WO2008151980A1 - Einrichtung zur amplituden- und phasemodulation von licht - Google Patents
Einrichtung zur amplituden- und phasemodulation von licht Download PDFInfo
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- WO2008151980A1 WO2008151980A1 PCT/EP2008/057000 EP2008057000W WO2008151980A1 WO 2008151980 A1 WO2008151980 A1 WO 2008151980A1 EP 2008057000 W EP2008057000 W EP 2008057000W WO 2008151980 A1 WO2008151980 A1 WO 2008151980A1
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- light
- molecules
- modulation
- modulating
- optical
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- 230000003287 optical effect Effects 0.000 claims abstract description 97
- 239000000463 material Substances 0.000 claims abstract description 30
- 230000001427 coherent effect Effects 0.000 claims abstract description 14
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- 238000005516 engineering process Methods 0.000 description 1
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- 239000002356 single layer Substances 0.000 description 1
Classifications
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
- G03H1/00—Holographic processes or apparatus using light, infrared or ultraviolet waves for obtaining holograms or for obtaining an image from them; Details peculiar thereto
- G03H1/02—Details of features involved during the holographic process; Replication of holograms without interference recording
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1343—Electrodes
- G02F1/134309—Electrodes characterised by their geometrical arrangement
- G02F1/134381—Hybrid switching mode, i.e. for applying an electric field with components parallel and orthogonal to the substrates
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/135—Liquid crystal cells structurally associated with a photoconducting or a ferro-electric layer, the properties of which can be optically or electrically varied
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/137—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering
- G02F1/13725—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering based on guest-host interaction
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/137—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering
- G02F1/13768—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering based on magneto-optical effects
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
- G03H1/00—Holographic processes or apparatus using light, infrared or ultraviolet waves for obtaining holograms or for obtaining an image from them; Details peculiar thereto
- G03H1/22—Processes or apparatus for obtaining an optical image from holograms
- G03H1/2294—Addressing the hologram to an active spatial light modulator
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
- G03H1/00—Holographic processes or apparatus using light, infrared or ultraviolet waves for obtaining holograms or for obtaining an image from them; Details peculiar thereto
- G03H1/02—Details of features involved during the holographic process; Replication of holograms without interference recording
- G03H2001/0208—Individual components other than the hologram
- G03H2001/0224—Active addressable light modulator, i.e. Spatial Light Modulator [SLM]
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
- G03H2225/00—Active addressable light modulator
- G03H2225/20—Nature, e.g. e-beam addressed
- G03H2225/22—Electrically addressed SLM [EA-SLM]
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
- G03H2225/00—Active addressable light modulator
- G03H2225/20—Nature, e.g. e-beam addressed
- G03H2225/25—Optically addressed SLM [OA-SLM]
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
- G03H2225/00—Active addressable light modulator
- G03H2225/30—Modulation
- G03H2225/33—Complex modulation
Definitions
- the invention relates to a device for light modulation with regularly arranged controllable light-modulating elements, which has a birefringent material for the modulation of phase and amplitude of a sufficiently coherent light wave whose molecular axes receive an orientation by the action of controllable forces.
- Field of application of the invention are light modulation means, e.g. flat spatial light modulators with high image display solution, which are used in display equipment for video and TV sets, projectors or similar devices for holographic reproduction.
- these devices can be used as a holographic display for holographic reconstruction of a scene.
- the holographic display can be both a direct view display and a projection display.
- the controllable elements may be the pixels of a light modulator.
- the present invention is to be seen in the context of a preferred real-time or near real-time holographic representation of a video.
- the video consists in the document of a plurality of scenes (frames), each of which is encoded as a hologram in the elements of the light modulation means.
- frames each of which is encoded as a hologram in the elements of the light modulation means.
- various methods are known which take into account the properties of the available light modulating means.
- the term "regularly arranged controllable elements” encompasses both the pixels of a light modulator and a continuously extending, non-pixelated coding surface of a light modulator, which is formally subdivided into discrete regions by the information to be displayed.
- holographic display is from earlier documents, e.g. (1) EP 1 563 346 A2, (2) DE 10 2004 063 838 A1 or (3) DE 10 2005 023 743 A1, known to the Applicant.
