序号 专利名 申请号 申请日 公开(公告)号 公开(公告)日 发明人
121 PARAMETRIC TERAHERTZ RADIATION GENERATION EP10010843.0 2005-07-26 EP2309325B1 2018-05-30 Rae, Cameron Francis; Dunn, Malcolm Harry; Terry, Jonathan A.C.
An optical parametric device, for example an optical parametric generator or amplifier or oscillator, comprising a non-linear material that is operable to generate a signal and an idler wave in response to being stimulated with a pump wave, wherein the pump wave source and the non-linear medium are provided in the same optical cavity and the non-linear medium is such that the pump, idler and signal waves are non-collinear. Alternatively, the non-linear medium is provided in an optical cavity that resonates the pump wave, and the pump wave and the generated idler and signal waves are non-collinear.
122 OPTICAL PHASED ARRAY USING STACKED PARALLEL PLATE WAVE GUIDES AND METHOD OF FABRICATING ARRAYS OF STACKED PARALLEL PLATE WAVEGUIDES EP15840748 2015-09-01 EP3191890A4 2018-05-16 RUSSO PETER N; JEW JEFFREY L; MOFFITT PAUL R
A method for fabricating crystalline dielectric material on top of metal layers to produce an apparatus for non-mechanical steering of an input laser beam is provided. The apparatus may include a plurality of stacked parallel dielectric waveguides, each waveguide of which is fabricated by separating layers of dielectric material from a donor wafer and bonding the separated layers of dielectric material to a receiving wafer. A plurality of voltages is applied across the stacked parallel dielectric waveguides. Each of the stacked parallel dielectric waveguides is electrically phase modulated to deflect an output beam in a predictable manner.
123 ADJUSTABLE OPTICAL ATTENUATOR EP14893120 2014-10-22 EP3139208A4 2017-06-21 MAO CHONGCHANG; LI MINCHUN; MIN HONG
Embodiments of the present invention provide a variable optical attenuator. The variable optical attenuator includes: a collimator, a switchable polarization grating, a reflector, and a voltage controller for adjusting a voltage between electrodes at both ends of a liquid crystal layer of the switchable polarization grating, where the collimator, the switchable polarization grating, and the reflector are disposed successively; the collimator is configured to receive incident light and output the incident light to the switchable polarization grating; the switchable polarization grating is configured to diffract the incident light for one time and then perform emission onto the reflector; the switchable polarization grating is further configured to diffract, for one time, a beam reflected back by the reflector, and then emit resulting diffracted light; and the collimator is further configured to receive the diffracted light and output the diffracted light. The variable optical attenuator provided in the embodiments of the present invention has an extremely wide dynamically variable range, and is characterized by high reliability, a small size, and a low cost.
124 Liquid crystal optical element, manufacturing method thereof, and vehicle light using the same EP06019058.4 2006-09-12 EP1764642B1 2016-11-23 Toko, Yasuo
A liquid crystal optical element (1) is provided which is employed in a vehicle light (15), for example, having a light source (12), a reflector (13), and a lens (14). The liquid crystal optical element (1) is placed between the light source (12) and the lens (14), whereby light distribution control can be achieved over a wide range beyond a basic light distribution constituted by the light source (12), the reflector (13), and the lens (14). A liquid crystal having a photocurable liquid crystalline monomer added thereto is filled into a cell to form a liquid crystal layer (5), which is in turn irradiated with a stripe pattern of ultraviolet rays to partially cure and polymerize the monomer. This provides a cured grating portion (6) and a non-cured, non-grating portion (7) are formed. When a voltage is not applied to the liquid crystal optical element (1), this element (1) is in a transparent state due to the uniformity in the molecular arrangement and the refractive index of the grating portion (6) and the non-grating portion (7) adjacent to each other. When a voltage is applied, the light guided inside the liquid crystal layer (5) is refracted in a predetermined direction by means of the difference in refractive index between the grating portion (6) and the non-grating portion (7) to thereby form scattered light. This can extend projection direction range to the outside.
125 HEAT SHIELDING SYSTEM USING PARTICULATES EP14858047.5 2014-11-03 EP3068206A1 2016-09-14 CHO, Sung Nae

A multi-layered coating system for reflecting infrared waves is disclosed. The multi-layered coating system comprises a layer one positioned above a substrate, wherein the layer one includes a plurality of well separated spherical particulates of radius a1 and a plurality of well separated spherical voids of radius b1 > a1 that are randomly distributed, and a filler material of refractive index n1 intervening in the spaces between said spherical particulates and spherical voids; and subsequent layers expressible as the following word-equation, "a layer i positioned above the layer i-1, wherein the layer i includes a plurality of well separated spherical particulates of radius ai and a plurality of well separated spherical voids of radius bi > ai (where bi > bi-1) that are randomly distributed, and a filler material of refractive index ni intervening in the spaces between said spherical particulates and spherical voids," where integer i is greater than one.

