GB2265023A - Liquid crystal device; linear algebraic processor - Google Patents

Liquid crystal device; linear algebraic processor Download PDF

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Publication number
GB2265023A
GB2265023A GB9205160A GB9205160A GB2265023A GB 2265023 A GB2265023 A GB 2265023A GB 9205160 A GB9205160 A GB 9205160A GB 9205160 A GB9205160 A GB 9205160A GB 2265023 A GB2265023 A GB 2265023A
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Prior art keywords
liquid crystal
processor
optical
attenuation
polariser
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GB9205160D0 (en
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Michael Geraint Robinson
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Sharp Corp
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Sharp Corp
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    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL 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
    • G02F1/00Devices 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
    • G02F1/01Devices 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 
    • G02F1/13Devices 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
    • G02F1/133Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
    • G02F1/1333Constructional arrangements; Manufacturing methods
    • G02F1/1337Surface-induced orientation of the liquid crystal molecules, e.g. by alignment layers
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL 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
    • G02F1/00Devices 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
    • G02F1/01Devices 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 
    • G02F1/13Devices 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
    • G02F1/133Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
    • G02F1/1333Constructional arrangements; Manufacturing methods
    • G02F1/1343Electrodes
    • G02F1/13439Electrodes characterised by their electrical, optical, physical properties; materials therefor; method of making
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06NCOMPUTING ARRANGEMENTS BASED ON SPECIFIC COMPUTATIONAL MODELS
    • G06N3/00Computing arrangements based on biological models
    • G06N3/02Neural networks
    • G06N3/06Physical realisation, i.e. hardware implementation of neural networks, neurons or parts of neurons
    • G06N3/067Physical realisation, i.e. hardware implementation of neural networks, neurons or parts of neurons using optical means
    • G06N3/0675Physical realisation, i.e. hardware implementation of neural networks, neurons or parts of neurons using optical means using electro-optical, acousto-optical or opto-electronic means
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL 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
    • G02F1/00Devices 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
    • G02F1/01Devices 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 
    • G02F1/13Devices 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
    • G02F1/137Devices 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
    • G02F1/139Devices 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 orientation effects in which the liquid crystal remains transparent
    • G02F1/141Devices 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 orientation effects in which the liquid crystal remains transparent using ferroelectric liquid crystals

Abstract

A liquid crystal cell includes a polariser having an electrically insulating or semiconductive substrate having on its surface a series of ridges composed of a conductive material such as aluminium. The ridges act as an alignment layer and may also be connected to an electrical contact and are produced by oblique evaporation. A linear algebraic processor is formed by such a liquid crystal device 3 disposed between light emitting diode strips 4 and photodiode strips 8. Optical attentuation brought about by the liquid crystal device represents the values of an output vector while the outputs of the photodiodes represent the product of the input vector and the matrix. The processor may form part of a neural network. <IMAGE>

Description

MULTIPLYING DEVICE, LINEAR ALGEBRAIC PROCESSOR, NEUROMORPHIC PROCESSOR, OPTICAL PROCESSOR, LIQUID CRYSTAL DEVICE, AND METHOD OF MAKING A r LIQUID CRYSTAL DEVICE.
The present invention relates to a multiplying device, a linear algebraic processor, a neuromorphic processor, and an optical processor. The present invention also relates to a liquid crystal device and a method of making a liquid crystal device.
In the technical field of artificial intelligence, it is known to provide so-called "neural networks" which mimic the operation of small networks of neurones in an animal brain. Such neural networks include neuromorphic linear algebraic processors which are capable of being taught to perform various functions, for instance in the field of pattern recognition. The linear algebraic processors are required to perform vector matrix multiplications, effectively in parallel with the matrix elements being updatable effectively in parallel for the purpose of teaching the network to perform its intended function.
Although it is possible to simulate the operation of a neural network by means of a conventional programmed data processor, the speed of operation is severely limited because of the essentially serial operation of such arrangements. In order to overcome this problem, dedicated electronic devices have been provided in which the matrix multiplication and updating of matrix elements are performed in parallel. Such devices may employ digital circuitry, in which the matrix elements are stored inbinary format, or analog circuitry, in which conventional charge storage devices such as capacitors or charge coupled devices store the matrix elements.