- a hologram computation is performed on the following basis:
- a three-dimensional scene is used for coding and holographic Reconstruct decomposed into a plurality of object points.
- the controllable elements change the amplitude and / or phase of the light to reconstruct each object point of the scene.
- Each object point is coded, for example, in a separate area of the coding surface of the light modulation means, which reconstructs this object point. This area is called the sub-hologram of this object point.
- the sub-hologram corresponds approximately to a holographically coded lens function that reconstructs this one object point at its focal point.
- the object point must be coded in the form of complex values.
- the amount of the complex values is approximately constant over the extent of the sub-hologram and depends in its height on the axial distance of the object point to the screen and on the intensity of the object point.
- the phase distribution of the complex values in the region of the sub-hologram corresponds approximately to the function of a lens whose focal length depends on the axial distance of the object point to the light modulation means or screen. Outside the sub-hologram, the value 0 is to be written in the light modulation means for this object point. Only the pixels of the light modulator within the sub-hologram contribute to the reconstruction of the single object point. The entire hologram is obtained by adding up the individual sub-holograms.
- the holographic reconstruction of the scene is generated, for example, in cooperation with a reconstruction optics in a reconstruction space that is spanned by the visibility area and the light modulation means. Wavefronts emanating from the holograms of the scene encoded in the light modulation means are superimposed in the visibility region and the reconstructed object points can be seen there from an eye position.
- the reconstruction from the superimposed modulated wavefronts is not simultaneously visible to both eyes of an observer. For each eye of an observer, in time or space multiplex, different perspective 3D representations of the scene are generated which differ in parallax but are seen by the brain as a single holographic 3D representation.
- the viewer can either look at a light modulation means, in which a hologram of the scene is coded directly and which serves as a screen. This is called a direct-view setup.
- the viewer may look at a screen onto which either an image or a transform of the hologram values encoded in the light modulation means is projected. This is called projection construction.
- the eye positions of observers are determined in a known manner by a position finder, which is program-technically coupled to a computing unit
- a hologram of the scene which may also be computer-generated and whose values are stored in a memory unit as a look-up table
- complex numbers or complex values for each object point are entered in the arithmetic unit, which are written into the light modulation means must be coded.
- the complex values are coded into the pixels of a spatial light modulator (SLM) in the case of a pixelated SLM or, in the case of a non-pixelated SLM, into a continuously extending coding surface which is formally divided into discrete regions by the respective information to be displayed.
- SLM spatial light modulator
- SLMs For modulating the incident coherent light waves, SLMs are known which perform only a modulation of the phase of the light waves and those which only effect a modulation of the amplitude. Furthermore, there are also SLMs that perform a coupled amplitude / phase modulation. Certain fixed combinations of amplitude and phase values - but not arbitrary complex values - can be written into this SLM.
- Document US 5 719 650 describes a light modulator for independently controlling amplitude and phase. It consists of two polarization rotating elements, each with a liquid crystal layer, which are each arranged between two carrier substrate plates. The base electrodes and the grid electrodes are also available separately for each layer. An adjustment of the elements to each other is already performed in the manufacturing phase. However, there is currently no single SLM consisting of only one liquid crystal layer into which the complex-valued information of a holographic scene can be written directly and modulated with light.
- a light modulator is known to be based on the use of liquid crystals (LC).
- LC liquid crystals
- Liquid crystals are birefringent materials in which the orientation of the optical axis of the molecules can be adjusted in a desired direction, e.g. through an electric field.
- the optical axis corresponds to the longitudinal axis of a molecule.
- the modulation of the incident light in such a light modulator depends on the direction of adjustment of the optical axes of the molecules relative to the direction of passage through the light modulator and on the polarization of the light.
- LC light modulators are known, which are to be used either as amplitude modulators or as phase modulators.
- Patent EP 0583114 describes an optically addressable SLM (OASLM). It contains a photoconductive layer in addition to the liquid crystal layer and the electrodes. By means of write light falling on the SLM, the conductivity of the photoconductive layer is changed as a function of the intensity of the writing light. When an electric field is applied across the electrodes and the photoconductive layer, the photoconductive layer is affected due to its conductivity set by the writing light, the field applied to the liquid crystal layer. The alignment of the molecules of the liquid crystal layer is carried out according to the set electric field and then serves to modulate the sufficiently coherent reading light. While an individual drive voltage must be addressed for each pixel in an EASLM, the OASLM has a fixed drive voltage and the local alignment of the molecules takes place via the write light. Nevertheless, a conventional OASLM can only be used to modulate either the phase or the amplitude of the reading light.