126 MULTI-LAYER COATING SYSTEM USING VOIDS FOR HEAT SHIELDING SYSTEM AND METHOD FOR MANUFACTURING SAME EP14857339.7 2014-11-03 EP3067197A1 2016-09-14 Cho, Sung Nae

Provided are a multilayered-coating system and a method of manufacturing the same. The multi-layered coating system includes: a layer 1 including a plurality of spherical voids with a radius a1 that are randomly distributed and separated from one another and a filler material with a refractive index n1 that is disposed in a space between the spherical voids; and subsequent layers expressed as the following word-equation, "a layer i located above a layer i-1 and including a plurality of spherical voids with a radius a¡ that are randomly distributed and separated from one another, and a filler material with a refractive index ni, the filler material disposed in a space between the spherical voids where i is an integer greater than 1".

127 OPTICAL SHUFFLING EP12880104 2012-06-28 EP2868012A4 2016-04-06 ROSENBERG PAUL KESSLER; FATTAL DAVID A; FIORENTINO MARCO; BEAUSOLEIL RAYMOND G
Techniques relating to optical shuffling are described herein. In an example, a system for shuffling a plurality of optical beams is described. The system includes a plurality of sources to output respective beams of light. The system further includes a plurality of receivers to receive respective beams of light. The system further includes a shuffling assembly including a plurality of sub-wavelength grating (SWG) sections. Each of the plurality of SWG sections is for defining optical paths of the plurality of beams. The plurality of SWG sections includes at least one reflecting SWG section to reflect and direct light from a respective one of the plurality of sources toward a respective one of the plurality of receivers.
128 OPTICAL SHUFFLING EP12880104.0 2012-06-28 EP2868012A1 2015-05-06 ROSENBERG, Paul Kessler; FATTAL, David A.; FIORENTINO, Marco; BEAUSOLEIL, Raymond G.
Techniques relating to optical shuffling are described herein. In an example, a system for shuffling a plurality of optical beams is described. The system includes a plurality of sources to output respective beams of light. The system further includes a plurality of receivers to receive respective beams of light. The system further includes a shuffling assembly including a plurality of sub-wavelength grating (SWG) sections. Each of the plurality of SWG sections is for defining optical paths of the plurality of beams. The plurality of SWG sections includes at least one reflecting SWG section to reflect and direct light from a respective one of the plurality of sources toward a respective one of the plurality of receivers.
129 Display panel comprising metal grid color selective polarizer EP11177489.9 2011-08-12 EP2487530B1 2015-02-25 Chung, Seong-eun; Kim, Dong-hwan; Jung, Il-yong; Kim, Tae-bae
130 Element, device and method for generating electromagnetic radiation in the terahertz domain EP12184055.7 2012-09-12 EP2607945A2 2013-06-26 Nakanishi, Hidetoshi; Tonouchi, Masayoshi

An electromagnetic radiation generating device generates electromagnetic wave pulses (LT1) from a plane surface which receives pulsed light (LP1). The electromagnetic radiation generating device includes an electromagnetic radiation generating element (10), a light irradiating unit, and a reverse bias voltage applying circuit. The electromagnetic radiation generating element (10) includes a depletion layer forming body (90) formed by stacking a p-type silicon layer (14) and an n-type silicon layer (15) in a planar pattern having a pn junction (17), an antireflection film (16) and a light receiving surface electrode formed on the light receiving surface (10A) which is one surface of the depletion layer forming body (90), the light receiving surface electrode including a plurality of parallel electrode parts (121) that are equally spaced while the distance is maintained between the parallel electrode parts (121), the distance corresponding to the wavelength of the electromagnetic wave pulses (LT1) generated from the depletion layer forming body (90) and a rear surface electrode (13) formed on the rear surface (10B) which is the opposite surface of the depletion layer forming body (90). The reverse bias voltage applying circuit applies a voltage to bring a depletion layer formed in the depletion layer forming body into a reverse biased condition through the light receiving surface electrode and the rear surface electrode (13).

