公开(公告)号：EP2414794A1

公开(公告)日：2012-02-08

申请号：EP10758114.2

申请日：2010-03-31

Applicant: Teknologian Tutkimuskeskus VTT

Inventor： SAARI, Heikki ,  HOLMLUND, Christer ,  KANTOJÄRVI, Uula ,  MANNILA, Rami ,  LAMMINPÄÄ, Antti ,  TEPPOLA, Pekka

IPC: G01J3/26 ,  G02B26/00

CPC classification number: G01J3/51 ,  G01J3/02 ,  G01J3/0208 ,  G01J3/0235 ,  G01J3/12 ,  G01J3/26 ,  G01J3/32

Abstract: The invention relates to a system and a method for optical measurement of a target, wherein the target is illuminated, either actively illuminated, reflecting ambient light, or self illuminating, and a measurement light beam received from the target or through it is detected. The prior art optical measurement systems generally include mechanical filter wheels and photomultiplier tubes, which cause the equipment to be expensive, large-sized and often not sufficiently accurate and stable. The objective of the invention is achieved with a solution, in which the illuminating light beam and/or measurement light beam is led through a Fabry-Perot interferometeror a set of two or more Fabry-Perot Interferometers, and the Fabry-Perot interferometer or a set of two or more Fabry-Perot Interferometersis controlled into different modes during the measurement of a single target. The invention can be applied inoptical measurements where, for example, reflectance, absorption of fluorescence of the target is measured.

公开(公告)号：EP2333501A1

公开(公告)日：2011-06-15

申请号：EP09306159.6

申请日：2009-11-30

Applicant: Horiba Jobin Yvon SAS

Inventor： Kashiwagi, Shinsuke ,  Froigneux, Emmanuel ,  Roussel, Bernard

IPC: G01J3/44 ,  G02B21/00

CPC classification number: G02B21/0076 ,  G01J3/02 ,  G01J3/0208 ,  G01J3/021 ,  G01J3/0235 ,  G01J3/0237 ,  G01J3/0289 ,  G01J3/44 ,  G02B7/005 ,  G02B21/0032

Abstract: An optical measurement apparatus (100) comprises a light source (1) for generating an incident light beam (4), a first optical system (13, 9a, 9b, 9c) for directing said incident light beam from said light source to said microscope objective (25) along an incident beam path, a spectrometer (27) and a measurement detector (7) for measuring secondary light (5) emitted from said sample (23), a second optical system (14a, 14b, 17) for collecting secondary light (5) generated from said sample (23) and for directing said secondary light toward said spectrometer (27) along a return beam path. According to the invention, the apparatus comprises at least one out of a 1 st switching mirror (10) and a 2 nd switching mirror (15), said 1 st switching mirror (10) having a position where it is inserted in said incident light path for directing said incident light beam toward a first detector (6) for optical misalignment detection of said incident beam path and said 2 nd switching mirror (15) having a position where it is inserted in said incident light path for directing said incident light beam along said return beam path toward a second detector for detecting optical misalignment in said return beam path.

Abstract translation: 光学测量装置（100）包括用于产生入射光束（4）的光源（1），用于将来自所述光源的入射光束引导到所述显微镜的第一光学系统（13,9a，9b，9c） 物镜（25），用于测量从所述样品（23）发射的二次光（5）的光谱仪（27）和测量检测器（7），用于收集 从所述样品（23）产生的二次光（5）并且用于沿着返回光束路径将所述次级光导向所述光谱仪（27）。 根据本发明，该装置包括第一开关镜（10）和第二开关镜（15）中的至少一个，所述第一开关镜（10）具有插入入射光的位置 用于将所述入射光束引导到第一检测器（6）的路径，用于所述入射光束路径的光学偏移检测和所述第二转换镜（15），其具有插入所述入射光路中的位置，用于引导所述入射光束 沿着所述返回光束路径朝向用于检测所述返回光束路径中的光学未对准的第二检测器。

公开(公告)号：EP2287591A3

公开(公告)日：2011-05-11

申请号：EP10173120.6

申请日：2010-08-17

Applicant: Opsolution Nanophotonics GmbH

Inventor： Sandhagen, Carl

IPC: G01N21/35 ,  G01N33/00 ,  G01N1/22

CPC classification number: G01N21/534 ,  G01J3/02 ,  G01J3/0235 ,  G01J3/027 ,  G01J3/0289 ,  G01J3/26 ,  G01J3/32 ,  G01J3/42 ,  G01N21/31 ,  G01N33/0037 ,  G01N2021/151 ,  G01N2021/3174 ,  Y02A50/245

