序号 专利名 申请号 申请日 公开(公告)号 公开(公告)日 发明人
41 COMPACT, HIGH BRIGHTNESS LIGHT SOURCES FOR THE MID AND FAR IR EP11851371.2 2011-12-14 EP2656455A1 2013-10-30 FERMANN, Martin E.; JIANG, Jie; PHILLIPS, Christopher; FEJER, Martin M.
Compact laser systems are disclosed which include ultrafast laser sources in combination with nonlinear crystals or waveguides. In some implementations fiber based mid-IR sources producing very short pulses and/or mid-IR sources based on a mode locked fiber lasers are utilized. Some embodiments may include an infrared source with an amplifier system comprising, in combination, a Tm fiber amplifier and an Er fiber amplifier. A difference frequency generator receives outputs from the Er and/or Tm amplifier system, and generates an output comprising a difference frequency. Exemplary applications of the compact, high brightness mid-IR light sources include medical applications, spectroscopy, ranging, sensing and metrology.
42 ANORDNUNG ZUM ERZEUGEN EINES SIGNALS MIT EINSTELLBARER ZEIT- ODER PHASENLAGE EP11704940.3 2011-02-11 EP2488917A1 2012-08-22 SARTORIUS, Bernd; ROEHLE, Helmut; STANZE, Dennis
The invention relates to a system for producing a signal having a variably adjustable time position or phase position, comprising at least one light source for producing a first light component (2) having a first wavelength and a second light component (2') having a second wavelength deviating from the first wavelength and a phase modulator (5) for varying a phase of the first light component (2), wherein the system is designed to produce a beat note signal by superposing the two light components (2, 2') and has a common optical fiber (4) for coupling in both light components (2, 2'), wherein furthermore the phase modulator (5) is arranged at an end or in the course of said optical fiber (4) and is transparent to both light components (2, 2') and is designed to vary the phase of the first light component (2) selectively independently of a phase of the second light component (2') or more intensely than the phase of the second light component (2'). The invention further relates to a use of such a system.
43 WAVELENGTH CONVERTER EP08721984.6 2008-03-13 EP2120090A1 2009-11-18 OKUNO, Toshiaki

Provided is a wavelength converter having a simple and low-cost structure. The wavelength converter generates converted light having a wavelength different from that of input light. The wavelength converter includes (1) a pump light source that outputs pump light, (2) an optical multiplexer that combines and outputs input light and the pump light, (3) a first optical fiber that receives and guides the input light and the pump light that have been combined and output by the optical multiplexer and generates converted light using a nonlinear optical phenomenon that occurs while the first optical fiber guides the input light and the pump light, the first optical fiber being coiled, and (4) zero-dispersion wavelength adjusting means that adjusts a zero-dispersion wavelength of the first optical fiber.

44 LIGHT SOURCE DEVICE EP06730243 2006-03-28 EP1855155A4 2008-04-02 OKUNO TOSHIAKI
There is provided a light source device having a structure for stably providing a wide-band pulse light having a wavelength spectrum of excellent flatness over a wide band. The light source device uses, as a seed light source, a short-pulse light source having such excellent output pulse characteristic that a frequency band width from the peak to lowered value by 10 dB or 20 dB is 5 THz or above. Furthermore, the light source device includes a wide-band light generation fiber appropriate for combination with such a short-pulse light source. The wide-band light generation fiber inputs a pulse light from a pulse light source and generates a wide-band pulse light by using non-linear optical phenomenon. With this configuration, it is possible to obtain a wide-band pulse light having a wavelength spectrum in which the region having power fluctuation suppressed to 6 dB or below exists over 100 nm or above.
45 A BROAD SPECTRUM LIGHT SOURCE EP04804987.8 2004-12-22 EP1697793A1 2006-09-06 WADSWORTH, William
The invention relates to the field of light sources and in particular to sources of light of wavelengths extending across a broad spectrum of hundreds of nanometres. An object of the invention is to provide a relatively compact and inexpensive source of light of wavelengths spread over a broad spectrum. The light source comprises a laser (4) , which operates at or near its fundamental wavelength and produces pulses of a duration longer than 0.5 ns, and a micro-structured optical fibre (9) arranged to guide the pulses, wherein the light is generated by the pulses in the fibre (9) . The invention further relates to a method of generating a light of a spectrum. The invention may e.g. be useful in applications such as spectral testing of fibre components and spectral analysis of chemical and biological samples.
46 Method and device for generating a spectrally broadened optical signal EP03014509.8 2003-07-03 EP1378789A3 2005-04-06 Watanabe, Shigeki, Fujitsu Limited

