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公开(公告)号：JP2016507892A
公开(公告)日：2016-03-10
申请号：JP2015549558
申请日：2013-12-17
Applicant: デイビッド ウェルフォード, , デイビッド ウェルフォード, , バドゥル エルマーナオウイ, , バドゥル エルマーナオウイ,
Inventor： デイビッド ウェルフォード， , デイビッド ウェルフォード， , バドゥル エルマーナオウイ， , バドゥル エルマーナオウイ，
CPC classification number: G01J9/0246 , A61B5/0066 , A61B5/0073 , G01B9/02091 , G01J3/0245 , G01J3/10 , G01J3/12 , G01J2003/1213 , G01J2009/0226 , H01S3/06791
Abstract: 本発明は、概して、光の波長放出を幅狭化するための方法およびシステムに関する。ある側面では、本発明の方法は、フィルタを通して光を伝送し、光の一部がフィルタを通して再び通過する前に、少なくとも2回、フィルタリングされた光の一部を利得チップアセンブリを通して通過させるステップを伴う。一実施形態において、少なくとも2回、前記フィルタリングされた光の一部を利得チップアセンブリを通して通過させるステップは、1回目に、前記利得チップアセンブリ内の利得媒体を通して前記光を送信するステップと、前記利得チップアセンブリから射出する前記光の一部を前記利得チップアセンブリを通して反射させ、前記フィルタを通して再び通過する前に、前記利得チップアセンブリ内の利得媒体を通る2回面の通過をもたらすステップと、を含む。
Abstract translation: 本发明一般涉及一种用于窄的光的波长发射的方法和系统。 在一个方面，本发明的方法中，所述光通过所述滤光器，所述光的所述部分之前，再次通过过滤器，所述传送步骤的至少两倍，通过增益芯片组件的经滤波的光的一部分 用。 在一个实施方案中，至少2倍，穿过的光，在第一时间增益芯片组件的过滤部分，和透射光通过在所述增益芯片组件中的增益介质的步骤，所述增益 从尖端组件发射的光的一部分被通过增益芯片组件反射的，之前通过过滤器再次通过，包括导致两次通过平面通过增益介质传递中的步骤，所述增益芯片组件 。
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22.发明专利
公开(公告)号：JP2010204308A
公开(公告)日：2010-09-16
申请号：JP2009048608
申请日：2009-03-02
Applicant: Osaka Univ , 国立大学法人大阪大学
Inventor： KONISHI TAKESHI , KATO TAKUYA , GOTO HIROOMI
CPC classification number: G01J11/00 , G01J3/02 , G01J3/0213 , G01J3/0218 , G01J3/0245
Abstract: PROBLEM TO BE SOLVED: To provide a waveform reconstruction device capable of easily reconstructing the accurate time waveform of an optical signal without using an ultrafast time gate or a reference light source. SOLUTION: The waveform reconstruction device 140 includes: a phase spectrum calculation section 143 which calculates power spectrum of an output optical signal with respect to each of input optical signals with multiple intensities when a phase spectrum of each of the input optical signals with multiple intensities is assumed to have a predetermined phase spectrum, by simulating propagation of the input optical signal through an optical fiber using a parameter relating to self-phase modulation of the optical fiber, and calculates, as the phase spectrum of the input optical signal, the predetermined phase spectrum in which the difference value between the calculated power spectrum and a measured power spectrum is equal to or less than a predetermined threshold value; and a waveform reconstruction section 144 which reconstructs the time waveform of the input optical signal by frequency/time transforming the calculated phase spectrum and the power spectrum of the input optical signal. COPYRIGHT: (C)2010,JPO&INPIT
Abstract translation: 要解决的问题：提供一种能够容易地重构光信号的精确时间波形而不使用超快时间门或参考光源的波形重建装置。 解决方案：波形重建装置140包括：相位谱计算部分143，当每个输入光信号的相位谱具有多个强度时，相对于具有多个强度的输入光信号，输出光信号的功率谱， 通过使用与光纤的自相位调制有关的参数通过光纤模拟输入光信号的传播，假设多个强度具有预定的相位频谱，并且计算输入光信号的输入光信号的相位谱， 其中所计算的功率谱与测量的功率谱之间的差值等于或小于预定阈值的预定相位频谱; 以及波形重建部分144，其通过频率/时间变换计算出的相位频谱和输入光信号的功率谱来重构输入光信号的时间波形。 版权所有（C）2010，JPO＆INPIT
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公开(公告)号：KR1020090095464A
公开(公告)日：2009-09-09
申请号：KR1020090010115
申请日：2009-02-09
Applicant: 소니 주식회사
IPC: A61B3/00
CPC classification number: G01J3/02 , G01J3/0245 , G01J3/42 , G01N21/3586 , G02B6/29376
Abstract: A terahertz spectrometer is provided to achieve the miniaturization of the terahertz spectrometer by inducing a pulse light to an emitter through an optical fiber without using an optical lens. A terahertz spectrometer includes an optical fiber(11C) and an emitter(12), and the emitter is distributed from a gain fiber configuring an ultra-short pulse oscillator. The emitter generates a terahertz wave by using the pulse light that passes through the optical fiber via the gain fiber, and the optical fiber offsets the spreading of the pulse width of the pulse light outputted from the gain fiber.
