序号 专利名 申请号 申请日 公开(公告)号 公开(公告)日 发明人
61 INTER-MODE LIGHT SWITCH EP13833826 2013-08-27 EP2889672A4 2016-05-18 HAMAMOTO KIICHI
Provided is an optical mode switch that can effect a more compact optical switch. The optical mode switch (100) is provided with: a single input port (1); a single output port (2); two waveguides (10) provided in parallel between the input port (1) and the output port (2); and a refractive index altering means (8) that alters the refractive index of the waveguides. Any given mode light input to the input port (1) is output as any given mode light from the output port (2) in accordance with the refractive index altered by the refractive index altering means (8).
62 OPTICAL MODE CONVERSION BY NONLINEAR EFFECTS EP12862528 2012-12-06 EP2788817A4 2015-08-05 GRUNER-NIELSEN LARS; JAKOBEN DAN P; XU CHUNHUI; CHENG JI
Embodiments of the present invention generally relate to optical mode conversion by nonlinear effects. More specifically, embodiments of the present invention relate to nonlinear mode conversion utilizing intermodal four-wave mixing to convert light between modes having different wavelengths for complex applications. In one embodiment of the present invention, a fiber comprises an input end for receiving light in a first mode at a first wavelength, and an output end for outputting light in a desired second mode at a desired second wavelength, wherein the first wavelength and the second wavelength are not the same. In many embodiments, the fiber comprises a higher-order mode fiber.
63 INTER-MODE LIGHT SWITCH EP13833826.4 2013-08-27 EP2889672A1 2015-07-01 HAMAMOTO, Kiichi

Provided is an optical mode switch that can effect a more compact optical switch. The optical mode switch (100) is provided with: a single input port (1); a single output port (2); two waveguides (10) provided in parallel between the input port (1) and the output port (2); and a refractive index altering means (8) that alters the refractive index of the waveguides. Any given mode light input to the input port (1) is output as any given mode light from the output port (2) in accordance with the refractive index altered by the refractive index altering means (8).

64 LASER A FIBRE DE PUISSANCE A CONVERSION DE MODE EP01984196.4 2001-07-06 EP1299930B1 2012-05-09 HUIGNARD, Jean-Pierre Thales Intellectual Property; BRIGNON, Arnaud Thales Intellectual Property
The invention concerns a pumped fibre laser comprising essentially a doped fibre (1), Said laser is mainly characterised in that the doped fibre is multimode (1) and it also comprises a spatial mode converting device (3) receiving the beam. Said multimode fibre has a core with diameter greater than 30 micrometers, even greater than 50 micrometers.
65 SHORT PULSE MID-INFRARED PARAMETRIC GENERATOR FOR SURGERY EP98903709.8 1998-01-28 EP1006967B1 2005-10-26 TELFAIR, William, B.; ZENZIE, Henry; MOULTON, Peter; HOFFMAN, Hannah, J.
A laser parametric generator for surgical applications is disclosed which utilizes short-pulse, mid-infrared radiation. The mid-infrared radiation may be produced by a pump laser source (20), such as a neodymium-doped laser, which is parametrically downconverted in a suitable nonlinear crystal (15) to the desired mid-infrared range. The short pulses reduce unwanted thermal effects and changes in adjacent to potentially submicron levels. The parametrically converted radiation source preferably produces pulse durations shorter than 25 ns at or near 3.0 νm but preferably close to the water absorption maximum associated with the tissue. The down-conversion to the desired mid-infrared wavelength is preferably produced by a nonlinear crystal (15) such as KTP or its isomorphs. In one embodiment, a non-critically phased-matched crystal is utilized to shift the wavelength from a near-infrared laser source emitting at or around 880 to 900 nm to the desired 2.9 to 3.0 νm wavelength range. A fiber, fiber bundle or another waveguide means utilized to separate the pump laser from the optical parametric oscillation (OPO) cavity is also included as part of the invention.
66 Externally controllable waveguide type higher order optical mode converter EP01308393.6 2001-10-02 EP1193515A2 2002-04-03 Kim, Kwang-Bae

A higher order mode generator is for converting the 0th order fundamental guiding mode into higher modes higher than the 0th order in a waveguide. The waveguide is made from thermo-optic materials in which the refractive index is changed according to the applied electrical power. The waveguide has at least two guiding modes and a straight heater or a linear electrode to invoke refractive index perturbation due to temperature or electric field, and is laid across the waveguide at a certain tilt angle α with respect to the waveguide. When there is no external electric power applied to the heater/electrode, the 0th order single mode light of the waveguide will be propagated through the waveguide without any conversion into higher order modes. When electric power is applied, the refractive index of the waveguide beneath the heater changes and higher order modes can be excited by external control.