Abstract: Eine Vorrichtung zur Bestimmung der Konzentration von NO 2 in Gasgemischen, insbesondere Abgasen von Dieselmotoren, umfasst eine Lichtquelle zur Ausgabe von Licht in einen Lichtweg; eine Sensoreinrichtung zum Empfang zumindest eines Teils des über den Lichtweg zur Sensoreinrichtung vordringenden Lichtes, wobei der Verlauf des Lichtweges so gewählt ist, dass dieser das zu untersuchende Gas durchsetzt, wobei die Sensoreinrichtung so gestaltet ist, dass diese Signale liefert die das Spektrum des erfassten Lichtes beschreiben; und eine Auswertungsschaltung zur Auswertung der durch die Sensoreinrichtung generierten Signale, wobei die Sensoreinrichtung derart gestaltet ist, die Bestimmung der NO 2 -Konzentration erfolgt indem die Bestimmung innerhalb eines eingeschränkten spektralen Bereiches erfolgt, in dem eine ausgeprägte absolute oder relative Variation des Absorptionskoeffizienten des NO 2 und eine geringe absolute oder relative Variation der weiteren Gase vorliegt. Hierdurch ist es möglich, für die Konzentration von NO 2 im Abgas eines Verbrennungsmotors indikative Signale über einen langen Zeitraum hinweg zuverlässig zu generieren.

公开(公告)号：EP2263061A1

公开(公告)日：2010-12-22

申请号：EP09727747.9

申请日：2009-04-02

Applicant: Sirona Dental Systems GmbH

Inventor： THIEL, Frank ,  FORNOFF, Peter

IPC: G01B11/02 ,  G01B11/24 ,  G01J3/50 ,  G01N21/25

CPC classification number: G01B11/026 ,  A61C9/0053 ,  G01B11/24 ,  G01B2210/50 ,  G01J3/02 ,  G01J3/0208 ,  G01J3/021 ,  G01J3/0229 ,  G01J3/0235 ,  G01J3/0237 ,  G01J3/10 ,  G01J3/50 ,  G01J3/508 ,  G01N21/255 ,  G02B21/0028 ,  G02B21/0032 ,  G02B21/0064

Abstract: The invention relates to a device and a method for optical 3D measurement, wherein the device can be shifted between a first mode for optical 3D measurement using a chromatic confocal measurement method or the triangulation measurement method and a second mode for color measurement. In the first mode, a broadband illuminating beam is focused on a first plane and in the second mode the broadband illuminating beam is focused onto a second plane outside the first plane at a distance d from the surface of the measured object.

公开(公告)号：EP1929278A1

公开(公告)日：2008-06-11

申请号：EP06769715.1

申请日：2006-08-17

Applicant: GLUCOSTATS SYSTEM PTE LTD

Inventor： ZHANG, Xiqin ,  TING, Choon Meng

IPC: G01N21/35 ,  G01N21/00 ,  A61B5/1455 ,  G01N33/49

CPC classification number: G01J3/108 ,  A61B5/14532 ,  A61B5/1455 ,  G01J3/02 ,  G01J3/0229 ,  G01J3/0232 ,  G01J3/0235

Abstract: The present invention relates to an arrangement for a selection of a wavelength including a wavelength source for providing a plurality of wavelengths, a wavelength selector for allowing a selection of a desired wavelength from the wavelength source, and a wavelength detector to detect a selected wavelength for subsequent use.

公开(公告)号：EP1744199A1

公开(公告)日：2007-01-17

申请号：EP06117072.6

申请日：2006-07-12

Applicant: Hach Lange GmbH

Inventor： Mitreiter, Andreas ,  Hanschke, Clemens

IPC: G02B27/44 ,  G02B5/18 ,  G01J3/18

CPC classification number: G01J3/1804 ,  G01J3/02 ,  G01J3/0235 ,  G01J3/0262 ,  G01J3/04 ,  G01J3/42 ,  G02B5/18 ,  G02B27/4244

Abstract: Die Erfindung betrifft ein kreisscheibenförmiges Trägersystem mit einer Mehrzahl integrierter Beugungsstrukturen zur Spektralzerlegung von Licht der Wellenlängen 340 - 800 nm, wobei jede Beugungsstruktur eine Schicht aus einem transparenten Kunststoff umfasst, die eine zur Beugung einer innerhalb des Wellenlängenspektrums des Lichts liegende Wellenlänge geeignete Mikrostruktur aufweist, und das Trägersystem mindestens zwei Beugungsstrukturen zur Beugung von Licht unterschiedlicher Wellenlänge umfasst.

Abstract translation: 圆盘形载体系统（100）具有许多用于光谱分裂波长为340-800nm的光的集成衍射结构（1-38）。 每个衍射结构包括透明塑料层，其具有用于在波长光谱内的光衍射的波长合适的微结构。 载体系统包括用于不同波长的光的衍射的两个衍射结构。 还包括以下独立权利要求：（A）制造圆盘形载体系统的方法; 和（B）光度计。

公开(公告)号：EP1596238A2

公开(公告)日：2005-11-16

申请号：EP05009608.0

申请日：2005-05-02

Applicant: Olympus Corporation

Inventor： Nakata, Tatsuo

IPC: G02B21/00

CPC classification number: G02B21/0032 ,  G01J3/0208 ,  G01J3/0229 ,  G01J3/0235 ,  G01J3/4406 ,  G01N21/6456 ,  G01N2021/6463 ,  G02B21/002 ,  G02B21/0036 ,  G02B21/0044 ,  G02B21/16

Abstract: The invention provides an optical stimulation apparatus including a light source (2); a scanning unit (4) that scans light from the light source; and an objective optical system (12) that images the light scanned by the scanning unit onto a specimen (A). The scanning unit (4) includes an acousto-optic device that varies the diffraction angle in response to a vibration frequency input thereto.