However, semi-conductor devices of these types require relatively large silicon substrate areas for implementation and relatively large numbers interconnections for parallel updating.
An alternative type of processor is disclosed in an article entitled "GaAs/AlGaAs Optical Interconnection Chip for Neural Network" in the Japanese Journal of Applied Physics, Volume 28, No.11, November 1989, pages L2101 to L2103 by Y. Nitta, J. Ohta, K. Mitsunaga, M.
Takahashi, S. Tai and K. Kyuma. The device disclosed in this article uses arrays of light emitters and facing light detectors separated by a fixed mask of transparent and opaque regions. The elements of an input vector are applied to strips of light emitters whereas the elements of the output vector are formed by orthogonal strips of light detectors. Light from each element of each strip emitter is modulated or attenuated by the mask before being received by a facing portion of an orthogonal light detector, so that the matrix elements for the matrix multiplication are formed by the light transmissive properties of the elements of the mask. Thus, this arrangement is capable of performing a fixed algebraic operation but, after manufacture, cannot be adapted or taught to perform other operations.
According to a first aspect of the invention, there is provided a multiplying device comprising an electrooptical emitter, and opto-electric transducer, and a controllable attenuator having controllable non-volatile attenuation to optical radiation and being disposed between the emitter and the transducer.
It is thus possible to perform multiplication optically, for instance using visible light or infra-red radiation.
The emitter may be a semi-conductor light emitter, such as a light emitting diode. The detector may be a semiconductor photo-detector, such as a photo diode.
Preferably the controllable attenuator comprises a liquid crystal having non-volatile variable optical attenuation and means for varying the optical attenuation. The liquid crystal preferably has a substantially continuously variable optical attenuation. The liquid crystal may be a ferro-electric liquid crystal and the means for varying the optical attenuation may comprise electrodes for injecting charge into the ferro-electric liquid crystal. However, other types of liquid crystal may be used, such as anti-ferromagnetic liquid crystals and liquid crystal polymers.
According to a second aspect of the invention, there is provided a linear algebraic processor comprising a plurality of multiplying devices in accordance with the first aspect of the invention.
The multiplying devices may be arranged in a onedimensional array. The emitters of the multiplying devices may comprise portions of a strip emitter.
Alternatively, the transducers of the multiplying devices may comprise portions of a strip detector. Such processors may be used to perform multiplication operations on vectors.
The multiplying devices may be arranged in a twodimensional array. Such a processor may thus be used to perform matrix multiplication operations. The emitters of the multiplying devices may comprise portions of strip emitters aligned in a first of the dimensions of the array, so as to perform multiplication of an input vector by a matrix. The transducers of the multiplying devices may comprise portions of a strip detector aligned in a second of the dimensions of the array, so as to provide an output vector from a matrix multiplication.
According to a third aspect of the invention, there is provided a neuromorphic processor including a linear algebraic processor in accordance with the second aspect of the invention. Such a neuromorphic processor may be arranged to operate as a neural network, for instance by including means for performing a non-linear operation on the output of the linear algebraic processor.
According to a fourth aspect of the invention, there is provided an optical processor including an optical matrix attenuator having a plurality of cells, each of which comprises a controllable attenuator having controllable non-volatile attenuation to optical radiation and being disposed in an optical radiation pathway of the optical processor.
The controllable attenuator may comprise a liquid crystal having non-volatile variable optical attenuation and means for varying the optical attenuation. Preferably the liquid crystal has a substantially continuously variable optical attenuation. The liquid crystal may be a ferro-electric liquid crystal and the means for varying the optical attenuation may comprise electrodes for injecting charge into the ferro-electric liquid crystal.
Charge injection results in the switching of bistable domains such that the average transmission over the area of a matrix element can be incremented or decremented in a pseudo-analogue fashion. However, other types of liquid crystals, such as anti-ferromagnetic liquid crystals and liquid crystal polymers, may be used.
It is thus possible to provide devices and processors in which multiplication is performed optically by a coefficient which can be varied. In the case of processors employing a plurality of multiplying devices, vector and matrix multiplication may be performed in parallel with the elements or coefficients being adaptable. By using liquid crystals to store the elements in a non-volatile manner, very little power consumption is required in order to adapt and store the elements. Further, little or no electronic circuitry is required for these functions so that relatively small substrate areas on integrated circuits forming the processors are required.
