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公开(公告)号:US09246312B2
公开(公告)日:2016-01-26
申请号:US14476838
申请日:2014-09-04
Applicant: Ludwig-Maximilians-Universität München
Inventor: Robert Huber , Wolfgang Wieser , Thomas Klein , Christoph Eigenwillig , Benjamin Biedermann , Dieter Muellner , Michael Eder
CPC classification number: H01S5/423 , G01J3/26 , G02B6/29358 , G02B26/001 , H01S3/105 , H01S5/02284 , H01S5/141 , H01S5/183
Abstract: A Fabry-Pérot tuneable filter device is described with reflecting elements separated by an optical path length to form an optical resonator cavity. A first actuator means is directly or indirectly coupled with a first reflecting element. And the first actuator means is configured to modulate the optical path length between first and second reflecting elements by a modulation amplitude to thereby sweep the optical resonator cavity through a band of optical resonance frequencies with a sweep frequency of 70 kHz or more. And the mechanical coupling between selected elements of the arrangement is sufficiently low such that when operated at the sweep frequency, the selected elements act as a system of coupled oscillating elements. In addition or alternatively, the first actuator means is directly or indirectly coupled with the first reflecting element so as to substantially drive the first reflecting element only.
Abstract translation: 通过用光程长度分离的反射元件描述法布里 - 珀罗可调谐滤波器装置,以形成光谐振腔。 第一致动器装置与第一反射元件直接或间接耦合。 并且第一致动器装置被配置为通过调制幅度来调制第一和第二反射元件之间的光路长度,从而通过具有70kHz或更大的扫频频率的光学谐振频率带扫掠光学谐振腔。 并且所述装置的选定元件之间的机械耦合足够低,使得当以扫描频率操作时,所选择的元件用作耦合振荡元件的系统。 另外或替代地,第一致动器装置与第一反射元件直接或间接耦合,以便仅基本驱动第一反射元件。
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公开(公告)号:US09709380B2
公开(公告)日:2017-07-18
申请号:US14386658
申请日:2013-03-21
Applicant: Ludwig Maximilians Universität München
Inventor: Robert Alexander Huber , Thomas Klein , Wolfgang Wieser
IPC: G01B9/02
CPC classification number: G01B9/02091 , G01B9/02004 , G01B9/02041 , G01B9/02048 , G01B9/02069 , G01B9/02083 , G01B2290/45
Abstract: At least one embodiment of the method is designed to create a two-dimensional image of a three-dimensional sample. The method comprises the following steps: provision of a wave-length-tunable light source (1) that emits primary radiation (P) with wavelengths that vary over time; sampling of location points of the sample (2) with the primary radiation (P); collection of secondary radiation (S), wherein the secondary radiation (S) is a part of the primary radiation (P) reflected by the sample (2); creation of an interferometer-based detection signal for a plurality of sample areas, each with at least one location point, using a detection unit (4), wherein the detection signal is created as a difference signal from two output signals of a beam splitter (61) that receives reference radiation (R) and/or secondary radiation (S) at two inputs, wherein the reference radiation (R) is a portion of the primary radiation (P) that is not guided to the sample (2); and determination of a brightness value for at least one of the sample areas from the associated detection signal, wherein the determination of the brightness values is not substantially based on the summation of the individual signal amplitudes of the results of a Fourier transformation.
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公开(公告)号:US09638638B2
公开(公告)日:2017-05-02
申请号:US14890109
申请日:2014-05-09
Applicant: Ludwig-Maximilians-Universität München
Inventor: Robert Alexander Huber , Thomas Klein , Wolfgang Wieser , Sebastian Karpf , Matthias Eibl
IPC: G01J3/44 , G01N21/65 , H01S3/067 , H01S3/10 , H01S3/23 , H01S3/30 , H01S3/0941 , H01S3/16 , H01S3/00 , H01S3/094
CPC classification number: G01N21/65 , G01J3/44 , G01J3/4412 , G01N2021/655 , G01N2201/06113 , G01N2201/0683 , G01N2201/0697 , H01S3/0064 , H01S3/0078 , H01S3/06758 , H01S3/094069 , H01S3/09415 , H01S3/10015 , H01S3/1618 , H01S3/2391 , H01S3/302
Abstract: Disclosed herein is a system (10) for measuring light induced transmission or reflection changes, in particular due to stimulated Raman emission. The system comprises a first light source (12) for generating a first light signal having a first wavelength, a second light source (14) for generating a second light signal having a second wavelength, an optical assembly (16) for superposing said first and second light signals at a sample location (18), and a detection means (24) for detecting a transmitted or reflected light signal, in particular a stimulated Raman signal caused by a Raman-active medium when located at said sample location. Here in at least one of the first and second light sources (12, 14) is one or both of actively controllable to emit a time controlled light pattern or operated substantially in CW mode and provided with an extra cavity modulation means (64) for generating a time controlled light pattern. The detection means (24) is capable of recording said transmitted or reflected light signal, in particular stimulated Raman signal, as a function of time.