67 POLARIZER AND POLARIZATION MODULATION SYSTEM EP13899938.8 2013-12-20 EP3073302B1 2018-09-26 TU, Xin; FU, Hongyan; LIU, Wanyuan
The present invention provides a polarizer and a polarization modulation system. The polarizer includes at least one MMI multi-mode waveguide, where one side of each MMI multi-mode waveguide is connected to an input waveguide, and the other side is connected to an output waveguide; an end portion of the side, on which the output waveguide is located, of the MMI multi-mode waveguide is provided with an adjustable portion, and the adjustable portion is connected to the output waveguide; and the polarizer further includes a controller connected to the adjustable portion, where the controller is configured to perform control to change a material property of the adjustable portion, so that the output waveguide outputs optical signals in different polarization states. The present invention implements adjustable polarization, and the structure is simple.
68 POLARIZER AND POLARIZATION MODULATION SYSTEM EP13899938.8 2013-12-20 EP3073302A1 2016-09-28 TU, Xin; FU, Hongyan; LIU, Wanyuan

The present invention provides a polarizer and a polarization modulation system. The polarizer includes at least one MMI multi-mode waveguide, where one side of each MMI multi-mode waveguide is connected to an input waveguide, and the other side is connected to an output waveguide; an end portion of the side, on which the output waveguide is located, of the MMI multi-mode waveguide is provided with an adjustable portion, and the adjustable portion is connected to the output waveguide; and the polarizer further includes a controller connected to the adjustable portion, where the controller is configured to perform control to change a material property of the adjustable portion, so that the output waveguide outputs optical signals in different polarization states. The present invention implements adjustable polarization, and the structure is simple.

69 A supercontinuum source EP14155841.1 2014-02-19 EP2770370A3 2016-08-31 Clowes, John Redvers; Devine, Adam; Grudinin, Anatoly Borisovich

A supercontinuum optical pulse source provides a combined supercontinuum. The supercontinuum optical pulse source comprises one or more seed pulse sources (13), and first and second optical amplifiers (7) arranged along first and second respective optical paths. The first and second optical amplifiers are configured to amplify one or more optical signals generated by said one or more seed pulse sources. The supercontinuum optical pulse source further comprises a first microstructured light-guiding member (9) arranged along the first optical path and configured to generate supercontinuum light responsive to an optical signal propagating along said first optical path, and a second microstructured light-guiding member (9) arranged along the second optical path and configured to generate supercontinuum light responsive to an optical signal propagating along said second optical path. The supercontinuum optical pulse source further comprises a supercontinuum-combining member (5) to combine supercontinuum generated in at least the first and second microstructured light-guiding members to form a combined supercontinuum. The supercontinuum-combining member comprises an output fibre, wherein the output fibre comprises a silica-based multimode optical fibre supporting a plurality of spatial modes at one or more wavelengths of the combined supercontinuum.

70 ALL-OPTICAL FLIP-FLOP EP02798659 2002-09-10 EP1437622A4 2005-06-29 NAKANO YOSHIAKI; TAKENAKA MITSURU
A set-reset flip-flop of all-optical operation. A set light is inputted through a set port. Then, a multimode interference portion in a waveguide oscillates only in a set mode. As a result, a noninverted output Q is produced from a noninverted output port. Even if the input of the set light is turned off, the output state is maintained. When a reset light is inputted through a reset port, the multimode interference portion stops its oscillation in the set mode and causes oscillation in a reset mode. Thus, an inverted output Q-bar is generated from an inverted output port. Even if the reset light input is turned off, the output state is maintained.
71 Externally controllable waveguide type higher order optical mode converter EP01308393.6 2001-10-02 EP1193515A3 2003-06-04 Kim, Kwang-Bae

A higher order mode generator is for converting the 0th order fundamental guiding mode into higher modes higher than the 0th order in a waveguide. The waveguide is made from thermo-optic materials in which the refractive index is changed according to the applied electrical power. The waveguide has at least two guiding modes and a straight heater or a linear electrode to invoke refractive index perturbation due to temperature or electric field, and is laid across the waveguide at a certain tilt angle α with respect to the waveguide. When there is no external electric power applied to the heater/electrode, the 0th order single mode light of the waveguide will be propagated through the waveguide without any conversion into higher order modes. When electric power is applied, the refractive index of the waveguide beneath the heater changes and higher order modes can be excited by external control.