Also, the interconnection requirements for parallel updating of the elements are relatively low, thus easing the packaging and external electrode needs.
According to a fifth aspect of the invention, there is provided a liquid crystal device comprising a liquid crystal and at least one polariser, the at least one polariser comprising an electrically insulative substrate having a plurality of substantially parallel surface ridges of an electrically conductive material formed by oblique evaporation deposition.
According to a sixth aspect of the invention, there is provided a method of making a liquid crystal device, comprising forming on at least one electrically insulating substrate a plurality of substantially parallel surface ridges of an electrically conductive material by oblique evaporation deposition to form at least one polariser, and assembling the polariser and a liquid crystal.
The polariser may also act as a liquid crystal alignment layer.
The electrically conductive material is preferably a metal, such as aluminium.
The substrate may be a semi-conductor, such as gallium arsenide, silicon or a compound of silicon. The substrate may be part of a monolithically integrated circuit and the polariser may be formed as part of the monolithic integrated circuit fabrication.
The electrically conductive material may be connected to an electrical contact.
The liquid crystal device may comprise first and second polarisers with a layer of liquid crystal disposed therebetween. In the case of certain liquid crystal devices, e.g. twisted nematic, the polarisers can act as alignment layers as the polarisers in such devices are aligned along the alignment direction.
It is thus possible to provide liquid crystal devices in which the conventional bulky polarisers can be replaced by thin polarising layers formed or coated at the interface between the liquid crystal and the substrate.
The electrically conductive material forms an optical grid which has high anisotropic electrical conductivity and is semi-transparent to certain optically polarised light. By using a metal such as aluminium, which has a resistivity approximately two orders of magnitude lower than that of indium tin oxide as normally used for liquid crystal electrodes, switching speeds of the optical properties of the liquid crystal can be increased.
In the case of ferro-electric liquid crystals, the contrast ratio can degrade over time because of the build up of charge over a conventional insulating alignment layer, such as polyvinyl alcohol. The use of a surface preparation of an electrically conductive material, which can be used as an electrode, can reduce this problem. In the case of ferro-electric liquid crystals, one polarising layer can act as an alignment layer with the other rotated by 2 x e from the alignment layer, where e is the smectic tilt angle.
The polariser can be formed during or after fabrication of a monolithic integrated circuit as the same or similar processing steps are required. For instance, the polariser may be formed as a surface layer or treatment of a substrate on top of or adjacent integrated electronic devices.
The invention will be further described, by way of example, with reference to the accompanying drawings, in which: Figure 1 is a schematic diagram of a neuromorphic linear algebraic processor constituting an embodiment of the invention; Figure 2 shows a cross section of the processor of Figure 1; Figure 3 illustrates schematically part of the lay out of an integrated circuit forming part of the processor of Figure 1; Figure 4 is a schematic circuit diagram of a portion of the part shown in Figure 3; and Figures 5 and 6 illustrate steps in the forming of polarisers of the processor of Figure 1.
The processor illustrated in Figure 1 comprises a semiconductor substrate 1, for instance made of gallium arsenide, on whose lower surface are formed parallel strips of light emitting diodes. The strips are connected to electrodes (not shown) for supplying current to the light emitting diode strips. The input currents may represent binary data such that, for instance, a binary 1 is represented by light emission and a binary zero is represented by no light emission. It is also possible for the current supplied to the electrodes, and hence the amount of light emitted by the light emitting diode strips, to represent analogue quantities. In either case, the input to the processor may be considered as an input vector whose elements are either binary digits or analog quantities.
The processor further comprises a semi-conductor substrate 2, for instance of gallium arsenide, on whose upper surface are formed light detectors 8 in the form of photo-diode strips arranged parallel to each other and orthogonal to the light emitting diode strips on the lower surface of the substrate 1. The photo-diode strips 8 are connected to electrodes (not shown) which provide output voltages or currents representing the elements of an output vector. These elements may also represent binary digits or analogue coefficients of the output vector, depending upon the application.