131 OPTICAL DEVICE FOR BROADBAND NONLINEAR OPTICAL PROCESSES BASED ON ANGULAR DISPERSION EP11728658.3 2011-04-07 EP2556407A2 2013-02-13 FÜLÖP, József; ALMÁSI, Gábor; HEBLING, János; TRINN, Tamás
The invention relates to an optical device (100) for performing nonlinear optical processes, allowing especially broadband optical parametric amplification or frequency conversion, wherein one or more of several input beams exhibit angular dispersion and the angular dispersive element (105) of said optical device (100) is in direct optical contact with the nonlinear medium (107). The device according to the invention allows the construction of high efficiency, compact amplifiers and frequency converters with ultrahigh broadband that can be scaled for large beam sizes and high powers as well.
132 SURFACE-PLASMON-BASED OPTICAL MODULATOR EP09789134.5 2009-08-13 EP2310901A1 2011-04-20 KOBYAKOV, Andrey; SPARKS, Kevin, B; ZAKHARIAN, Aramais
An optical modulator that utilizes Bloch surface plasmon (BSP) effects is disclosed. The BSP optical (BSPO) modulator (10) includes a permittivity-modulated (P-M) grating (20) that can be one-dimensional or two-dimensional. Electro-optic (EO) substrates (30) sandwich the P-M grating. The EO substrates have electrodes (64) arranged thereon, and a voltage source (60) connected to the electrodes is used to provide an applied voltage (V 30) via a modulation voltage signals (SM) that switches the modulator. Index-matching layers (40) may be used to mitigate adverse reflection effects. The BSPO modulator allows for normally incident input light (1001) to be modulated directly without having to generate oblique angles of incidence for the input light in order to excite the surface plasmon.
133 INTEGRATED PLANAR DEVICE FOR LIGHT GUIDING, CONCENTRATING, AND WAVELENGTH SHIFTING EP09718695 2009-03-11 EP2260342A4 2011-04-13 JI JIN; KAUFMAN LAWRENCE A; SLAFER W DENNIS
134 Liquid crystal optical element, manufacturing method thereof, and vehicle light using the same EP06019058.4 2006-09-12 EP1764642A1 2007-03-21 Toko, Yasuo

A liquid crystal optical element (1) is provided which is employed in a vehicle light (15), for example, having a light source (12), a reflector (13), and a lens (14). The liquid crystal optical element (1) is placed between the light source (12) and the lens (14), whereby light distribution control can be achieved over a wide range beyond a basic light distribution constituted by the light source (12), the reflector (13), and the lens (14). A liquid crystal having a photocurable liquid crystalline monomer added thereto is filled into a cell to form a liquid crystal layer (5), which is in turn irradiated with a stripe pattern of ultraviolet rays to partially cure and polymerize the monomer. This provides a cured grating portion (6) and a non-cured, non-grating portion (7) are formed. When a voltage is not applied to the liquid crystal optical element (1), this element (1) is in a transparent state due to the uniformity in the molecular arrangement and the refractive index of the grating portion (6) and the non-grating portion (7) adjacent to each other. When a voltage is applied, the light guided inside the liquid crystal layer (5) is refracted in a predetermined direction by means of the difference in refractive index between the grating portion (6) and the non-grating portion (7) to thereby form scattered light. This can extend projection direction range to the outside.