Abstract translation: 提供太赫兹光谱仪以通过在不使用光学透镜的情况下通过光纤向发射器施加脉冲光来实现太赫兹光谱仪的小型化。 太赫兹光谱仪包括光纤（11C）和发射极（12），发射极分布在构成超短脉冲振荡器的增益光纤上。 发射器通过使用通过增益光纤穿过光纤的脉冲光产生太赫兹波，并且光纤抵消从增益光纤输出的脉冲光的脉冲宽度的扩展。
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公开(公告)号：KR1020130055672A
公开(公告)日：2013-05-28
申请号：KR1020137008439
申请日：2011-08-26
Applicant: 생-고뱅 퍼포먼스 플라스틱스 코포레이션
Inventor： 파밀리아,아지즈,마푸드 , 새클포드,데이비드,에스. , 맥힐레프,나피 , 짐머만,마이크,에이.
CPC classification number: G01J3/021 , G01J3/0245 , G01J3/42 , G01N15/082 , G01N21/3554 , G01N21/39 , G01N2021/399
Abstract: 본 발명은 증기 투과속도의 측정을 위해 실행되는 캐비티 링-다운 분석기(CRDS) 기술을 이용하는 시스템 및 방법을 대상으로 한다. 일 실시예에서, 측정되는 증기 함량은 광 캐비티 내에 포함된다. 광이 그 다음에 한계치 수준까지 캐비티에 조사되며 조사된 광의 지연 시간이 측정된다. 조사된 광의 파장이 증기의 흡수 특징과 공진할 때, 감쇠 시간은 증기 함량의 기능으로서 선형으로 증가된다. 이 방식으로, 증기 함량은 더 긴 지연 시간을 야기하며 그에 따라 필름을 통과하는 증기의 양(필름 투과속도)이 실시간으로 판단될 수 있다.
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25.发明专利
公开(公告)号：JP5158810B2
公开(公告)日：2013-03-06
申请号：JP2009048608
申请日：2009-03-02
Applicant: 国立大学法人大阪大学
CPC classification number: G01J11/00 , G01J3/02 , G01J3/0213 , G01J3/0218 , G01J3/0245
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Patent Agency Ranking
公开(公告)号：JP2009210423A
公开(公告)日：2009-09-17
申请号：JP2008053804
申请日：2008-03-04
Inventor： FORMANEK FLORIAN , BRUN MARC-AURELE
IPC: G01J3/28 , G01N21/35 , G01N21/3586
CPC classification number: G01J3/02 , G01J3/0245 , G01J3/42 , G01N21/3586 , G02B6/29376
Abstract: PROBLEM TO BE SOLVED: To provide a terahertz spectroscopic apparatus for simplifying a constitution, and measuring a sample. SOLUTION: An optical fiber OF2 is directly coupled to a gain fiber 11C in an ultrashort fiber laser device 11 through an optical coupler 11D. A pulse light (a pump light) is output from the gain fiber 11C, and guided to an emitter 12 through the optical fiber OF2. COPYRIGHT: (C)2009,JPO&INPIT
Abstract translation: 要解决的问题：提供一种用于简化结构并测量样品的太赫兹分光装置。 解决方案：光纤OF2通过光耦合器11D直接耦合到超短光纤激光器装置11中的增益光纤11C。 脉冲光（泵浦光）从增益光纤11C输出，并通过光纤OF2被引导到发射极12。 版权所有（C）2009，JPO＆INPIT
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公开(公告)号：EP3179220A1
公开(公告)日：2017-06-14
申请号：EP15199309.4
申请日：2015-12-10
Applicant: Aragon Photonics Labs, S.L.U. , Fibercom S.L.
CPC classification number: G01J3/027 , G01J3/0245 , G01J3/0264 , G01J3/0275 , G01J3/0297 , G01J3/2803 , G01J3/32 , G01J3/4412 , G01J9/0246 , G01J9/04
Abstract: A system and method of optical spectrum analysis that circumvents the trade-off between resolution and sensitivity by combining two spectral measurements: a first spectrum (102) from first spectral measurement means (240), having high resolution and low sensitivity; and a second spectrum (103) from second spectral measurement means (220), having lower resolution but higher resolution. The input of the of the first spectral measurement means (240) is amplified by an optical amplifier (230), being the effects induced by said amplifier (230) on the first spectrum (102) corrected at processing means (270) by comparison with the second spectrum (103).