The processor further comprises a liquid crystal layer 3 disposed between the light emitting diode strips and the photo-diode strips 8. The liquid crystal layer 3 acts as a spatial light modulator and may be notionally divided into a rectangular grid of elements, each of which controls the attenuation of light travelling from a portion of a light emitting diode strip immediately above the element to a portion of a photo-detector strip 8 immediately below the element. The light attenuation properties of these matrix elements are individually adjustable and are non-volatile, so that the liquid crystal stores a matrix of coefficients whose values may be adapted or altered effectively in parallel.
Any liquid crystal having the appropriate properties may be used for the layer 3. For instance, the liquid crystal may comprise a ferro-electric liquid crystal with associated polarisers such that the light attenuation properties are non-volatile but may be altered by charge injection by means of electrodes disposed on opposite sides of the layer 3. However, other types of liquid crystal may be used, such as anti-ferromagnetic liquid crystals and liquid crystal polymers with appropriate means for altering or adapting the light attenuation properties of the matrix elements. It is also possible to use nematic liquid crystals but, as such liquid crystals have volatile light attenuation properties, further electronic circuitry would be required in order to produce non-volatile elements and this would increase the semi-conductor substrate area required and the interconnection requirement of the processor. Thus, at present, ferro-electric liquid crystals are preferred.
Figure 2 shows (not to scale) in more detail the structure of the processor. The section is taken perpendicular to the light emitting diode strips and longitudinally through one of the photodiode strips. The substrate 1 has formed therein elongate strips 4 representing the light emitting diode strips, together with associated structures 5, all of which are formed by conventional monolithic integrated circuit fabrication techniques. Insulating layers 6 cover the light emitting diode strips 4 and, together with layers 7, provide isolation from and alignment to the ferro-electric liquid crystal 3. The insulating layer 6 and the polarisation layer 7 are substantially transparent to the radiation, such as visible light or infra-red, of the desired polarisation emitted by the light emitting diode strips 4.
The photodiode strips 8 are likewise formed by conventional monolithic integrated circuit fabrication techniques on the surface of the substrate 2 and are covered by a polarisation layer 9 and an alignment layer 10. The layers 9 and 10 are likewise transparent to radiation of the desired polarisation from the light emitting diode strips 4.
The layers 7, 9, and 10 together with the ferro-electric liquid crystal 3 form part of the spatial optical modulator and co-operate with each other to provide adjustable non-volatile attenuation of the radiation passing from the light emitting diode strips 4 to the photodiode strips 8. Each of the layers 7 and 10 comprises an elongate electrode and an optical polariser whose structure and method of manufacture will be described in more detail hereinafter. The electrodes permit the application of suitable voltages for injecting charge into the ferro-electric liquid crystal 3 in order to vary its optical attenuation. The electrodes are arranged as a rectangular grid so as to permit the optical attenuation of each element to be adjusted independently of the other elements.The polarisations of the layers 7 and 9 co-operate with the adjustable optical polarisation rotation of the ferro-electric liquid crystal 3 to provide the variable attenuation.
In use, the processor shown in Figures 1 and 2 performs multiplication of an input vector by a matrix, the output appearing as an output vector. For use with digital input vectors, each element of the input vector has a value of 0 or 1 so that the light emitting diode strips 4 associated with the input vector elements having the value 1 are illuminated whereas those associated with the input vector elements having value 0 are not illuminated.
Each photodiode strip 8 sums the amount of optical radiation received from all of the light emitting diode strips 4 via the intervening matrix elements of the ferro-electric liquid crystal 3 and thus provides a signal representing the value of one element of the output vector. In practice, some cross-talk may occur i.e. some optical radiation may be received via matrix elements not directly above the photodiode strip.
However, such cross-talk is of a sufficiently low level not to be a problem for the sorts of applications for which the processor is intended.
Although the processor may be used simply as a matrix multiplication device, it is more likely to be used as part of a neural network, for instance for pattern recognition applications. This requires an initial process of teaching the neural network to respond in a predetermined way to certain input stimuli, and the teaching process is performed by adjusting the optical attenuation properties of the matrix elements formed by the liquid crystal layer 3. In order to perform this teaching process, a predetermined input vector is applied to the processor and the output vector from the photodiode strips is compared by associated circuitry, fabricated on one of the substrates 1 or 2 or on a separate substrate, with a target vector in order to calculate an error vector.The error vector components are then transformed into voltages which are then applied to the electrodes forming part of the layer 9.
