be produced e .g. so that 2D images of a spatial scene or figure are taken simultaneously from each of said directions defining said field of view by means of appropriate TV or video cameras, advantageously a multielement CCD camera containing a corresponding number of CCD chips, and the 2D signals recording the different view images are composed to consitute a 3D video signal format . The signal components associated with the different picture points and various view directions are ordered in a defined time sequence . Other means for recording a 3D video signal are known per se . The problem of producing three-dimensional picture can also be solved by controlling spatially coherent elementary light sources, such as CSD or monolithic surface-emitting laser diode arrays, or preferably elementary laser sources, arranged to constitute a light emitting surface, so that each of the elementary light sources is controlled according to the corresponding view direction information of a 3D video signal, wherein said view directions define a given field of view. In this case preferably each of said elementary light sources is associated with one of said view directions, and controlled according to the one direction it belongs to. The light rays emitted by said elementary light sources are directed to the — o — view direction the corresponding elementary light source belongs to, by use of optical means integrated in the pixels of said light emitting surface . The elementary laser sources can also be simultaneously controlled in combination with each other according to holographic patterns, so that the laser beams sent to said view directions are achieved by the interference of coherent light waves emitted by the elementary laser sources . In order to reduce the sharp resolution requirements of the deflection system used in carrying out of the invention, a further method is suggested, employing a light beam comprising independently controllable coherent light rays; The suggested method comprises the steps of: modulating a coherent light beam, preferably a laser beam by a 3D video signal, wherein the modulated light beam should contain light rays each associated with a view direction, said view directions defining a given field of view, said light rays of the beam being modulated simulaneously, each light ray according to its associated view direction, directing said modulated coherent light beam into pixels arranged to define a light emitting surface, and emitting each component of the modulated coherent light beam from the pixels to the direction said component (light ray) is associated with . The invention also relates to an apparatus for producing three-dimensional picture . The apparatus according to the invention comprises: a spatially coherent light source, preferably laser source; a modulator to modulate laser ray produced by said light source, said modulator controlled by a 3D video signal; a deflecting sysem to deflect modulated laser ray, controlled by the synchronizing signal of the 3D video signal; a light emitting surface composed of pixels of definite mutual arrangement; and optical elements adjusted in said pixels of the light emitting surface to deflect and/or transmit incident laser ray from the pixels to various directions, said directions defining a given field of view, wherein said deflecting system is controlled to deflect laser ray in accordance with said directions of the field of view into said pixels. Preferably, the pixels constituting the light emitting surface are arranged in conformity with the picture point configuration of a standard TV screen, and said deflection system comprises horizontal and vertical deflection units controlled by the line synchronizing signal and frame synchronizing signal, respectively, of the 3D video signal . The vertical deflection unit and the horizontal deflection unit can comprise e.g. acousto-optical crystals controlled by voltage-controlled oscillators . The deflecting system may involve acousto- optical elements controlled in accordance with the directions of said field of view. The optical elements can also be passive elements of pre-defined horizontal deflection characteristic and definite vertical dispersion, preferably cylindric-optical elements, holographic optical elements etc. , said holographic optical elements having vertical focus line, and light dispersing in vertical planes involving said vertical focus line. In the latter case, when the optical elements in the pixels are passive ones, the deflecting system provides that the laser ray arriving the pixels is deflected according to the various directions . The deflection range of said deflection system should correspond to the number and width of said optical elements adjusted in said pixels. In a preferred apparatus according to the invention the deflection system comprises fibreglass groups, one for each pixel, said fibreglass groups each having a number of fibreglasses, which number is equal to the number of various directions defining said field of view, the input end of said fibreglass groups being attached to the output of a unit deflecting said modulated laser ray in accordance with the pixels, the other end of said fibreglass groups being attached to the concerning one of said pixels, the end sections of