Abstract translation: 一种光谱分析的系统和方法，其通过组合两个光谱测量来避开分辨率和灵敏度之间的折衷：来自第一光谱测量装置（240）的具有高分辨率和低灵敏度的第一光谱（102） 和来自第二光谱测量装置（220）的第二光谱（103），具有较低的分辨率但较高的分辨率。 第一光谱测量装置（240）的输入通过光放大器（230）放大，该光放大器是由所述放大器（230）对在处理装置（270）处校正的第一光谱（102） 第二谱（103）。
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28.发明公开Systems and methods for coherent Raman spectroscopy 审中-公开Systeme und Verfahren zurkohärentenRaman-Spektroskopie
公开(公告)号：EP2982947A1
公开(公告)日：2016-02-10
申请号：EP14002783.0
申请日：2014-08-08
Applicant: Baden-Württemberg Stiftung gGmbH
Inventor： Steinle, Tobias , Steinmann, Andy , Giessen, Harald
CPC classification number: G01J3/44 , G01J3/0245 , G01J3/10
Abstract: A system (1; 2; 3) for coherent Raman spectroscopy, comprises a first optical parametric amplifier (30) providing a first light pulse (100), a pulsed laser (20) providing a second light pulse (200) such that a first fraction (201) of the second light pulse (200) pumps the first optical parametric amplifier (30), and a cw-laser (10) seeding the first optical parametric amplifier (30). Therein, the first light pulse (100) and a second fraction (202) of the second light pulse (200) are converted into a synchronised pump pulse (103) and Stokes pulse (203) for coherent Raman spectroscopy with a predetermined tunable frequency difference between the pump pulse (103) and the Stokes pulse (203).
Abstract translation: 一种用于相干拉曼光谱的系统（1; 2; 3）包括提供第一光脉冲（100）的第一光参量放大器（30），提供第二光脉冲（200）的脉冲激光器（20） 第二光脉冲（200）的分数（201）泵送第一光参量放大器（30），以及cw激光器（10），接合第一光参量放大器（30）。 其中，第二光脉冲（200）的第一光脉冲（100）和第二分数（202）被转换成具有预定可调谐频率差的相干拉曼光谱的同步泵浦脉冲（103）和斯托克斯脉冲（203） 在泵脉冲（103）和斯托克斯脉冲（203）之间。
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公开(公告)号：EP2098839A2
公开(公告)日：2009-09-09
申请号：EP09003036.2
申请日：2009-03-03
Applicant: Sony Corporation
Inventor： Formanek, Florian , Brun, Marc-Auréle
IPC: G01J3/42
CPC classification number: G01J3/02 , G01J3/0245 , G01J3/42 , G01N21/3586 , G02B6/29376
Abstract: A terahertz spectrometer includes an optical fiber and an emitter. The optical fiber is branched from a gain fiber constituting an ultra-short pulse oscillator. The emitter generates a terahertz wave from a pulse beam guided from the gain fiber through the optical fiber.
Abstract translation: 太赫兹光谱仪包括光纤和发射器。 光纤从构成超短脉冲振荡器的增益光纤分支。 发射器从通过光纤从增益光纤引导的脉冲光束产生太赫兹波。
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公开(公告)号：EP1949151A2
公开(公告)日：2008-07-30
申请号：EP06837744.9
申请日：2006-11-16
Applicant: OMNI Sciences, Inc.
Inventor： ISLAM, Mohammed, N.
CPC classification number: G01J3/108 , G01B9/02091 , G01J3/0218 , G01J3/0245 , G01J3/42 , G01J2003/102 , G01J2003/423 , G02B6/29349 , G02F1/365 , G02F2001/3528 , G02F2202/32 , H01S3/06725 , H01S3/06754 , H01S3/094007 , H01S3/094069 , H01S3/094076 , H01S3/1024 , H01S3/302 , H01S5/0064 , H01S5/0085 , H01S5/0092 , H01S5/1092 , H01S5/146 , H01S5/4012 , H01S2301/085
Abstract: A broadband light source includes one or more laser diodes that are capable of generating a pump signal having a wavelength shorter than 2.5 microns, a pulse width of at least 100 picoseconds and a pump optical spectral width. The light source also includes one or more optical amplifiers that are coupled to the pump signal and are capable of amplifying the pump signal to a peak power of at least 500 W. The light source further includes a first fiber that is coupled to the one or more optical amplifiers. The first fiber including an anomalous group-velocity dispersion regime and a modulational instability mechanism that operates to modulate the pump signal. In one particular embodiment, the pump signal wavelength resides in the anomalous group-velocity dispersion regime of the first fiber and where different intensities in the pump signal can cause relative motion between different parts of the modulated pump signal produced through modulational instability in the first fiber. The light source also including a nonlinear element that is coupled to the first fiber that is capable of broadening the pump optical spectral width to at least 100 nm through a nonlinear effect in the nonlinear element.
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