| 序号 | 专利名 | 申请号 | 申请日 | 公开（公告）号 | 公开（公告）日 | 发明人 |
|---|---|---|---|---|---|---|
| 161 | Optische Schaltungsvorrichtung | EP08103431.6 | 2008-04-08 | EP2108996A1 | 2009-10-14 | Blöhbaum, Frank |
Die Erfindung betrifft eine optische Schaltungsvorrichtung mit einem Substrat (10,12,14) aus einem Halbleitermaterial, auf welchem eine Metallschicht (20,22,24) mit einer oberen und einer unteren Grenzschicht angeordnet ist, deren Höhe (h) derart ausgebildet ist, dass sich bei Auftreffen von elektromagnetischer Strahlung (S) in der Metallschicht (20,22,24) Plasmonen ausbilden können, wobei Mittel zum Ändern der Ladungsträgerkonzentration des Halbleitermaterials vorgesehen sind.
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| 162 | MAGNETO-OPTICAL DEVICE | EP06843760.7 | 2006-12-27 | EP1971897A1 | 2008-09-24 | KATSURAGAWA, Tadao |
| A magneto-optical device is disclosed that includes a non-magnetic support body and a fine particle arrangement layer on the non-magnetic support body. The fine particle arrangement layer includes multiple regularly arranged fine metal magnetic particles. In the magneto-optical device, magnetization is generated by applying an external magnetic field to the fine metal magnetic particles, and linearly polarized light is made incident on the fine metal magnetic particles, so that a magneto-optical effect is increased by the interaction between the incident light on the fine metal magnetic particles and the surface plasmon oscillation of the fine metal magnetic particles. | ||||||
| 163 | OPTICAL RADIATION MODULATION METHOD, AN ELECTROOPTICAL MODULATOR (VARIANTS) AND AN ELECTROOPTICAL DEVICE (VARIANTS) | EP05784422.7 | 2005-03-03 | EP1860485A1 | 2007-11-28 | Guscho, Yury Petrovich |
The invention is related to modulation of light by the controlling of intensity and phase characteristics of a light radiation with the help of using of relief-phase deformations and surface plasmon resonance effect. It is achieved by a combination of advantages of the relief-phase record and the surface plasmon resonance effect. The technical result, reachable at realization of the offered invention, consists in increase of a efficiency of control of the optical radiation, due to an opportunity of the full deviation (switching) of radiation from the main optical axis at the switching on an input electric signal. The «valvate effect» which is achieved here allows to increase sensitivity, contrast and the resolution of the processable optical information. For the first time the opportunity of dynamic control of the surface plasmon resonance effect both in prismatic and in grating is received. The offered method and the modulator can be used, in particular, in nanotechnology as the high-sensitivity sensor reacting to change of properties of the dielectric medium in real time. The invention can be applied also in the optical-mechanical industry, high-sensitive and high-resolution sensors control of gas, liquid and firm dielectric mediums (in biology, chemistry, etc.), projection and display TV, printing and communication facility, light fiber switching and light filtering devices, high-speed linear and matrix printers, as tunable diffractional grating and in other areas of technics. |
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| 164 | Image display apparatus | EP06126562.5 | 2006-12-19 | EP1808728A1 | 2007-07-18 | Lee, Hong-seok; Lee, Su-mi |
An image display apparatus (1000) is provided to improve display characteristics, the apparatus including a prism (300) and a pixel section (400) on one side of the prism (300). The pixel section (400) includes a reflective electrode (410) and dielectrics (420) disposed at a predetermined distance from the reflective electrode (410). The dielectrics (420) are in contact with the reflective electrode (410) if voltage is applied, and the effective refractive index changes according to the image signal. The effective refractive index of the section of the reflective electrode (410) in contact with the dielectrics (420) changes, and accordingly, the reflectivity of the reflective electrode (410) changes corresponding to the image signal. The pixel section (400) is able to regulate the surface plasmon resonance by regulating the reflective electrode (410), and is able to display the black state using the surface plasmon resonance. The image display apparatus (1000) provides improved contrast ratio by preventing color leaks from arising in the black state, and thus, improve display characteristics.