the fibreglasses of said groups being adjusted to direct laser ray to the very direction associated with the corresponding one of said fibreglasses . Each fibreglass of a group transmits a component of the modulated laser beam, which component is associated with the view direction said fibreglass belongs to. In a further preferred embodiment of the invention the laser source and said modulator are realized in a laser unit comprising laser diode controlled by said 3D video signal . A more practical construction can be achieved by integrating said laser source, modulator and deflection system in an integrated optical unit . In a preferred embodiment of the invention the laser source is directed to an acousto-optical modulator crystal which is controlled by said 3D video signal through a signal forming unit . The apparatus according to the invention can be appropriate to reproduce colour spatial image, in which case it comprises multicolour laser sources or more, e.g. three laser sources of different basic wavelength . Either there is one optical element in each pixel and electronically copmensated deflection applied, or there are three optical elements arranged in each pixel to deflect or transmit the incident laser ray of corresponding wavelength to the various directions defining said field of view. A further preferred embodiment of the invention comprises: - control means for receiving 3D video signal, - a light emitting surface constituted by pixels, - spatially coherent elementary light sources, e .g. CSD-s or elementary lasers (e .g.) MSELDA arranged in said pixels, to emit coherent light rays of appropriate direction-related intensity to direct¬ ions defining a given field of view. In a preferred embodiment of the above apparatus each of said elementary lasers is associated with at least one of said directions defining said field of view. This feature can also be achieved so that there are optical elements adjusted in said pixels of the light emitting surface, each of said optical elements directing the laser ray emitted . by one of said elementary lasers to the direction said elementary laser is associated with . In another preferred embodiment the distances between adjacent elementary lasers are in order of magnitude of the light wavelength, so that the laser rays emitted by said elementary lasers interfere with each other in accordance with a holographic control of the whole set of said elementary lasers . The apparatus according to the invention can realize a three-dimensional television receiver or video or computer monitor comprising a closed receiver apparatus having 3D video input and/or arial input, wherein said laser sources, modulator an deflecting system are placed in the bottom part of the closed apparatus, said light emitting surface is arranged along the front face of the closed apparatus, and said deflecting system is connected with the optical elements of said light emitting surface through focusing scanner mirror optics arranged behind the light emitting surface, inside of said closed apparatus . BRIEF DESCRIPTION OF THE DRAWINGS The invention is illustrated hereinafter with reference to the accompanying drawings in which: FIGURE 1 is a block diagram of a system illustrating a way of carrying out of the invention; FIGURE 1A is a light intensity diagram of a laser beam modulated by the luminescence signal component of a 3D video signal; FIGURE IB is a voltage diagram of the luminescence signal component of a 3D video signal modulating a laser beam in the system of Fig. 1; FIGURE 2 is a schematic diagram of a preferred embodiment of the invention; FIGURE 3 is a schematic diagram of an embodiment of the deflection system and light emitting surface employed in a system according to the invention; FIGURE 4 is a schematic diagram illustrating the function mode of another preferred embodiment of the deflection system and light emitting surface; FFIGURES 5A and 5B are schematic diagrams illustrating the function mode of a pixel of the light emitting surface, in case of providing and not providing vertical parallax, respectively; FIGURE 6 is a schematic diagram illustrating the function mode of a preferred embodiment of the invention, providing no parallax, and the laser beam emitted from a pixel of the light emitting surface having a definite dispersion in vertical plane; FIGURE 7 is a block diagram of a further preferred embodiment of the invention; FIGURE 8 is a schematic perspective view and illustration of function of the apparatus of Fig. 7; FIGURES 9A and 9B are schematic diagrams illustrating two preferred way of modulating laser ray in a system according to the invention; FIGURES 10 A and 10B are schematic, partly block diagrams of preferred ways of carrying out the deflection of laser ray according to the invention; FIGURE 11 is a schematic view of the preriodical cylindric optical element employed in the deflection system of an apparatus according to the invention; FIGURE 12 is a schematic view of a holographic optical element arranged in a pixel of the light emitting surface of an embodiment of the invention; FIGURE 13 is a schematic diagram illustrating the function mode of a preferred way of carrying out of the invention; FIGURE 14 is a schematic top view of a part of the light emitting