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公开(公告)号:US20160091429A1
公开(公告)日:2016-03-31
申请号:US14890109
申请日:2014-05-09
Applicant: LUDWIG-MAXIMILIANS-UNIVERSITÄT MÜNCHEN
Inventor: Robert Alexander Huber , Thomas Klein , Wolfgang Wieser , Sebastian Karpf , Matthias Eibl
CPC classification number: G01N21/65 , G01J3/44 , G01J3/4412 , G01N2021/655 , G01N2201/06113 , G01N2201/0683 , G01N2201/0697 , H01S3/0064 , H01S3/0078 , H01S3/06758 , H01S3/094069 , H01S3/09415 , H01S3/10015 , H01S3/1618 , H01S3/2391 , H01S3/302
Abstract: Disclosed herein is a system (10) for measuring light induced transmission or reflection changes, in particular due to stimulated Raman emission. The system comprises a first light source (12) for generating a first light signal having a first wavelength, a second light source (14) for generating a second light signal having a second wavelength, an optical assembly (16) for superposing said first and second light signals at a sample location (18), and a detection means (24) for detecting a transmitted or reflected light signal, in particular a stimulated Raman signal caused by a Raman-active medium when located at said sample location. Here in at least one of the first and second light sources (12, 14) is one or both of actively controllable to emit a time controlled light pattern or operated substantially in CW mode and provided with an extra cavity modulation means (64) for generating a time controlled light pattern. The detection means (24) is capable of recording said transmitted or reflected light signal, in particular stimulated Raman signal, as a function of time.
Abstract translation: 本文公开了一种用于测量光诱导的透射或反射变化的系统(10),特别是由于受激的拉曼发射。 该系统包括用于产生具有第一波长的第一光信号的第一光源(12),用于产生具有第二波长的第二光信号的第二光源(14),用于叠加所述第一波长的光学组件 以及检测装置(24),用于检测发射或反射的光信号,特别是当位于所述采样位置时由拉曼活性介质引起的受激拉曼信号。 这里,第一和第二光源(12,14)中的至少一个是主要可控制的一个或两个以发射时间控制的光图案或基本上以CW模式操作,并且设置有用于产生的额外的空腔调制装置(64) 时间控制的光图案。 检测装置(24)能够作为时间的函数记录特定的受激拉曼信号的所述发射或反射的光信号。
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公开(公告)号:US20140369374A1
公开(公告)日:2014-12-18
申请号:US14476838
申请日:2014-09-04
Applicant: Ludwig-Maximilians-Universität München
Inventor: Robert Huber , Wolfgang Wieser , Thomas Klein , Christoph Eigenwillig , Benjamin Biedermann , Dieter Muellner , Michael Eder
CPC classification number: H01S5/423 , G01J3/26 , G02B6/29358 , G02B26/001 , H01S3/105 , H01S5/02284 , H01S5/141 , H01S5/183
Abstract: A Fabry-Pérot tuneable filter device is described with reflecting elements separated by an optical path length to form an optical resonator cavity. A first actuator means is directly or indirectly coupled with a first reflecting element. And the first actuator means is configured to modulate the optical path length between first and second reflecting elements by a modulation amplitude to thereby sweep the optical resonator cavity through a band of optical resonance frequencies with a sweep frequency of 70 kHz or more. And the mechanical coupling between selected elements of the arrangement is sufficiently low such that when operated at the sweep frequency, the selected elements act as a system of coupled oscillating elements. In addition or alternatively, the first actuator means is directly or indirectly coupled with the first reflecting element so as to substantially drive the first reflecting element only.
Abstract translation: 通过用光程长度分离的反射元件描述法布里 - 珀罗可调谐滤波器装置,以形成光谐振腔。 第一致动器装置与第一反射元件直接或间接耦合。 并且第一致动器装置被配置为通过调制幅度来调制第一和第二反射元件之间的光路长度,从而通过具有70kHz或更大的扫频频率的光学谐振频率带扫掠光学谐振腔。 并且所述装置的选定元件之间的机械耦合足够低,使得当以扫描频率操作时,所选择的元件用作耦合振荡元件的系统。 另外或替代地,第一致动器装置与第一反射元件直接或间接耦合,以便仅基本驱动第一反射元件。
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