Simultaneously, voltages representing the input vector elements are applied to the electrodes in the layer 7.
The resulting electric fields which appear across the liquid crystal matrix elements cause charge to be injected into the ferro-electric liquid crystal so as to alter its state by a finite positive or negative amount and hence to alter the light attenuation between facing portions of the light emitting diode strip 4 and the photodiode strip 8. This process is then repeated until the elements of the error vector are all zero or are below respective threshold values.
The usual update rule for matrix elements performed within an adaptable linear algebraic processor requires that the change in light attenuation of each matrix element should be proportional to the product of the element of the error vector supplied to the electrode on the photodiode layer and the element of the input vector supplied to the electrode on the light emitting diode strip. However, the field across the ferro-electric liquid crystal of the matrix element is in the form of the sum of a function of the error vector element and a function of the input vector element. In order to approach the ideal incremental or decremental change in optical attenuation, the input vector components may be supplied through a solid state switch which is switched off when no update is required i.e. when the input vector element is equal to zero.Such an arrangement is illustrated in Figures 3 and 4.
The light emitting diode strip 4 is fabricated as individual light emitting diodes for each of the matrix elements, the diodes being connected between a common line and an input vector element line 24. The electrodes of the layer 7 are likewise arranged as individual electrodes 20 connected via the source/drain paths of respective insulating gate field effect transistors 21 to an update voltage supply line 23. The gates of the field effect transistors 21 are connected to the line 24.
Thus, when the value of the input vector element associated with the line 24 is equal to one, the light emitting diodes of the strip 4 are illuminated and the field effect transistors 21 are turned on so as to permit updating of the associated matrix elements. However, when the input vector element has a value equal to zero, the light emitting diodes of the associated strip are extinguished and the field effect transistors 21 are turned off so as to isolate the electrodes 20. Thus, the electrodes of the strip are allowed to float to the potential of the opposite electrode on the photodiode strip so that negligible electric field is applied across the ferro-electric liquid crystal matrix element.
During updating of the matrix element, the line 23 receives the appropriate analogue positive, negative, or zero voltage so as to permit the appropriate change in the optical attenuation of the matrix element. This permits the optical attenuation to be incremented or decremented or to remain unchanged. The updated value of the optical attenuation is then held because of the nonvolatile properties of the ferro-electric liquid crystal.
Thus, very little electric power is required to alter and hold the optical attenuations of the matrix elements. It has been found that this non-volatile storage mechanism is possible through bistable domain formation associated with ferro-electric liquid crystal cell surface microscopic non-uniformity. By forming ferro-electric domains, the liquid crystal traps charge that can be incremented or decremented as described hereinbefore.
Thus, once it has been trained, the ferro-electric liquid crystal matrix elements store the analogue matrix values as non-volatile optical attenuation values and the processor may subsequently be used for fast parallel processing of data as part of a neural network or for other applications.
The processor as described hereinbefore and shown in the drawings may be used without substantial additional circuitry in various applications. For instance, it may be used as a mathematical co-processor to solve simple linear algebraic problems, or as a feature extractor and classifier for classifying input patterns by template matching. However, the processor may be used with associated electronic circuitry as part of a neural network. For instance, it may be used to perform vector matrix multiplications followed by non-linearities so as to provide a multi-layer perceptron. Also, more complex layered structures than those shown in the accompanying drawings may be provided.For instance, it is possible to provide a "single chip" implementation of multiple layer networks where optically encoded information passes in both directions through the ferro-electric liquid crystal, which requires optical sources or reflectors on both sides of the liquid crystal. It is also possible to provide a reciprocal chip architecture in which semiconductor diode structures are used for optical emission and detection. Such an arrangement permits the use of parallel back error propagation.
It is further possible to utilise the ferro-electric liquid crystal layer and the associated polarising and electrode layers in such a way that they form part of an optical processor not necessarily in direct contact with optical emitters and/or optical detectors. In this case, the matrix elements are disposed such that they are in optical pathways within the processor structure.