surface, illustrating a mode of function of an optical element arranged in a pixel of the light emitting surface; FIGURE 15 is a schematic top view of a light emitting surface, illustrating a three dimensional visual field achieved by the invention; FIGURE 16 is a schematic top view of an arcuate light emitting surface, providing a wider three dimen- sional visual field; FIGURE 17 is a schematic diagram of a preferred embodiment of the invention providing three dimensional colour picture; FIGURE 17 A is an enlarged front view of a pixel of the light emitting surface of the apparatus of Fig. 17; FIGURES 18A and 18B are schematic side sectional and front sectional views, respectively, of a three- dimensional television receiver set according to the invention; FIGURE 19a is a εchematical view of an apparatus for recording 3D video signal; FIGURE 19b is a schematic plan view illustrating the function of the apparatus for recording 3D video signal; FIGURE 19c is a schematic plan view illust- rating a display arrangement for displaying the recorded 3D video signal; FIGURES 20a and 20b are intensity diagrams of a two-dimensional and three-dimensional video signal, respectively; FIGURE 21 is a schematic perspective view of a part of an embodiment of the light emitting surface of a further embodiment of the invention; and FIGURE 22 is a schematic top view of pixels of the light emitting surface of Fig. 21 . DETAILED DESCRIPTION OF THE DRAWINGS Referring first to Fig. 1, an apparatus 10 for carrying out the invention comprises a laser and modulator unit 20, a separator unit 21, a deflection system 30 and a light emitting surface 40 having pixels 42 arranged in a defined configuration . The input signal is a 3D video signal which is separated by separator unit 21 to luminescence and colour signal component and synchronizing signal component . The synchronizing signals are applied to the control input of the deflection system 30, while the luminescence and colour signals control the laser and modulator unit 20, modulating a laser beam according to the three- dimensional picture information . From the output of laser and modulator unit 20 a modulated laser beam is applied to a deflection means 34 which directs the incoming laser beam by controlled deflection into the pixels 42 of the light emitting surface 40, into each pixel 42 subsequently after each other. The deflection system also comprises deflection means 36 providing a time controlled deflection of the laser beam arriving in the pixels 42 to various directions ii, i ∑ . . . i n of a given field of view. An essential feature of the invention is that the pixels 42 of the light emitting surface should emit laser beam to each direction with corresponding intensity and colour, in contrast with the two-dimensional screen, where the intensity and colour of the light emitted from any picture point is direction invarious. In order to achieve laser beam emission of dir- ection various intensity it is necessary to have the laser beam modulated corresponding to various direct¬ ions and have a deflection controlled in accordance with those directions . As illustrated in Fig. 1A and IB, respectively, the luminescence signal component of a 3D video signal, and so the modulated laser signal have time sections corresponding to the various picture points, i .e . pixels 42, and each section corresponding to any of the pixels has subsections, each associated with one of the directions ii, i . . .i n . For comparison purposes, Figs . 20a and 20b illu¬ strate a two-dimensional and a three-dimensional video signal, respectively. As seen in the figures, the 2D video signal is substantially constant within a section interval corresponding to a picture element, while the 3D video signal comprises subsections of different amplitude even within one section interval, each of said subsections corresponding to a definite view direction . In the embodiment of Fig. 2 the deflection system 30 comprises deflection means 36 composed of fibreglaεs-groups 37. Each pixel 42 is associated with one of the fibreglaεs-groups 37, each of them comprising a number of fibreglasses, which number is equal to the number n of directions i , i ∑ ••• in ' Tne modulated laser beam applied to the deflection means 34 is forwarded to the input and of said fibreglass- -groups 37 so that each section of the modulated laser beam corresponding to one of the pixels 42 arrives at the input of the fibreglass-group 37 which is associated with that of pixels 42. The end sectionε of the fibreglasseε are arranged εo that the laεer beam emitted from the fibreglaεεeε, that is emitted from the pixel is directed to the corresponding one of directions i , i . . . in - If necesεary, a correcting optical deflection can be employed in the pixels 42, in order to exactly meet the defined directions ij, 2 • • • i n . The function of the deflecting εyεtem illuεtrated in Fig. 3 basicly differs from the above embodiment . In this deflecting system the modulated laser beam arrives the pixels only deflected by deflection means 34, without being deflected according to the various directionε ij, i 2 . . . i n . Thiε εecond deflection iε carried out in the pixels 42, by means of active optical elementε, preferably acouεto-optical elementε, controlled by a radio- frequency