- phase and amplitude can not be modulated independently of each other, because typically only one parameter can be varied with an electric field generated at the LC layer or a similarly effective force to influence the liquid crystal molecules. This will be explained in more detail below with reference to FIGS. 1 for a phase modulation and FIG. 2 for an amplitude modulation.
- the pixel P is shown with a frame and comprises a birefringent
- Material for example a liquid crystal layer LC with molecules M, on which almost coherent light falls. Since the direction of light incidence perpendicular to
- the molecules M can be seen in the plan view of Fig. 1a in a starting position in the off state of the phase modulator.
- the incident light is vertically polarized, indicated by the double arrow, and the optical axes of the
- Molecules M are aligned parallel to the incident light.
- FIGS. 1 b and 1 c schematically show the pixel P in the switched-on state of the phase modulator at a medium voltage.
- Axes of the molecules M are by the applied voltage V by a certain Angles have been oriented out of the plane. At an applied maximum tension, alignment of the axes would be perpendicular to the plane.
- the liquid crystal layer LC is enclosed according to FIG. 1c by two mutually opposite carrier substrates TS, eg glass.
- the molecules M are controlled by generating an electric field between opposing electrodes E1 and E2 in their optical properties. The direction of incidence of the light is indicated by arrows.
- the applied voltage V does not change the polarization direction of the light, but the phase of the light is affected by the orientation of the optical axes of the molecules M.
- FIGS. 2 a and 2 b show, analogously to FIG. 1, the plan view of a pixel P, while FIG. 2 c shows the side view.
- the orientation of the optical axes of the molecules M as well as the polarization PO of the incident light in the switched-off state of the pixel P in FIG. 2a correspond to those in FIG. 1a.
- the electrodes E1 and E2 are arranged differently.
- the applied voltage V acts in this case from left to right, while there is no electric field in the representation of the side view.
- This drawing is roughly schematic. Since, as a rule, the lateral extent of a pixel is greater than a few micrometers, usually the transverse electrode is subdivided once again so as not to apply excessive voltages. So there are several electrodes per pixel connected in series. For better clarity, however, only 2 electrodes are shown.
- Fig. 2b and 2c the pixel P is shown in the on state.
- a mean voltage V a rotation of the optical axes of the molecules M in Fig. 2b in the plane, recognizable by the slight inclination of the molecules M.
- Fig. 2c takes place according to Fig. 2c from the plane of plan view out no rotation of the molecular axes .
- the incident light is rotated in its polarization by the alignment of the optical axes of the molecules M by applying a voltage V at a predetermined thickness of the liquid crystal layer LC from the value PO1 by a certain angle in the position PO2.
- the size of the rotation angle is twice the angle between the polarization PO of the incident light and the caused alignment of the optical axes of the molecules M.
- the amplitude of the light be modulated.
- a maximum amplitude and with applied voltage and a rotation of the optical axis of the molecules by 45 ° - thus a polarization rotation by 90 ° - an amplitude of 0.
- the incident light waves can always be modulated only with a proportion of a complex value.
- the pixels of both SLM would have to be congruent with each other so that the light passes through two correspondingly assigned pixels. Due to the unavoidable distance between the LC layers, however, this condition is no longer satisfied even for small angles of the incident light rays, in particular in oblique passage through the SLM. But even in the case of vertical light incidence, e.g. an inaccurate adjustment of the light source associated with the two pixels will result in a passage of the light through respective different pixels in both SLMs.
- the object of the invention is to avoid the stated disadvantages of the prior art in presenting complex hologram values and to simplify the modulation of light waves in phase and amplitude in a single light modulation device.
- the invention is based on a device with regularly arranged controllable light-modulating elements, which has a birefringent material in molecular form for modulating the phase and amplitude of a sufficiently coherent light wave, wherein a modulation control controls a force-induced alignment of the optical axes of the molecules.
- controllable means which align the optical axes of the molecules in the light-modulating elements independently in two dimensions, as well as a polarizer arranged on the output side,
- the birefringent material consists of a single layer of liquid crystals.