Abstract translation: 本发明提供一种包括光源（2）的光学刺激装置; 扫描单元（4），其扫描来自所述光源的光; 以及将由扫描单元扫描的光成像到样本（A）上的物镜光学系统（12）。 扫描单元（4）包括响应于输入的振动频率来改变衍射角的声光装置。

公开(公告)号：EP1352230A2

公开(公告)日：2003-10-15

申请号：EP01994417.2

申请日：2001-12-31

Applicant: Chromagen, Inc.

Inventor： GOULD, Gene ,  CONRAD, Michael, J.

IPC: G01N21/64 ,  G01J3/44 ,  G01J3/12 ,  G01J3/02

CPC classification number: G01N21/6445 ,  G01J3/02 ,  G01J3/0216 ,  G01J3/0224 ,  G01J3/0229 ,  G01J3/0235 ,  G01J3/06 ,  G01J3/12 ,  G01J3/18 ,  G01J3/4406 ,  G01J2003/1217 ,  G01N21/645 ,  G01N21/6452 ,  G01N2021/6417 ,  G01N2021/6421 ,  G01N2021/6463

Abstract: A fluorescence spectrophotometer system may be implemented in scanning fluorescence polarization detection applications. A wavelength and area scanning fluorescence spectrophotometer system may include a light source, an excitation double monochromator, an excitation/emission light transfer module, an emission double monochromator, a high speed timer-counter circuit board, a precision positioning apparatus for positioning a sample relative to the focal plane of the excitation light, and polarizing filters at the excitation side and the emission side. The system may be operative to analyze more than one fluorescent compound in the sample; additionally or alternatively, the system enables analysis of samples from selected ones of a plurality of samples.

公开(公告)号：EP1311189A2

公开(公告)日：2003-05-21

申请号：EP01968013.1

申请日：2001-08-17

Applicant: Euro-Celtique, S.A.

Inventor： CIURCZAK, Emil, W. ,  MARK, Howard ,  BYNUM, Kevin, P.

IPC: A61B5/00

CPC classification number: G01J3/28 ,  A61B5/14532 ,  A61B5/1455 ,  A61B5/1495 ,  G01J3/02 ,  G01J3/0232 ,  G01J3/0235 ,  G01J3/0237 ,  G01J3/0254 ,  G01J3/0289 ,  G01J3/10 ,  G01J3/12 ,  G01J2003/1213 ,  G01J2003/1828 ,  G01J2003/2866 ,  G01N21/359 ,  G01N2201/065

Abstract: An individualized modeling equation for predicting a patient's blood glucose values is generated as a function of non-invasive spectral scans of a body part and an analysis of blood samples from the patient, and is stored on a central computer. The central computer predicts a blood glucose value for the patient as a function of the individualized modeling equation and a non-invasive spectral scan generated by a remote spectral device. If the spectral scan falls within the range of the modeling equation, the predicted blood glucose level is output to the patient. If the spectral scan falls outside the range of the modeling equation, regeneration of the model is required, and the patient takes a number of noninvasive scans and an invasive blood glucose level determination. The computer regenerates the individualized modeling equation as a function of the set of spectral scans and corresponding blood glucose values.

公开(公告)号：EP0631663A1

公开(公告)日：1995-01-04

申请号：EP93906641.0

申请日：1993-03-19

Applicant: RAUTARUUKKI OY

Inventor： KERÄNEN, Heimo ,  PIETARINEN, Pasi ,  ALAJÄRVI, Tapani ,  VÄLI, Veli

IPC: G01J3 ,  G01N21

CPC classification number: G01J3/02 ,  G01J3/021 ,  G01J3/0235 ,  G01J3/0237 ,  G01J3/51 ,  G01J3/513 ,  G01J2003/064 ,  G01N21/314 ,  G01N21/474

Abstract: The invention relates to a method of and a device for measuring optical radiation. In the method, the intensity (2) of a radiation coming from an object (1) to be measured and to be lighted by collimated radiation is measured at several wavelength by focusing the radiation by an optical means (4) and a mirror means (6) on a detector group (3) comprising several detector elements (3a to 3d). The radiation coming from the object (1) to be measured is directed by the optical means (4) and the planar mirror means (6) in such a way that, by rotating the mirror means (6) tilted with respect to its axis (5) round this axis (5) and by keeping the radiation on the surface of the same planar mirror means (6), the focus (F) of radiation is moved in a detector plane (D) along a regular uninterrupted path (R) alternatingly over each detector element (3a to 3d) positioned substantially in the same plane and excited at a different wavelength.