135 LIQUID CRYSTAL VARIABLE OPTICAL ATTENUATOR EP04713482 2004-02-21 EP1606669A4 2006-12-06 CAVANAUGH SHANTI A; AUSTIN LINDSAY W; YOUNG MARK E; MOLINARI LOUIS J
A twisted nematic liquid crystal variable optical attenuator[100] is presented with one substrate that includes a integrated subwavelength nanostructured polarizer[111]. The device may incorporate an integrated isolator whereby a substrate of the liquid crystal sandwich is formed from doped garnet to comprise a faraday rotator etched with a subwavelength optical nanostructured polarizing grating and enabling the substrate to function as an isolator. The liquid crystal variable optical attenuator may include a deposited metal gasket moisture barrier[106] bonding the opposing top and bottom substrates each having a spacer layer[107] to accurately control cell gap thickness. The liquid crystal variable optical attenuator[100] may also include an integrated thermal sensor and heater deposition layer[ 108] sandwiched between or deposited on at least one or both opposing substrates.
136 QUADRUPLE GRATING PERIOD PPLN OPTICAL PARAMETRIC OSCILLATOR DIFFERENCE FREQUENCY GENERATOR WITH COMMON DOUBLY RESONANT CAVITY EP99956474.3 1999-07-09 EP1127392B1 2006-03-08 MEYER, Ronald, K., Jr.; VAIDYANATHAN, Mohan; PEKNY, William; GRIFFITH, Gerald, P.; MUI, Peter, H.
The present invention relates generally to the field of optical devices and particularly to embodiments of a four-stage PPLN optical parametric oscillator/difference-frequency generator configuration. The present invention allows simultaneously and colinear generation of four wavelengths in efficient use of the pump signal. A first embodiment comprises a singly resonant cavity (38) having an internal monolithic non-linear optical medium (20) disposed in the cavity. The cavity is bounded by an input mirror (34) and an output mirror (36). The monolithic non-linear optical medium is divided into four regions each having its own grating period. A second embodiment of the present invention comprises a monolithic non-linear optical medium (40) divided into four separate regions (46, 48, 50, 52). The entrance facet (42) and exit facet (44) of the monolithic non-linear optical medium includes a coating (58, 60) which acts as the cavity mirrors.
137 LIQUID CRYSTAL VARIABLE OPTICAL ATTENUATOR EP04713482.0 2004-02-21 EP1606669A2 2005-12-21 CAVANAUGH, Shanti, A.; AUSTIN, Lindsay, W.; YOUNG, Mark, E.; MOLINARI, Louis, J.
A twisted nematic liquid crystal variable optical attenuator[100] is presented with one substrate that includes a integrated subwavelength nanostructured polarizer[111]. The device may incorporate an integrated isolator whereby a substrate of the liquid crystal sandwich is formed from doped garnet to comprise a faraday rotator etched with a subwavelength optical nanostructured polarizing grating and enabling the substrate to function as an isolator. The liquid crystal variable optical attenuator may include a deposited metal gasket moisture barrier[106] bonding the opposing top and bottom substrates each having a spacer layer[107] to accurately control cell gap thickness. The liquid crystal variable optical attenuator[100] may also include an integrated thermal sensor and heater deposition layer[ 108] sandwiched between or deposited on at least one or both opposing substrates.
138 BISTABLE NEMATIC LIQUID CRYSTAL DEVICE EP00977689.9 2000-11-23 EP1234207B1 2005-07-20 JONES, John Clifford
A liquid crystal device comprises a layer (2) of a nematic liquid crystal material contained between two cell walls (3, 4) each carrying electrode structures (6, 7) and an alignment surface (20, 21). The alignment layer (20, 21) on one or both cell wall (4), is formed of a plurality of small (<15 mu m) surface features each separably capable of providing a bistable pretilts and an alignment direction and collectively causing larger variations of molecular orientation across the layer (2). The device may be switched between a light transmissive state and a light non-transmissive state. The small surface features may be areas of grating (21), protrusions (25), or blind holes (26), separated by mono stable flat surfaces (Fm) coated with a homeotropic alignment layer. Preferably, the grating etc provides bistable switching operation between a low surface tilt and high surface tilt, and the low tilt alignment direction varies between adjacent grating areas.
139 LIQUID CRYSTAL DEVICE EP01956649.6 2001-07-18 EP1301823A1 2003-04-16 WOOD, Emma Louise; BRYAN-BROWN, Guy Peter; HUI, Victor; JONES, John Clifford; BROWN, Carl Vernon
Liquid crystal devices are described that exhibit bistable, tri-stable or other multistable operation. The stable liquid crystal configurations are attained using a surface alignment grating (144) on the internal surface of at least one cell wall (142). The surface profile of the surface alignment grating comprises three or more defect sites per grating period and permit the liquid crystal molecules to adopt any one of two or more stable pretilt angles in the same azimuthal plane. Application of a suitable voltage causes the liquid crystal material to switch between the stable configurations.
140 Methods of microstructuring ferroelectric materials EP01305202.2 2001-06-15 EP1266983A1 2002-12-18 Eason, Robert William c/o Un. of Southampton; Brown, Paul c/o University of Southampton; Mailis, Sakellaris c/o University of Southampton

A method of micro-structuring a surface of a sample of ferroelectric material, the method comprising: (a) taking a sample of ferroelectric material having a -z face which is to be etched; (b) illuminating the -z face with ultraviolet light to define illuminated and unilluminated parts of the surface; and (c) immersing the -z face in an etchant to selectively remove the unilluminated parts of the -z face at a greater rate than the illuminated parts. The method can be carried out using pulsed ultraviolet light to etch lithium niobate crystals cut for etching on the -z face, and may further be combined with ablation to produce multi-level surface structures.

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