- Alignment of the optical axes of the molecules may be accomplished by two externally-controllable means according to a feature of the invention. These can act in a stepwise controllable manner on the optical axes of the molecules and so independently set two angles of projection of the optical axes of the birefringent material into two different mutually perpendicular planes.
- At least one of the externally acting means is an electric field. In a second embodiment of the means, at least one of the externally acting means is a magnetic field.
- At least one axis of the molecules is aligned by optical means.
- Another essential feature of the invention is that two means generating an electric or magnetic field are arranged approximately perpendicular to each other on each of a light modulating element in the light modulator.
- the layer of liquid crystal or other birefringent material is doped with dye molecules and alignment in one plane is accomplished by varying the polarization of writing light falling on the device. Alignment in the other plane is achieved by generating an electric or magnetic field .
- the alignment of the optical axes of the molecules in a plane takes place by varying the intensity of incident writing light.
- the device additionally includes a layer of photoconductive material which reacts to the writing light. For alignment in the other plane, an electric or magnetic field can be generated again.
- the device is a spatial light modulation means with light-modulating elements. If a hologram of a scene is inscribed in these elements and if the device additionally contains a lighting unit and an optical system, then it can be used to reproduce the holographic scenes. Such trained devices can be used as light modulators in a holographic display.
- the light-modulating elements are pixels and the means for aligning the pixels are pairwise aligned for two-level alignment to concurrently modulate the incident light pixel by pixel with phase and amplitude.
- the object is further achieved by a method of light modulation using a device comprising a birefringent material in molecular form with a regular array of controllable light modulating elements for modulating the amplitude and phase of sufficiently coherent lightwaves, the optical axes of the molecules being affected by the action of Forces, controlled by a modulation control, be aligned.
- the method is characterized in that the optical axes of the molecules are aligned independently of one another in two dimensions by controllable means acting externally on the light-modulating elements and a polarizer arranged on the output side is provided.
- the alignment of the axes of the molecules is carried out in process steps by two externally acting, independently controllable means.
- the alignment of the axes is continuously controlled.
- a hologram of a scene is written in the device designed as a spatial light modulation means. If a lighting unit illuminates the hologram, then a holographic reconstruction of the scene can be generated together with an optical system and the components together realize a holographic display means.
- two electric fields, perpendicular to one another and in their strength independently adjustable electrical fields act on the optical molecular axes, so as to achieve the simultaneous modulation of the incident light in phase and amplitude.
- two magnetic fields which act perpendicular to one another and can be adjusted independently of one another can also act on the optical molecule axes and change their orientations. It is also possible to use a combination of an electrical and a perpendicular magnetic field to align the optical molecular axes. However, other combinations of the mentioned in the Einhachtungst means for aligning the optical axes of the molecules can be used in the process.
- optical molecule axes in the plane of the light modulation means can also be aligned optically, for example by photoalignment, by means of polarized writing light in the dye-molecule doped doubly refractive material and in a plane perpendicular thereto by the action of an electric or magnetic field , If the device already contains an illumination means with at least one linearly polarized light source, then the polarization of the light source replaces the function of a polarizer to be arranged on the light entry surface. In this case, the polarization of the writing light can be varied without causing any disturbing effects by the polarizer.
- Another possibility for using polarized writing light is a reflection of the wavelength of the reading light light modulator, which can be described from the back.
- a holographic display can be realized to produce a holographic reconstruction.
- the holographic display device has a light modulation device with a light modulator means with regularly arranged pixels and a liquid crystal layer whose optical molecular axes for modulating the phase and amplitude of sufficiently coherent light waves of a lighting unit independently of each other two-dimensionally by externally acting on the pixels controllable means according to the aforementioned examples by a Modulation control are aligned to simultaneously modulate resulting phase and amplitude values of a holographically encoded 3D scene, wherein the holographic display device further comprises an optical system for reconstructing the 3D scene in a reconstruction space with the modulated light modulated light waves.
- the coding of calculated complex hologram values of a 3D scene and the modulation of incident coherent light waves with phase and amplitude values can be simplified since only a single SLM with a single liquid crystal layer is needed.
- the prior art uses a combination of several SLMs or an SLM with multiple independent liquid crystal layers.