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| 165 | OPTICAL DEVICE | EP04788146.1 | 2004-09-17 | EP1672409A1 | 2006-06-21 | ISHIHARA, Kunihiko, c/o NEC Corporation; HATAKOSHI, Genichi, c/o Toshiba Corporation; OHASHI, Keishi, c/o NEC Corporation; ICHIHARA, Katsutaro, c/o Toshiba Corporation |
A conductive thin film has first and second surfaces and at least one opening extending through from the first surface to the second surface. At least on one of the first and second surfaces, first and second periodic surface patterns having different period lengths are provided. The period length of the second periodic surface pattern is substantially equal to an odd integral multiple of a half of the period length of the first periodic surface pattern. With this, surface plasmon polaritons excited by the first periodic surface pattern undergo odd-order Bragg reflection by the second periodic surface pattern. As a result, the intensity of the light falling on the first surface and transmitted to the second surface through the opening is increased with high efficiency. |
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| 166 | Light modulator controlled by surface plasmon waves | EP04016812.2 | 2000-05-12 | EP1473586B1 | 2005-09-14 | Takatori, Ken-ichi |
| 167 | LONG RANGE SURFACE PLASMON POLARITON MODULATOR | EP03793609.3 | 2003-09-05 | EP1546774A2 | 2005-06-29 | BOZHEVOLNYI, Sergey; NIKOLAJSEN, Thomas; KRYGER, Bonni; LE SSON, Kristján; SALAKHUTDINOV, Ildar; S NDERGAARD, Thomas; SKOVGAARD, Peter, M., W. |
| The present invention relates to waveguides for guiding and modulating long range surface plasmon polaritons (LR-SPPs). The guiding devices comprise a core stripe of e.g. metal of finite width embedded in a cladding such as a dielectric cladding. Particularly, in the waveguides of the invention, the complex propagation constant of the guided LR-SPP mode(s) can be dynamically adjusted by heating of the metal core leading to dissipation of heat into the surrounding dielectric material. The devices may be used in the construction of dynamic light guiding integrated components for optical telecommunication. | ||||||
| 168 | Light modulator controlled by surface plasmon waves | EP04016812.2 | 2000-05-12 | EP1473586A1 | 2004-11-03 | Takatori, Ken-ichi |
A light modulator has two unit devices (1,2) each using surface plasmon waves generated at the interface between thin metal films (13,14) formed respectively on prisms (11,12) and a mirror (3), in which the thin metal films are oppositely disposed with an air gap in between which can be varied by means of a piezo material. Both the transmitted light due to absorption and re-radiation, and the reflected light arising from the unit devices (1,2) appear in the outgoing light, the incident light on the next unit device, or the incident light on the mirror (3). Consequently, all light beams can be utilized as the final outgoing light beams with no loss of light. Further, the colour of light can be spatially divided, and still further, it can also be temporally divided by changing the wavelength by means of a voltage. As a result, the original light can be divided both temporally and spatially with almost no loss by combining two unit devices so configured as to re-radiate the absorbed light by the surface plasmon waves using surface plasmon and a mirror, and thus utilize both the reflected light and the transmitted light. |
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| 169 | OPTICAL WAVEGUIDE STRUCTURES | EP02734965.3 | 2002-06-21 | EP1402293A1 | 2004-03-31 | BERINI, Pierre Simon Joseph |
| An optical device comprises a waveguide structure formed by a strip (100) of a material having a relatively high free charge carrier density surrounded by a material having a relatively low free charge carrier density. The strip has finite width (W) and thickness (t) of the same order with dimensions such that optical radiation having a wavelength in a predetermined range couples to the strip and propagates along the length of the strip as a plasmon-polariton wave. Preferably the width and thickness are substantially equal and less than about 300 nm. | ||||||
| 170 | Light modulator controlled by surface plasmon waves | EP00304024.3 | 2000-05-12 | EP1054290A2 | 2000-11-22 | Takatori, Ken-ichi |