Figures 5 and 6 illustrate diagrammatically the steps in forming the layers 7 and 9. This technique is performed in a vacuum with aluminium being vaporised and being directed obliquely, as shown by the arrows in Figures 5 and 6, on to the surface of a surface region of the substrate 30. A build-up of material occurs due to shadowing effects and strips 33 are formed from the symmetry defined by the deposition angle. Oblique evaporation techniques are known, for instance SiO patent and polarising effects of strips of metallic material in an article in the journal of the Optical Society of America, Volume 50 Number 9, September 1960, by G.R. Bird and M. Parrish entitled "The Wire Grid as a Near-Infrared Polariser".
The spatial period of the grid or grating thus formed by the metal strips 33 is much less than the wavelength of light emitted by the light emitting diode strips 4, so that the strips 33 of aluminium have a greater conductivity in one direction parallel to the surface than in orthogonal directions. Thus, this structure acts as a polariser and as an alignment layer for the liquid crystal. Further, the aluminium strips 33 are connected together and to an electrical contact so as to form a switching contact for each of the liquid crystal cells.
These electrodes are in contact with the liquid crystal 3 and thus prevent the build up of charges which can affect the contrast ratio of the liquid crystal.
The layers 7 and 9 can be formed on top of other electronic structures formed within the substrates 1 and 2. For instance, once the electronic structures 5 have been formed, a layer of silicon may be deposited on the surface, oxidised to form the insulating layers 6 and 10, and processed as illustrated in Figures 5 and 6. These techniques are consistent with very large scale monolithic integrated circuit fabrication and allow a very fine optical grating to be formed and accurately aligned on the surfaces of the substrates 1 and 2. The orientations of the strips 33 may be the same for the whole surface. However, by using successive deposition and photolithographic steps, the directions of polarisations for different surface regions may differ from each other in accordance with the design requirements.
Although the structure and manufacture of the combined polariser, switching electrode, and surface treatment have been described with reference to use as the layers 7 and 9 in the processor of Figures 1 to 4, these techniques may be used for other types of liquid crystal devices. For instance, they may be used for liquid crystal display devices, spatial light modulators, and other types of semi-conductor/liquid crystal hybrid devices in which emitters and detectors may be directly above or below the liquid crystal modulator.

Claims (37)

CLAIMS.
1. A liquid crystal device comprising a liquid crystal and at least one polariser, the at least one polariser comprising an electrically insulative substrate having a plurality of substantially parallel surface ridges of an electrically conductive material formed by oblique evaporation deposition.
2. A device as claimed in Claim 1, in which the electrically conductive material is a metal.
3. A device as claimed in Claim 2, in which the metal is aluminium.
4. A device as claimed in any one of the preceding claims, in which the polariser is arranged to act as an alignment layer for the liquid crystal.
5. A device as claimed in any one of the preceding claims, in which the substrate is made of a semiconductor.
6. A device as claimed in any one of the preceding claims, in which the electrically conductive material is electrically connected to an electrical contact.
7. A device as claimed in any one of the preceding claims, in which the at least one polariser comprises first and second polarisers with the liquid crystal therebetween.
8. A method of making a liquid crystal device, comprising forming on at least one electrically insulating substrate a plurality of substantially parallel surface ridges, of an electrically conductive material by oblique evaporation deposition to form at least one polariser, and assembling the polariser and a liquid crystal.
9. A method as claimed in Claim 8, in which the electrically conductive material is a metal.
10. A method as claimed in Claim 9, in which the metal is aluminium.
11. A method as claimed in any one of Claims 8 to 10, in which the substrate is made of a semiconductor.
12. A method as claimed in any one of Claims 8 to 11, in which the electrically conductive material is electrically connected to an electrical contact.
13. A method as claimed in any one of Claims 8 to 12, comprising forming first and second polarisers and assembling the first and second polarisers with the liquid crystal therebetween.
14. A multiplying device comprising an electro-optical emitter, an opto-electric transducer, and a controllable attenuator having controllable non-volatile attenuation to optical radiation and being disposed between the emitter and the transducer.
15. A device as claimed in Claim 14, in which the emitter is a semiconductor light emitter.
16. A device as claimed in Claim 15, in which the semiconductor light emitter is a light emitting diode.
17. A device as claimed in any one of Claims 14 to 16, in which the transducer is a semiconductor photodetector.
18. A device as claimed in Claim 17, in which the semiconductor photodetector is a photodiode.
19. A device as claimed in any one of Claims 14 to 18, in which the controllable attenuator comprises a liquid crystal having non-volatile variable optical attenuation and means for varying the optical attenuation.