- a further advantage results from the fact that, in comparison to solutions with several SLMs, disturbing effects in the propagation of the light between the individual LC and carrier layers are avoided.
- 1 a is a top view of a pixel of an SLM with molecules of a
- 1 b is a plan view of a pixel of an SLM with molecules of a
- FIG. 1 c is a side view of FIG. 1 b
- 2a is a plan view of a pixel of an SLM with molecules of a
- Fig. 2b is a top view of a pixel of an SLM with molecules of a
- Liquid crystal layer in the on state, for amplitude modulation according to the prior art
- FIG. 2c is a side view of Fig. 2b
- Fig. 3a is a plan view of a pixel of an SLM with molecules of a liquid crystal layer in the off state according to the
- FIG. 3b is a side view 1 to Fig. 3a
- FIG. 3c shows a comparison with FIG. 3b rotated by 90 ° side view 2
- Fig. 3d is a plan view of a pixel of an SLM with molecules of a liquid crystal layer in the on state
- FIG. 3f shows a side view 2 rotated by 90 ° with respect to FIG. 3e, FIG.
- 4a is a plan view of a pixel of an SLM with molecules of a
- Liquid crystal layer with optical alignment of the molecules 4b is a side view of Fig. 4a,
- FIG. 5a is a side view of an optical-alignment pixel of FIG.
- 6 is a graphical representation of amplitude and phase combinations as complex valued modulations.
- Light modulation means are formed with their pixelated Kodier materials either transmissive or reflective and consist of a regular array of pixels with finite extent, which are due to production separated by gaps.
- the coding surface is e.g. traversed by a grid of thin electrodes, between which the pixels are at a pixel distance from each other.
- the electrodes are switched by a control unit, in particular by means of a computer with programmatic means located therein, so that the pixels are encoded in amplitude and phase with regard to transparency or reflection.
- the transmissive pixels encoded with complex values pass the incident light waves while the reflection pixels reflect the light waves.
- the presentation of optical / lighting technology and other electrical / electronic means is omitted for clarity.
- the invention is based on the following consideration:
- a birefringent material is suitable because it consists of molecules with two optical axes acting in two different planes.
- the optical axes of the molecules In order to be able to independently influence the phase and amplitude of the light waves, the optical axes of the molecules must be able to be aligned independently of one another in two dimensions. This happens on the following basis: When you enter the birefringent matter! Places a cutting plane and in this cutting plane a coordinate axis, then forms the geometric projection of the optical axis in this cutting plane at an angle with the coordinate axis. This angle can be changed by moving the optical axis of the molecules in this plane.
- the geometric projection of the optical axis also forms an angle with this coordinate axis.
- a change in these two angles independently corresponds to an independent two-dimensional alignment of the optical axes of the molecules according to the invention.
- the alignment of the optical axes is generally combined with the polarization of the incident light.
- a polarizer is placed in front of the light modulator. If linearly polarized light sources are used for illumination, the polarization of the light source itself takes the place of the polarizer.
- This path difference depends on the one hand on the thickness of the traversed layer. On the other hand, it can also be influenced by a rotation of the LC molecules out of this plane.
- the path difference between the two Components lower.
- elliptically polarized light may be generated in the general case after passing through the LC layer.
- a polarizer after the LC layer transmits only a portion thereof, which is then linearly polarized. This has a defined amplitude A and a defined phase delay ⁇ .
- An optical path difference of a wavelength ⁇ generally corresponds to a phase delay ⁇ of 2 ⁇ . It is dependent on the birefringence ⁇ n and the layer thickness d of the LC layer according to the equation
- n the refractive index is parallel and ru the refractive index perpendicular to the optical axis of the molecules.
- ⁇ is the phase delay of the light resulting from the plane, depending on the thickness of the LC layer and the angle ⁇ of the optical axes of the molecules, and with ⁇ the angle of rotation of the molecules relative to the polarization direction of the light before entering the LC layer.
- the variation of both parameters ⁇ and ⁇ then allows a complex-valued modulation of the light.
- a pixel-wise modulation control preferably takes place in a transmissive light modulation means having a liquid crystal layer LC, wherein at least two electrodes E1 and E2 for the function-dependent control of the molecules M are effective for a pixel P.