generator 31 correεponding to the various directions ij, i ∑ . . . in - The input of the RF generator is driven by an appropriate saw-tooth signal . Fig. 4 shows a further posεible way to achieve deflection to the variouε directionε according to the invention . Passive optical deflection elements are arranged in the pixels 42. The modulated laεer beam εtrikes the pixels 42 parallel displaced in time, εo that the εubεectionε of the laεer signal corresponding to the different directions arrive the paεεive optical element in the pixel 42 in a defined shift position, εo that each εubεection of the laεer εignal will be deflected by the paεεive optical element to the correεponding one of εaid directonε . Fig. 5A illuεtrateε how the laεer beam, in time sequence, iε emitted from a pixel 42 to variouε directionε defining a three-dimenεional field of view, in caεe of producing three-dimenεional picture from a 3D video εignal compriεing vertical parallax. For εuch a three-dimenεional emiεεion optical elementε of εpherical εy metry or holographic optical elementε can be used. In the practice, however, the vertical parallax information may be omitted without significant restriction of the three-dimensional image, as illustrated in Fig. 5B. In order that the viewing height, i .e . the vertical position of the viewer' ε eyeε » - be not εo critical, the laεer beam modulated by a 3D video signal having no vertical parallax shall be emitted to various directions of a horizontal field of view, and dispersed in vertical planes, involving said directions as εhown in Fig. 6. For εuch purpoεe e .g. cylindrical optical elementε or holographic optical elementε are the appropriate deflection meanε . The block diagram of Fig. 7 baεicly differε from the εyεtem of Fig. 1 in that the light emitting εurface 40 of Fig. 7 iε a εeparate functional element, not part of the deflection εyεtem 30. Laεer and modulator unit 20 compriεeε a laεer εource 22 and a modulator 24, aε εhown in Fig. 8. Modulator 24 iε controlled by a lumineεcence and colour εignal component IN of the 3D video εignal . The modulated laser beam is deflected to the pixels 42 of the light emitting surface 40 and deflected or paralelly displaced corresponding to various view directions, according to a defined time sequence, by meanε of a deflection εyεtem 30 controlled by the εynchronizing εignal component SY of the 3D video εignal . Fig. 9 A εhowε a preferred embodiment of laεer and modulator unit 20, compriεing an integrated unit of a εemiconductor laεer diode 27 and chip 29 attached to forming opticε 28. The output εignal iε a modulated coherent laεer beam, the intenεity I of which being alεo illuεtrated in Fig. 9 A. Fig. 9B illustrates another preferred way of producing modulated laser beam, wherein a continuous laser source 22 sends laser beam to a modulator 24 carried out as acousto-optical crystal controlled by a 3D video signal through a radio- frequency generator 26. Fig. 10 A and 10B show preferred embodiments of a part of deflection εyεtem 30, providing εynchronized deflection of a modulated laεer beam L m to pixels 42 of the light emitting surface 40, according to a prescribed time sequence . In the exampleε the geometrical and εequential arrangement of the pixels 42 correεpondε to the picture element configuration of a standard two-dimensional televiεion εcreen, so the deflection unit 34 compriseε horizontal (line) deflection unit 33 and vertical (frame) deflection unit 32, εimilarly to the deflection εyεtem of known TV-ε . in Fig. lOA deflection unitε 32 and 33 are polygonal mirror arrangementε driven by precisely controlled motors not shown in the drawings . In Fig. 10B the horizontal and vertical deflections are provided by acousto-optical crystalε controlled by voltage-controlled oscillatorε 38 and 39, driven by εaw-tooth generators. Referring now to Figs . 11 and 12, optical elements 44 arranged in pixels 42 of the light emitting surface 40 are shown . In Fig. 11 optical elements 44 are realized as periodical cylindric-εymmetrical optics, while optical elementε of Fig. 12 are holographic opticε, such aε transmisεional relief hologramε . Holographic optical elementε are arranged on a planar carrier plate, preferably made out of coloured glaεε or plaεtic . In caεe of chooεing appropriate optical elements, the whole light emitting surface 40 can be produced by a single preεεing method. Aε illuεtrated in Fig 13, a modulated, focuεed laεer beam εtrikeε a pixel 42 εo that it arriveε, εhifted in time, at n different pointε of the holographic optical element 44 εet in the pixel 42. The direction to which the laεer beam iε emitted from the pixel 42 depends on where the laser beam strikeε the incidence surface of the optical element 44. As the point of incidence moves along the inner surface of the optical element 44, the direction of the emisεion of the laεer beam changeε between directionε ii and i n , εo that the emitted laεer beam εweepε along a field of view α, defined by said directions iι . . .i n . In order to achieve a continuous three- -dimenεional image the laεer beam emitted from a pixel to a defined direction εhall have a defined angle of divergence δ . In a εimple caεe for example the field of view α is equal to 90°, and there are 90 different directions ii, i ∑ • • • igo within the field of view, wherein the angle of divergence δ of the emitted laser beam shall be about 1°. Fig. 14 illustrates the function of another kind of light emitting surface 40. The deflection εyεtem provideε parallel diεplacement of the laεer beam εtriking the pixelε, εo that each relative poεition of the εtriking laεer beam within a pixel 42 correεpondε to one of the view directionε iι . . .i n . The laεer beam εtriking a given point of the optical element 44 in a pixel 42 at the moment tjζ will be deflected by the optical element in a direction 44 i^ correεponding to the point of incidence . As the point of incidence moveε along the surface of the optical element 44 in a pixel, the emitted laεer beam εweepε along the whole field of view α . Here the optical elementε are convergent opticε, while the εimilar εyεtem of Fig. 4 compriεeε divergent optical elementε . Figs . 15 and 16 illustrate the formation of the field V of full three-dimenεional viεual image . The field V is conεiderably ider in caεe of Fig. 16, where an arcuate, concave shaped light emitting εurface 41 iε employed. Similar feature can be simulated more practically by uεe of a plane εcreen having pixelε with changing propertieε . Referring now to Figε . 18 A and 18B, an example of a three dimenεional TV εet, carried out aε a preferred embodiment of the apparatuε according to the invention . The televiεion receiver apparatuε 12 compriεes a closed box having a front face realizing a screen-like light emitting surface 40. Inside the closed box there iε arranged focuεing εcanner mirror opticε 14 to reflect a modulated laεer beam into the pixels of said light emitting εurface 40. In the bottom part of the cloεed apparatuε there iε arranged a multicolour laεer and modulator unit 20 and deflection units of a deflection system 30. The apparatus can be used as a three-dimensional video or computer monitor with a 3D video input or as a television receiver with a 3D television signal/arial input . Figs . 17 and 17 A show by way of example only the principle of a three-dimenεional colour monitor accompliεhed according to the invention . The colour apparatuε compriεeε at leaεt three laser sources 22R, 22G and 22B, each of different basic wavelength (red, green and blue) . In the pixels 42 there are arranged above each other three deflecting optical elements 44R, 44G and 44B for each laser beam of different colour, to form and emit a light beam of definite colour to the corresponding directions . In a preferred embodiment the width of the optical elements 44R, 44G and 44B is about 0.5mm, while their height iε about 0.15 mm . Optical elementε 44R, 44G and 44B are preferably realized by holographic optical elementε . Figε . 19a and 19b illustrate a picture recording apparatuε for producing a 3D video εignal without vertical parallax, aε εhown in Fig. 20B . The apparatuε compriεeε a number of 2D recording cameraε Cl, C2 ... Cn, e .g. CCD chipε with optical εupplement arranged next to each other in horizontal plane in a fixed mutual poεition, in accordance with the view directionε of the diεplaying system, in a similar way as stereograms are recorded. The number of εaid cameraε iε equal to the number n of the view directionε . Pictureε of a εpatial figure or εcene are taken by the cameraε Cl, C2 ... Cn simultaneously from different view directions , and the 2D video signals recorded by the 2D cameras are subsequently ordered in a pre-defined way to achieve a 3D video signal format. During recording a virtual screen, marked by reference numeral 1 shall be considered, the relative position of which corresponding to that of the light emitting surface of the 3D display system, as illustrated in Figε . 19b and 19c, reεpectively . Fig. 19c demonεtrateε that the light εignal received from a εame point of the light emitting surface 40 by the left eye L of a viewer is different from the light εignal received by the right eye R. Fig. 21 and 22 illustrate the principle and function of a further way of carrying out the invention . In a light emitting εurface 40 ' compriεing pixelε 42, there iε a number of εpatially coherent elementary light εourceε, preferably elementary laεer s 50 arranged in each pixel 42 ' . The elementary lasers 50 are controlled to emit light signalε to each direction of the field of view. In a preferred embodiment each elementary laser 50 of a pixel 42 ' belongs to a defined view direction, being controlled by a 3D video signal to emit laser beam of corresponding intensity and colour to the related direction. In another poεεible embodiment the elementary laεerε 50 are mutually arranged so that the diεtanceε between adjacent elementary laεerε SO fall in the order of magnitude of light wavelength . In thiε caεe the elementary lasers 50 are controlled simultaneously in a holographic way, so that the light beamε emitted by said elementary sourceε interfere with each other to provide light beamε of correεponding intensity and co¬ lour to each direction, according to the 3D video signal control . Such holographic control programs are known per se . Fig. 22 shows that the direction of the light beams emitted by the elementary laserε 50 can be deflected to meet the deεired view direcionε by meanε of optical elementε 44 ' , locatd in the pixels 42 ' .