A light modulator has two unit devices (1,2) each using surface plasmon waves generated at the interface between thin metal films (13,14) formed respectively on prisms (11,12) and an electro-optical material (15), and a mirror (3). Both the transmitted light due to absorption and re-radiation, and the reflected light arising from the unit devices (1,2) appear in the outgoing light, the incident light on the next unit device, or the incident light on the mirror (3). Consequently, all light beams can be utilized as the final outgoing light beams with no loss of light. Further, the colour of light can be spatially divided, and still further, it can also be temporally divided by changing the wavelength by means of a voltage. As a result, the original light can be divided both temporally and spatially with almost no loss by combining two unit devices so configured as to re-radiate the absorbed light by the surface plasmon waves using surface plasmon and a mirror, and thus utilize both the reflected light and the transmitted light. |
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| 171 | Optischer Leistungsbegrenzer mit intensitätsabhängigem Reflexionsvermögen | EP92112617.3 | 1992-07-23 | EP0534083B1 | 1996-11-20 | Lautenschlager, Peter, Dr.; Scherber, Werner, Dr. |
| 172 | Optischer Leistungsbegrenzer mit intensitätsabhängigem Reflexionsvermögen | EP92112617.3 | 1992-07-23 | EP0534083A2 | 1993-03-31 | Lautenschlager, Peter, Dr.; Scherber, Werner, Dr. |
Optischer Leistungsbegrenzer, dessen Durchlässigkeit innerhalb eines interessierenden Wellenlängenbereichs abhängig ist von der Intensität der einfallenden Strahlung, wobei die Verstimmung der Resonanz von Oberflächenplasmonen ausgenutzt wird. Sie eignet sich insbesondere zum Schutz von IR-Detektoren gegen den Einfall hoher Strahlungsintensitäten. |
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| 173 | Optical modulator | EP89114252.3 | 1989-08-02 | EP0365766A3 | 1991-08-14 | Collins, Reuben T.; Kirtley, John R.; Theis, Thomas N. |
A method of modulating light (28) incident to a semiconductor body (10) comprising the steps of: coupling the incident light (28) to the surface plasmon polariton mode (44) at an interface (21) of the semiconductor body (10); and selectively altering the absorption of the incident light (28) by the semiconductor body (10) so as to decouple the incident light (28) from the surface plasmon polariton mode (44). The absorption can be selectively altered by establishing a quantum confined optical absorption region (14) within the semiconductor body (10), and effecting a Stark shift of the quantum confined optical absorption region (14). |
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| 174 | OPTISCHE DIODE | EP15763815.6 | 2015-08-18 | EP3183607B1 | 2018-11-28 | VOLZ, Jürgen; SCHNEEWEISS, Philipp; SAYRIN, Clément; RAUSCHENBEUTEL, Arno |
| 175 | SPATIAL POSITIONING OF PHOTON EMITTERS IN A PLASMONIC ILLUMINATION DEVICE | EP15724268.6 | 2015-05-21 | EP3149783B8 | 2018-09-05 | VERSCHUUREN, Marcus Antonius; LOZANO BARBERO, Gabriel Sebastian; GOMEZ RIVAS, Jaime |
| There is provided an illumination device (100) comprising: a substrate (104); an optically transmissive first layer (106) arranged on the substrate; a photon emitting layer (108), arranged on the optically transmissive first layer and comprising a photon emitting material configured to receive energy from an energy source and to emit light having a predetermined wavelength; a periodic plasmonic antenna array, arranged on the substrate and embedded within the first layer, and comprising a plurality of individual antenna elements (114) arranged in an antenna array plane, the plasmonic antenna array being configured to support a first lattice resonance at the predetermined wavelength, arising from coupling of localized surface plasmon resonances in the individual antenna elements to photonic modes supported by the system comprising the plasmonic antenna array and the photon emitting layer, wherein the plasmonic antenna array is configured to comprise plasmon resonance modes such that light emitted from the plasmonic antenna array has an anisotropic angle distribution; and wherein the photon emitting layer is arranged at a distance from the antenna array plane corresponding to a location of maximum field enhancement for light out-coupling resulting from the plasmonic-photonic lattice resonances. | ||||||
| 176 | Liquid crystal display device and method of fabricating the same | EP10177574.0 | 2010-09-20 | EP2317372B1 | 2018-09-05 | Park, Se-Young; Kim, Jeong-Hyun; Yi, Sung-Chol; LEE, Chang-Gu |
| A liquid crystal display device includes a first substrate; a thin film transistor including a gate electrode, semiconductor layer, source electrode, and a drain electrode formed on the first substrate; a pixel electrode connected to the drain electrode formed on the first substrate; a color filter having a transmissive pattern with a plurality of periodic holes; a second substrate bonded to the first substrate; and a sealant formed between the first substrate and the second substrate. | ||||||