20. A device as claimed in Claim 19, in which the liquid crystal has a substantially continuously variable optical attenuation.
21. A device as claimed in Claim 19 or 20, in which the liquid crystal is a ferroelectric liquid crystal and the means for varying the optical attenuation comprise electrodes for injecting charge into the ferroelectric liquid crystal.
22. A linear algebraic processor comprising a plurality of multiplying devices as claimed in any one of Claims 14 to 21.
23. A processor as claimed in Claim 22, in which the multiplying devices are arranged in a one-dimensional array.
24. A processor as claimed in Claim 23, in which the emitters of the multiplying devices comprises portions of a strip emitter.
25. A processor as claimed in Claim 23, in which the transducers of the devices comprise portions of a strip detector.
26. A processor as claimed in Claim 22, in which the multiplying devices are arranged in a two-dimensional array.
27. A processor as claimed in Claim 26, in which the emitters of the multiplying devices comprise portions of strip emitters aligned in a first of the dimensions of the array.
28. A processor as claimed in Claim 26 or 27, in which the transducers of the multiplying devices comprise portions of a strip detector aligned in a second of the dimensions of the array.
29. A neuromorphic processor including a linear algebraic processor as claimed in any one of Claims 22 to 28.
30. An optical processor including an optical matrix attenuator having a plurality of cells, each of which comprises a controllable attenuator having controllable non-volatile attenuation to optical radiation and being disposed in an optical radiation pathway of the optical processor.
31. An optical processor as claimed in Claim 30, in which the controllable attenuator comprises a liquid crystal having non-volatile variable optical attenuation and means for varying the optical attenuation.
32. An optical processor as claimed in Claim 31, in which the liquid crystal has a substantially continuously variable optical attenuation.
33. A processor as claimed in Claim 31 or 32, in which the liquid crystal is a ferroelectric liquid crystal and the means for varying the optical attenuation comprise electrodes for injecting charge into the ferroelectric liquid crystal.
34. A linear algebraic processor substantially as hereinbefore described with reference to and as illustrated in Figures 1 to 4 of the accompanying drawings.
35. A device as claimed in any one of Claims 19 to 21 including a liquid crystal device as claimed in any one of Claims 1 to 7.
36. A processor as claimed in any one of Claims 22 to 29 when depended on any one of Claims 19 to 21, including a liquid crystal device as claimed in any one of Claims 1 to 7.
37. A processor as claimed in any one of Claims 31 to 33 including a liquid crystal device as claimed in any one of Claims 1 to 7.
GB9205160A 1992-03-10 1992-03-10 Liquid crystal device; linear algebraic processor Withdrawn GB2265023A (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8006144B2 (en) 2006-07-07 2011-08-23 Arm Limited Memory testing

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4213810A (en) * 1978-05-09 1980-07-22 Siemens Aktiengesellschaft Orientation layer for a liquid crystal display and method of manufacture
US4232947A (en) * 1974-07-01 1980-11-11 Sharp Kabushiki Kaisha Field effect mode liquid crystal display
US4256787A (en) * 1978-05-03 1981-03-17 Massachusetts Institute Of Technology Orientation of ordered liquids and their use in devices

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4232947A (en) * 1974-07-01 1980-11-11 Sharp Kabushiki Kaisha Field effect mode liquid crystal display
US4521080A (en) * 1974-07-01 1985-06-04 Sharp Kabushiki Kaisha Field effect mode liquid crystal display
US4256787A (en) * 1978-05-03 1981-03-17 Massachusetts Institute Of Technology Orientation of ordered liquids and their use in devices
US4370194A (en) * 1978-05-03 1983-01-25 Massachusetts Institute Of Technology Orientation of ordered liquids and their use in devices
US4213810A (en) * 1978-05-09 1980-07-22 Siemens Aktiengesellschaft Orientation layer for a liquid crystal display and method of manufacture

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8006144B2 (en) 2006-07-07 2011-08-23 Arm Limited Memory testing

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