The present invention is a method of processing an optical signal, including the steps of (a) inputting signal light into a first nonlinear optical medium to broaden the spectrum of the signal light through self phase modulation occurring in the first nonlinear optical medium, thereby obtaining first spectrally broadened light (supercontinuum light), (b) compensating for chromatic dispersion effected on the first spectrally broadened light obtained in the step (a), and (c) inputting the first spectrally broadened light processed by the step (b) into a second nonlinear optical medium to broaden the spectrum of the first spectrally broadened light through self phase modulation occurring in the second nonlinear optical medium, thereby obtaining second spectrally broadened light.

47 Optical fiber parametric amplifier with adjustable pump source EP03291570.4 2003-06-25 EP1491942A1 2004-12-29 Legrand, Anne; Bayart, Dominique

The invention is related to a parametric amplifier comprising an amplifying fiber (3) connected to a pump laser (8) with a feedback control device (6) for adapting the pump laser power and wavelength. This amplifier is used in a transmission system. In addition the invention comprises a method for controlling the pump laser source in an iterative process to optimize the gain of the amplifier.

48 Optical fiber and optical transmission method EP02255357.2 2002-07-31 EP1281989A3 2004-12-29 Shinichi, Arai, c/o The Furukawa Electroc Co., Ltd; Naoto, Oyama,c/o The Furukawa Electric Co., Ltd; Hirofumi, Saito, The Furukawa Electric Co., Ltd

An optical fiber comprising a core (1) and a cladding region (5) which covers an outer periphery of the core (1), having a zero-dispersion wavelength in a wavelength range of 1.4 µm to 1.65 µm, and being in a single mode in that zero-dispersion wavelength, wherein GeO2 is doped in the core (1) in a quantity such that a relative refractive index difference of the core (1) becomes not less than 1.8%, the cladding region (5) includes first, second, and third cladding regions (2, 3, 4), and a refractive index of the second cladding region (3) is smaller than those of the first cladding region (2) and the third cladding region (4).

49 APPARATUS FOR PROVIDING TIMING JITTER TOLERANT OPTICAL MODULATION OF A FIRST SIGNAL BY A SECOND SIGNAL EP02720094.8 2002-03-15 EP1368701B1 2004-08-11 RICHARDSON, David John; LEE, Ju Han; IBSEN, Morten; PETROPOULOS, Periklis; THE, Peh Choing
50 SYSTEM AND METHOD EMPLOYING LED LIGHT SOURCES FOR A PROJECTION DISPLAY EP01905389.1 2001-02-01 EP1258148B1 2004-04-07 PARKER, Fred; PETERSON, Mark
In a single path multimedia projector (30), the light emitted from blue, green, and red generally monochromatic LEDs (72) is propagated through optical fibers (76) and then integrated through an optical integrator (40). A display controller (56) receives image data from a personal computer (58) and converts the data to color frame sequential data delivered to a common display device (44). The controller (56) synchronizes the data with ON/OFF signals conveyed to an LED power supply (34). The electronically synchronized frame sequential information is cycled faster and more accurately than achievable with a color wheel system (10). In a multiple path projector (120), the light from LEDs (72) can be ON continuously, propagated along separate optical paths (36), and integrated through an integrator (40). The color frame sequential data is delivered to controller-synchronized, separate display devices (44). The output is coupled into a combiner (122) to form a composite image.
51 WAVELENGTH CONVERTER EP00963066.6 2000-10-03 EP1306718A1 2003-05-02 YAMASHITA, Shinji; TORII, Kenichi

A wavelength converter which employs an optical fiber and has high converter efficiency. The polarization planes of a signal light and an exciting light outputted from a laser diode (LD) (103) are respectively controlled by polarization controllers (PC's) (101 and 104) and the phases of the lights are respectively modulated by phase modulators (PM's) (102 and 105) in accordance with modulation signals outputted from an oscillator (110). Then, the output lights from the PM's (102 and 105) are multiplexed by a coupler (106). After the multiplexed signal light and exciting light are amplified by an optical amplifier (EDFA) (107), they are inputted to a dispersion shift fiber (DSP) (108). After wavelength transformation (four light waves mixing (FWM)) is practiced in the DSP, an FWM light is outputted through a band-pass filter (BPF) (109).