Claims: WHAT WE CLAIM IS: 1. Method for producing three-dimenεional picture, compriεing the εtepε of - modulating the intenεity of a εpatially coherent light ray, preferably a laεer ray by a 3D video εignal (video signal containing three-dimensional picture information) , and - directing the modulated laser ray by controlled deflection into pixels defining a light emitting surface, c h a r a c t e r i z e d in that the modulated laser ray is deflected to be emitted from every pixel of the light emitting εurface to a number of directionε, εaid directionε defining a given field of view, wherein said deflection to said various directionε is carried out so that the instant value of the intensity of said laser ray emitted from εaid pixelε in any of εaid directions of the field of view correεpondε to the information content of the 3D video signal related to the concerning direction . 2. Method as claimed in claim 1, wherein the modulated laεer ray iε deflected according to εaid directionε to εtrike the pixelε in εuch a dist¬ inguishing position that the incident time components of the laser ray shall be deflected through pasεive optical element/s/ to the directions they are associated with. 3. Method aε claimed in claim 1, wherein εaid modulated laεer ray iε deflected to εtrike the pixelε εo that the angleε of incidence of εaid incident time componentε correεpond to the direction they are associated with . 4. Method as claimed in claim 1, wherein the modulated laεer ray directed into the pixelε iε deflected and emitted through active, controlled optical elementε located in the pixelε to εaid variouε directionε of εaid field of view. 5.) Method aε claimed in any of claimε 1 to 4, wherein said modulated laεer ray iε directed into εaid pixelε by use of horizontal and vertical (frame) deflection according to TV εtandardε, said pixels being arranged so as to be conform with the standard TV picture point configuration . 6. ) Method as claimed in any of claimε 1 to 5, wherein the laεer beam iε modulated by a 3D video εignal having no vertical parallax information content, wherein εaid laεer beam emitted from a pixel horizontally εweepε along εaid field of view, εaid laser beam having a definite vertical dispersion . 7.) Method as claimed in any of claimε 2 or 5, wherein the modulated laεer ray incident in εaid pixelε iε deflected and directed through holographic optical element/ε/ or through periodical εpheric-εym- metrical optical element/ε/ to εaid directionε . 8.) Method aε claimed in claims 5 or 6, wherein the modulated laser ray incident in said pixels iε deflected and directed through holographic optical element/ε/ or through cylindric-εymmetrical optical element/ε/ to εaid directionε . 9. ) Method aε claimed in any of claimε 1 to 8, wherein εaid modulated laεer ray iε achieved by directly modulating a laεer source by said 3D video signal . 10. ) Method as claimed in any of claimε 1 to _- _- 8, wherein εaid modulated laεer ray is achieved by modulating CW laεer beam by acouεto-optical cryεtalε controlled by with εaid 3D video εignal . 11.) Method aε claimed in any of the preceeding claimε, wherein εaid modulated laεer ray iε directed into εaid pixelε by controlled mechanical or acouεto-optical deflecting means. 12.) Method aε claimed in claim 2 or , wherein εaid modulated laεer ray iε directed into εaid pixelε by use of mechanical or acousto-optical deflecting meanε controlled in accordance with εaid directionε of the field of view, εo that the angle of incidence of said modulated laεer ray, or the striking point where the modulated laser ray arrives in the pixel changes in accordance with said directions of the field of view. 13.) Method as claimed in claim 11, wherein said mechanical or acouεto-optical deflection is controlled by horizontal and vertical deflection information contained in the synchorinizing component of said 3D video signal . 14.) Method aε claimed in any of the preceeding claimε, wherein the width of εaid field of view iε 30 to 150°, wherein the number of εaid variouε directionε defining εaid field of view iε 30 to 150. 15. ) Method aε claimed in any of the preceeding claimε, wherein colour three-dimenεional picture iε produced by modulating three laεer rayε of different baεic wavelength, deflecting and directing them into εaid pixelε, and directing a laεer beam containing εaid three modulated laεer rayε of different baεic wavelength from each pixel in each direction of εaid field of view. 16. ) Method aε claimed in any of the preceeding claimε, wherein three dimenεional moving picture iε achieved by a definite number, preferably at least 20 picture repetitionε per εecondε . 