72 光子及び偏光変調システム JP2016541480 2013-12-20 JP6226496B2 2017-11-08 トゥ、シン; フ、ホンヤン; リウ、ワンユアン
73 光変調器及び光送信器 JP2014526672 2012-07-26 JP6131954B2 2017-05-24 杉山 昌樹
74 光変調器及び光送信器 JP2014526672 2012-07-26 JPWO2014016940A1 2016-07-07 杉山 昌樹; 昌樹 杉山
光変調器は、入された光を分岐する分岐部、前記分岐部により分岐された光がそれぞれ伝搬する一対のアーム、及び、前記一対のアームから出力された光を合波する合波部を含む光導波路が形成された基板と、前記基板上において前記光導波路の一部と重なり、印加された電圧に基づいて前記光導波路に電界を発生させる1以上の電極とを有し、前記光導波路は、他部分より狭い幅を有する狭幅部が、前記1以上の電極と重ならないように設けられている。
75 非線形効果による光モード変換 JP2014546081 2012-12-06 JP2015505064A 2015-02-16 グルナー−ニールセン,ラース; ヤコブセン,ダン,ピー.; ペデルセン,マーティン,イー.ヴイ.; シュ,チュンフイ; チェン,ジ
本発明の実施形態は、一般に非線形効果による光モード変換に関わる。より具体的には、本発明の実施形態は、複雑な応用に対して、光を異なる波長を有するモード間で変換するためにモード間四波混合を利用する、非線形モード変換に関わる。本発明の一つの実施形態において、ファイバは、第1のモードで、第1の波長において光を受けるための入端と、所望の第2のモードで、所望の第2の波長において光を出力するための出力端を備え、前記第1の波長と前記第2の波長は同じでない。多くの実施形態において、ファイバは高次モードファイバを含む。
76 半導体光変調器、半導体光集積素子、およびこれらの製造方法 JP2011502669 2010-03-05 JP5626203B2 2014-11-19 信也 須藤; 加藤 友章; 友章 加藤; 佐藤 健二; 健二 佐藤; 卓夫 森本
77 Surgical parametric oscillator using infrared rays in a short pulse JP54048198 1998-01-28 JP4278715B2 2009-06-17 ゼンジー,ヘンリー; テルフェア,ウィリアム・ビー; ホフマン,ハナ・ジェイ; ムールトン,ピーター
78 Laser device JP2006194600 2006-07-14 JP2007173769A 2007-07-05 MAEKAWA KEISUKE
<P>PROBLEM TO BE SOLVED: To provide a laser device capable of emitting a higher harmonic wave of multi-longitudinal mode laser light, and realizing higher efficiency and higher performance in a simple and economical fashion through the combination of basic members. <P>SOLUTION: The laser device has a semiconductor laser, as a light source, that emits a fundamental wave in a multi-longitudinal mode, and a polarization inversion element, as a wavelength converting element, comprising two or more periodic polarization inversion regions each of which has a period Δ that corresponds to the longitudinal mode constituting the fundamental wave, wherein the higher harmonic wave obtained by the polarization inversion element is in a multi-longitudinal mode. <P>COPYRIGHT: (C)2007,JPO&INPIT
79 All-optical flip-flop JP2001278213 2001-09-13 JP3578737B2 2004-10-20 義昭 中野; 充 竹中
80 All-optical flip-flop JP2001278213 2001-09-13 JP2003084327A 2003-03-19 NAKANO YOSHIAKI; TAKENAKA MITSURU
PROBLEM TO BE SOLVED: To provide a set-reset flip-flop which operates all-optically. SOLUTION: Set light is inputted from a setting port 321. Then a multimode interference part 31 of a waveguide 30 oscillates only in set mode. Consequently, an uninverted output Q can be obtained from an uninverted output port 331. This state lasts even after the set light input is ceased. Then reset light is inputted from a resetting port 322. Then the multimode interference part 31 stops oscillating in the set mode and oscillates in reset mode. Consequently, an inverted output Q can be obtained from an inverted output port 332. This state lasts even after the reset light input is ceased. COPYRIGHT: (C)2003,JPO
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