52 POLED WAVEGUIDE STRUCTURE WITH STABILISED INTERNAL ELECTRIC FIELD EP00972435.2 2000-10-25 EP1228394A1 2002-08-07 Wong, Danny; Xu, Wei; Blazkiewicz, Paul; Ryan, Thomas
An optical waveguide (11) includes a region (22) which, after electrical poling of a guiding region (16), maintains an internal electric field induced by the poling potential. The internal electric field may arise from charge separation between regions (18, 20) induced by an adjacent poling electrode (12A), and region (22) acts to inhibit decay of the space charge and to increase the lifetime of the induced electro-optic effect. The waveguide may comprise a twin hole optical fiber (11) with internal electrodes (12A, 14A), where the region (22) comprises a borosilicate layer concentrically disposed about one of the electrodes.
53 MMI Thermo-optic coupler EP00303626.6 2000-04-28 EP1048971A1 2000-11-02 Paiam, Reza

A multi-mode interference coupler is disclosed for coupling light between ports. The MMI coupler is a planar waveguide having a first input port for launching light into a core of the planar waveguide which has first refractive index n1. The waveguide is dimensioned to have a response that confines light launched therein to a single mode in one dimension, and multi-mode in another dimension. Two other ports are provided for receiving light launched into and propagating through the core from the input port. A polymer cladding of a second material having a refractive index n2 covers at least a portion of the core. A heater is provided and is thermally coupled to the cladding for heating the cladding when a control signal is applied.

54 Variable optical filter EP00303642.3 2000-04-28 EP1048962A2 2000-11-02 Diemeer, Mart

The present invention relates to a variable optical filter that can be used to filter an incoming signal, attenuate an incoming signal or in one configuration switch an incoming signal from one path to another. The present invention has found that an accurate and economical variable optical filter can be created by using an elastomeric material having a high coefficient of expansion in cooperation with a means for locally varying the temperature of the elastomeric material as an actuator for moving a reflective surface within the optical filter. The actuator can be operated in a controlled manner for example, to effect a tilt of the reflective surface for switching or attenuating an optical signal, or to vary the resonant wavelengths of a resonant cavity between partially reflective surfaces. In accordance with the invention there is provided, a variable optical filter comprising an input port and an output port; a first at least partially reflective surface disposed to receive a beam of light launched from the input port; an elastomeric material for supporting and varying the position of the at least partially reflective surface with respect to the input port; a heater for applying variable amounts of heat to the elastomeric material to move or pivot the at least partially reflective surface relative to the input port; and, control means for controlling the heater and for providing a signal to apply variable amounts of heat.

55 Variable optical fiber Bragg filter arrangement EP99101327.7 1990-12-21 EP0924546A1 1999-06-23 Morey, William W.; Glenn, William H.; Leonberger, Frederick J.; Meltz, Gerald

A variable light filtering arrangement (10) includes at least one optical fiber section (11) including a waveguiding core (13), and at least one permanent Bragg grating region (12) in the optical fiber section. The grating region includes a plurality of grating elements constituted by periodic refractive index variations of a predetermined initial periodicity and cumulatively redirecting, of the light launched into the core for guided propagation therein, that having an axial wavelength within a narrow band around a central wavelength that is determined by the periodicity and refractive index variations of the grating elements. At least one of the periodicity and refractive index variations of the grating region is controlledly modified in such a manner as to temporarily change the central wavelength within a predetermined wavelength range.