17. ) Method aε claimed in any of the preceeding claimε, wherein the bandwidth of the 3D video εignal is reduced by use of any data- or information-compresεing process . 18.) Method as claimed in claim 1, wherein said 3D video εignal iε produced εo that two- dimenεional imageε of a εpatial εcene or figure to be recorded are taken εimultaneouεly from each of εaid directionε defining εaid field of view, and the 2D εignalε recording the different view imageε are arranged subsequently according to said directions in a 3D video signal format . 19. ) Method for producing three-dimensional picture, wherein spatially coherent elementary light sourceε, preferably elementary laser sourceε, constituting a light emitting εurface, are controlled by a 3D video εignal to emit light ray to a number of directionε, εaid directionε defining a given field of view in εuch a way that the intenεity of the light ray emitted to any of εaid variouε directionε corresponds to the information content of the 3D video signal related to the concerning direction. 20. ) Method as claimed in claim 19, wherein each of said elementary light εourceε iε aεεociated with one of εaid directionε, and controlled according to the direction it belongs to, the light emitted by said elementary light sources being directed to the aεεociated direction by use of optical means placed in the pixels of said light emitting surface . 21 . ) Method as claimed in claim 19, wherein the elementary laεer εourceε are controlled simultaneouεly in a holographic way, so that the laser beams sent to said directions are achieved by the interference of coherent light waves emitted by two or more elementary laεer εourceε . 22 . ) Method for producing three-dimenεional picture, wherein a coherent light beam, preferably a laser beam is modulated by a 3D video signal, and the modulated coherent light beam is directed into pixels arranged to define a light emitting surface, c h a r a c t e r i z e d in that the modulated light beam contains light rays each aεεociated with a view direction, εaid directionε defining a given field of view, εaid light rayε being modulated simulaneously , each light ray according to itε associated direction, and each component (light ray) of the modulated light beam being emitted from said pixels to the corresponding direction said component is aεεociated with . 23 . ) Apparatuε for producing three-dimenεional picture, comprising a spatially coherent light source, preferably laser source; a modulator to modulate laser ray produced by said light source, said modulator controlled by a 3D video εignal; a deflecting εystem to deflect modulated laser ray, controlled by the synchronizing εignal of the 3D video εignal; and a light emitting εurface compoεed of pixelε of definite mutual arrangement; c h a r a c a t e r i z e d in that there are optical elementε (44) adjuεted in said pixels (42) of the light emitting surface (40) to deflect and/or transmit incident laser ray from said pixels to various view directions (i . . . i n ) , said directions defining a given field of view (α) , and said deflecting εyεtem (30) iε controlled to deflect laεer ray in accordance with εaid directionε of the field of view ( ) into εaid pixels (42) . 24.) Apparatus as claimed in claim 23, wherein said deflecting system (30) involveε said optical elements (44) adjusted in the pixels (42) of the light emitting surface (40) , said optical elements (44) being acousto-optical elements controlled in accordance with the directions (ii . . . i n ) of said field of view (α) . 25.) Apparatus as claimed in claim 23, wherein εaid optical elements (44) are pasεive elementε of conεtant horizontal deflection characteriεtic and definite vertical diεperεion in vertical planeε . 26. ) Apparatuε aε claimed in claim 25, wherein said paεεive optical elementε (44) are vertical cylindric-optical elementε . 27. ) Apparatuε aε claimed in claim 25, wherein εaid paεεive optical elementε (44) are holographic optical elementε . 28.) Apparatuε aε claimed in claim 25 or 27, wherein said holographic optical elements (44) having vertical focus line, and light diεperεing in vertical planeε involving εaid vertical focuε line . 29.) Apparatuε aε claimed in any of claimε 25 to 28, wherein the deflection range of εaid deflect¬ ion εyεtem (30) correεpondε to the number and width of said optical elements (44) adjusted in said pixels (42) . 