| 177 | ELECTROCHROMIC DEVICE CONTAINING COLOR-TUNABLE NANOSTRUCTURES | EP16839817.0 | 2016-08-15 | EP3341788A1 | 2018-07-04 | GARCIA, Guillermo; HOLT, Jason; THOMSEN, Scott; KOO, Bonil |
| An electrochromic device and method, the device including: a first transparent conductor layer; a working electrode disposed on the first transparent conductor layer and including nanostructures; a counter electrode; a solid state electrolyte layer disposed between the counter electrode and the working electrode; and a second transparent conductor layer disposed on the counter electrode. The nanostructures may include transition metal oxide nanoparticles and/or nanocrystals configured to tune the color of the device by selectively modulating the transmittance of near-infrared (NIR) and visibleradiation as a function of an applied voltage to the device. | ||||||
| 178 | DEVICES, IN PARTICULAR OPTICAL OR ELECTRO-OPTICAL DEVICES WITH QUANTIZED OPERATION | EP16727465.3 | 2016-06-02 | EP3304193A1 | 2018-04-11 | EMBORAS, Alexandros; LEUTHOLD, Jürg; SCHIMMEL, Thomas |
| The device (1) comprises a resonator (R) capable of supporting a plasmon mode, wherein the resonator (R) comprises a tip (T) made of a first material and a vacuum or a matrix element (15a, 15b, 15c) interfacing the tip (T). The device (1) comprises a material cluster derived from the first material, wherein the material cluster is present at the tip (T) inside the vacuum or matrix element (15a, 15b, 15c). The device (1) is structured and arranged to receive in the resonator a setting signal for changing a resonance condition of the plasmon mode by relocating the material cluster inside the vacuum or matrix element. This way, atomic scale switches and memory elements can be realized. | ||||||
| 179 | PHASE MODULATION ACTIVE DEVICE, METHOD OF DRIVING THE SAME, AND OPTICAL APPARATUS INCLUDING THE PHASE MODULATION ACTIVE DEVICE | EP17184396.4 | 2017-08-02 | EP3293570A1 | 2018-03-14 | LEE, Duhyun; SHIN, Changgyun; KYOUNG, Jisoo; CHOI, Byounglyong |
A phase modulation active device and a method of driving the phase modulation active device are provided. The phase modulation active device includes channels independently modulating a phase of incident light. The method includes selecting a first phase value and a second phase value to be used for the channels, setting a binary phase profile by allocating the selected first phase value or the selected second phase value to each of the channels quasi-periodically, in a sequence in which the channels are arranged, and driving the phase modulation active device, based on the set binary phase profile.
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| 180 | OPTISCHE DIODE | EP15763815.6 | 2015-08-18 | EP3183607A1 | 2017-06-28 | VOLZ, Jürgen; SCHNEEWEISS, Philipp; SAYRIN, Clément; RAUSCHENBEUTEL, Arno |
| An optical diode (1) comprising an optical wave guide for guiding light, preferably of a light mode, with a vacuum wavelength λ 0, wherein the optical wave guide has a wave guide core (2, 3, 14) with a first index of refraction (n 1), and the wave guide core (2, 3, 14) is surrounded by at least one second optical medium which has at least one second index of refraction (n2), wherein n 1 > n 2 applies, wherein the wave guide core (2, 3, 14) has at least in sections a smallest lateral dimension (7) which is a smallest dimension of a cross section (6) perpendicular to a propagation direction (5) of the light in the wave guide core (2, 3, 14), wherein the smallest lateral dimension (7) is greater than or equal to λ 0/(5*n 1) and less than or equal to 20*λ 0/n 1, wherein the optical diode (1) additionally comprises at least one absorber element (10, 11, 15, 16) which is arranged in a near field, wherein the near field consists of the electromagnetic field of the light of the vacuum wavelength λ 0 in the wave guide core (2, 3, 14) and outside of the wave guide core (2, 3, 14) up to a standard interval (12) of 5*λ 0, wherein the standard interval (12) is measured starting from one surface (8) of the wave guide core (2, 3, 14) forming an optical interface and in a direction perpendicular to the surface (8). The invention provides that the at least one absorber element (10, 11, 15, 16) for the light of the vacuum wavelength λ 0 has a strongly different absorption for left circular polarization (σ -) and for right circular polarization (σ +). | ||||||