56 Endlos-Polarisationsregelung EP92108244.2 1992-05-15 EP0514787A3 1993-01-20 Das, Chandan, Dipl.-Ing.

Insbesondere für optische Überlagerungsempfänger ist es notwendig, die Polarisation des lokal erzeugten Lichtes der des Empfangslichtes nachzuregeln. Die Polarisationsregelung erfolgt dabei durch Verstellung der Verzögerung doppelbrechender Elemente, die nach einer Anzahl gleichgerichteter Verstellschritte an eine Verstellgrenze gelangen können und zurückgestellt werden müssen. Dabei ergibt sich das Problem, daß schnelle Änderungen der Polarisation des Eingangslichtes auch während Rückstellphase berücksichtigt werden müssen, außerdem sollten auch nichtideale doppelbrechende Elemente verwendet werden. Erfindungsgemäß werden vier doppelbrechende Elemente verwendet, von denen die im Lichtweg ersten beiden Elemente der normalen Regelung und die beiden folgenden Elemente der Regelung während der Rückstellprozedur dienen.

57 VARIABLE OPTICAL FIBER BRAGG FILTER ARRANGEMENT EP91903518.0 1990-12-21 EP0507882A1 1992-10-14 MOREY, William, W.; LEONBERGER, Fred, J.; GLENN, William, H.; MELTZ, Gerald
Un agencement de filtrage de lumière variable (10) comprend au moins une section de fibre optique (11) comportant une âme (13) de guidage d'onde, ainsi qu'au moins une région de diffraction (12) de Bragg permanente dans la section de fibre optique. La région de diffraction comprend une pluralité d'éléments de diffraction constitués par des variations d'indice de réfraction périodique d'une périodicité initiale prédéterminée, et réorientant de manière cumulative la lumière envoyée dans l'âme dans laquelle sa propagation est guidée, ayant une longueur d'onde axiale comprise dans une bande étroite autour d'une longueur d'onde centrale, laquelle est déterminée par les variations de périodicité et d'indice de réfraction des éléments de diffraction. Au moins une des variations de périodicité et d'indice de réfraction de la région de diffraction, est modifiée de manière régulée, de manière à changer temporairement la longueur d'onde centrale située dans une plage de longueur d'ondes prédéterminée.
58 波長変換装置、制御光生成装置、波長変換方法、および制御光生成方法 JP2017082647 2017-04-19 JP2018180406A 2018-11-15 加藤 智行; 渡辺 茂樹; 星田 剛司
【課題】高い変換効率で、任意波長への広帯域での波長変換を実現するための波長変換器を提供する。
【解決手段】波長変換装置は、制御光生成部と非線形光学媒質とを備え、第1の周波数の入信号光を、同位相または位相共役である第2の周波数の出力信号光に変換する。制御光生成部は、第1の連続発振光と第2の連続発振光を、互いに直交する方向の偏波を有すると共に、第1の周波数と第2の周波数との差分と等しい周波数間隔を有するように出力する。非線形光学媒質は、入力信号光と第1の連続発振光と第2の連続発振光とを相互位相変調して、出力信号光を生成する。制御光生成部は、出力信号光の強度に基づいて第1の連続発振光と第2の連続発振光の各位相の変調のタイミングを互いに合わせるよう制御する。
【選択図】図2
59 受発光システム JP2016205885 2016-10-20 JP2018066674A 2018-04-26 都甲 康夫; 川上 康之
【課題】受発光システムの小型化、構造の簡素化等を図ること。
【解決手段】対象物体に光を照射し当該光により生じる反射光を用いて当該対象物体を検出する受発光システムであって、複数の光制御部を有する平板状の光制御装置と、少なくとも1つの光制御部に対して光を入射させる入光装置と、光制御部からの出射光を受光する受光装置と、入光装置と受光装置の動作を制御して対象物体を検出する制御装置を含む。光制御装置は、一対の基板間に複数の光制御部を保持する液晶素子、液晶素子を駆動する駆動装置を含む。各光制御部は、例えば、一対の電極、一対の電極の間に配置される高抵抗膜、少なくとも高抵抗膜と重なる領域に配置される液晶層を含む。
【選択図】図1
60 波数ドリフトを含むパルスの光パラメトリック増幅のための方法およびその装置 JP2014546464 2012-12-11 JP6114303B2 2017-04-12 ユゴノ,エマニュエル; ミュソ,アルノー; クドリンスキ,アレグザンドル
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