30.) Apparatus as claimed in claim 23, wherein said deflection system (30) compriεeε fibreglaεε groupε (37) , one for each pixel (42) , εaid fibreglaεε groupε (37) each having a number of fibreglaεses, which number iε equal to the number (n) of variouε directionε (i . . . i n ) defining εaid field of view ( ) , the input end of εaid fibreglaεε groupε (37) being attached to the output of a deflection unit (34) deflecting said modulated laser ray in accordance with the pixels (42) , the other end of said fibreglaεε groupε (37) being attached to the concerning one of said pixels (42) , the end εectionε of the fibreglaεses of εaid groupε (37) being adjuεted to direct laεer ray to the very direction (i^ . . . i n ) aεεociated with the correεpondϊng one of εaid fibreglaεεes . 31.) Apparatus as claimed in any of claims 23 to 30, wherein said pixelε (42) conεtituting a light emitting εurface (40) are arranged in conformity with the picture point configuration of a εtandard TV εcreen, and εaid deflection εyεtem (30) compriεeε ho¬ rizontal and vertical deflection unitε (32, 33) cont¬ rolled by the line εynchronizing εignal and frame εynchronizing signal, respectively, of the 3D video εignal . 32. ) Apparatus aε claimed in claimε 31, wherein εaid vertical deflection unit (32) and εaid horizontal deflection unit (33) compriεe acouεto- -optical cryεtalε controlled by voltage-controlled oscillators (38, 39) . 33.) Apparatus as claimed in any of the preceeding claims, wherein said laser source (22) , modulator (24) and deflection syεtem (30) are realized in an integrated optical unit . 34.) Apparatuε aε claimed in any of claimε 23 to 32, wherein εaid laser source (22) iε directed to an acousto-optical modulator crystal (24) controlled by said 3D video signal through a εignal forming unit (26) . 35. ) Apparatuε aε claimed in any of the preceeding claimε, compriεing multicolour laεer εource or more laεer εources (22R, 22G, 22B) of different basic wavelength, in which latter caεe there are more optical elementε (44R, 44G, 44B) arranged in εaid pixels (42) to deflect or transmit the incident laser ray of corresponding wavelength to the directions defining εaid field of view (α) . 36. ) A three-dimenεional television set com¬ prising a closed apparatuε (12) with a 3D video εignal input and/or arial input, c h a r a c t e r i z e d in that there iε a laεer εource (22) , a modulator (24) and a deflecting εyεtem (30) arranged in the cloεed apparatus (12) , and a light emitting surface (40) at the front face of the closed apparatus (12) , εaid deflecting εyεtem (30) providing deflection of laser beam produced by said laεer εource (22) into pixelε (42) of said light emitting εurface (40) , and a further deflection to direct laεer ray emitted from εaid pixelε (42) to variouε directionε defining a given field of view, under control of εynchronizing εignal correεponding to direction information of a 3D video εignal . 37. ) Apparatuε for producing three-dimenεional picture, compriεing control meanε for receiving 3D video εignal, c h a r a c t e r i z e d in that it further comprises a light emitting surface (40•) constituted by pixels (42*), and spatially coherent elementary light sources, such as controlled spontaneous-emission diode (CSD) , or preferably elementary lasers (50) arranged in said pixels, to emit highly directional light or laser ray in view directions (i^ ... i n ) defining a given field of view (α) . 38.) Apparatus as claimed in claim 37, wherein each of said elementary lasers (50) is associated with at least one of said directions (i^ ... i n ) defining said field of view (α) , and there are optical elements (44') adjusted in said pixels (42') of the light emitting surface (40'), each of said optical elements (44') directing the laser ray emitted by one of said elementary lasers (50) to the direction (ii ... i n ) said elementary laser (50) is associated with. 39.) Apparatus as claimed in claim 38, wherein the distances between adjacent elementary lasers (50) are in order of magnitude of the light wavelength, so that the laser rays emitted by said elementary lasers (50) interfere with each other in accordance with a holographic controlling of the whole set of said elementary lasers (50) .

Inventors: BALOGH TIBOR, BALOGH, TIBOR
Applicants: BALOGH TIBOR, BALOGH, TIBOR
Application year: 1993
Main classification: H04N13
IPC codes: G02B27, H04N13, H04N15