- the alignment of the optical axes of the molecules M of the liquid crystal layer LC is also performed pixel by pixel. If that does not apply, it will be pointed out.
- means for generating electric fields are used for the pixel-wise alignment of the optical axes of the molecules.
- a transmissive light modulator is shown in fragmentary form in the form of a pixel P in the switched-off state.
- the top view shows molecules M of the liquid crystal layer LC in a plane between two mutually perpendicular electrodes E1 and E2 for functionally controlled control of the molecules M.
- a vertical polarization PO of the incident light in the pixel P is indicated by a double arrow.
- the alignment of the optical axes of the molecules M 1, the vertical polarization PO and the direction of incidence of coherent light are consistent with the types of light modulators described in the prior art.
- FIGS. 3b and 3c show the side views 1 and 2 for the molecules M in the pixel P in the switched-off state.
- the arrows indicate the light incidence direction.
- the rotated by 90 ° side view 2 is now also shown for clarity.
- FIG. 3d The drawings of Figs. 3d to 3f show the on state of a pixel P according to the first embodiment.
- the two opposing electrodes E1 and E2 which can be controlled independently of one another by a modulation control, generate two electric fields for aligning the molecules.
- the optical axes of the molecules M in the pixel P are rotated within the one plane by rotation through the angle ⁇ (see Fig. 3d) and rotated by the angle ⁇ within the other plane.
- These angles of rotation ⁇ and ⁇ influence both the amplitude and the phase of incident light waves, as can be seen from the equations given above.
- the rotation angle ⁇ of the optical axes of the molecules produced by the applied voltage is indicated which acts in the other plane.
- FIG. 3f shows in the side view 2 rotated by 90 ° to FIG. 3e the pixel P with 4 voltage values VO, Va, Vb and Va + Vb as side view 2.
- the left lower electrode has the voltage value VO and the left upper electrode the voltage value vb. Between the left and right side can the voltage Va-VO abut, between the bottom and top, the voltage Vb-VO. The upper right electrode then has the voltage value Va + Vb.
- the optical axes of the molecules of the pixel P can be aligned in both dimensions-in plan view and side view. The alignment of the optical axes modulates the amplitude and phase of the transmitted light.
- FIGS. 3 a and 3 d can also be replaced by a plurality of series-connected individual electrodes via a pixel in order to take account of the different lateral extent and thickness extent of a pixel.
- magnetic fields acting perpendicular to one another can be generated in a second embodiment of the means, which is not shown in more detail.
- the means for this may be arranged analogously to the arrangement for generating the electric fields in order to align the optical axes of the molecules independently of one another in two planes.
- optical means and / or methods for aligning the optical axes of molecules can be used.
- the photoalignment is used, in which the molecules in the display plane are optically aligned in a light modulator with birefringent material.
- a liquid crystal layer is doped with dye molecules and the optical axes of the molecules align themselves with the polarization of incident writing light.
- Such light modulators are known as so-called dye-doped optically addressable spatial light modulators (English: dye-doped OASLM).
- the writing light falling from a light source onto the light modulator can be incoherent light.
- the optical axes of the molecules are aligned with an electric field by conventional electrodes.
- Such light modulators are known as EASLM.
- FIG. 4 a shows an example of a combination of an OASLM and an EASLM as a detail at a pixel P in plan view.
- the molecules M can be seen with a slight rotation out of the one plane. They are aligned perpendicular to the polarization direction of the writing light POS. With writing light here incident light for influencing the orientation of the molecules M in the liquid crystal layer LC is referred to.
- Reading light is the light modulated by the light modulator. It has in this example a vertical polarization POL, characterized by the double arrow outside the pixel P 1, and may also be different in its further properties and in the wavelength from the reading light. A polarizer in the plane of incidence of the light modulator is not necessary.
- FIG. 4b shows in side view the orientation of the molecules M in the other plane perpendicular to FIG. 4a, which is generated here by means of an electric field.
- the molecules are rotated more out of the plane in comparison to the plane in FIG. 4 a by the modulation control in accordance with the complex value to be represented here.
- the electrode structure and the electrical addressing of the light modulator and the arrangement of the carrier substrates TS, illustrated at the pixel P, are in accordance with a conventional liquid crystal modulator.
- the direction of incidence of the reading light is indicated by the dotted arrow.
- a light modulator includes a photoconductive layer in addition to the liquid crystal layer.
- FIG. 5 a again shows, as a section of a light modulator, a pixel P in side view with molecules M in the liquid crystal layer LC, the electrodes E1 and E2, the carrier substrates TS and the photoconductive layer PS. The molecules can be seen in the starting position.
- This figure indicates the writing operation in the pixel P and the broken arrows indicate which direction the writing light falls on the photoconductive layer PS.
- the conductivity of the photoconductive layer PS is changed.
- FIG. 6 shows in a graphical representation combinations of amplitude and phase values as complex-valued modulations on a light modulator falling light waves.
- the horizontal axis contains relative amplitudes between 0 and 1
- the vertical axis contains phases between 0 and 2 ⁇ r.
- the plotted points represent examples of various complex numbers with the respective amplitude and phase, which can be set via different combinations of the parameters ⁇ and ⁇ .
- the invention can be used both in pixelated and non-pixelated light modulators. If at least one of the means generates an electric field for aligning the axes of the molecules, the light modulator must be pixelated, that is also in a combination of electrical and optical alignment.
- a non-pixelized light modulator to which a pixel structure from the outside is formally imprinted by the information to be respectively displayed.
- an arrangement with two writing light beams may be used, one of which, by varying the intensity of the writing light, makes the alignment of the molecules in one plane and the other writing light beam through the polarization the alignment in the other plane.
- a hologram of a three-dimensional scene is encoded.
- a lighting unit with a nearly coherently radiating light source illuminates the light modulator.
- Modulation control causes the incident light to be modulated independently of one another in two different amplitude and phase planes by appropriate alignment of the molecules of the liquid crystal layer. Together with an optical system will reconstructed the scene in a reconstruction room with the modulated light waves.
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- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Holo Graphy (AREA)
- Liquid Crystal (AREA)
- Polarising Elements (AREA)
- Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
Abstract
Description
Claims
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KR1020107000812A KR101505927B1 (ko) | 2007-06-13 | 2008-06-05 | 광의 진폭 및 위상 변조 장치 |
JP2010511587A JP5409611B2 (ja) | 2007-06-13 | 2008-06-05 | 光変調用装置 |
CN2008801027019A CN101779168B (zh) | 2007-06-13 | 2008-06-05 | 用于光调幅和调相的装置 |
US12/663,649 US8687252B2 (en) | 2007-06-13 | 2008-06-05 | Device for light modulation |
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DE102007028371.9 | 2007-06-13 | ||
DE102007028371A DE102007028371B4 (de) | 2007-06-13 | 2007-06-13 | Einrichtung zur Lichtmodulation |
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WO2008151980A1 true WO2008151980A1 (de) | 2008-12-18 |
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PCT/EP2008/057000 WO2008151980A1 (de) | 2007-06-13 | 2008-06-05 | Einrichtung zur amplituden- und phasemodulation von licht |
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US (1) | US8687252B2 (de) |
JP (1) | JP5409611B2 (de) |
KR (1) | KR101505927B1 (de) |
CN (1) | CN101779168B (de) |
DE (1) | DE102007028371B4 (de) |
TW (1) | TWI409532B (de) |
WO (1) | WO2008151980A1 (de) |
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WO2020035206A1 (de) | 2018-08-16 | 2020-02-20 | Seereal Technologies S.A. | Lichtmodulationsvorrichtung |
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WO2020035206A1 (de) | 2018-08-16 | 2020-02-20 | Seereal Technologies S.A. | Lichtmodulationsvorrichtung |
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JP2010530080A (ja) | 2010-09-02 |
CN101779168A (zh) | 2010-07-14 |
DE102007028371B4 (de) | 2012-05-16 |
JP5409611B2 (ja) | 2014-02-05 |
US8687252B2 (en) | 2014-04-01 |
CN101779168B (zh) | 2013-08-21 |
DE102007028371A1 (de) | 2009-01-22 |
US20100195178A1 (en) | 2010-08-05 |
KR20100038101A (ko) | 2010-04-12 |
KR101505927B1 (ko) | 2015-03-25 |
TWI409532B (zh) | 2013-09-21 |
TW200918996A (en) | 2009-05-01 |
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