A SPECTROMETER AND A METHOD FOR CONTROLLING THE SPECTROMETER
    151.
    发明公开
    A SPECTROMETER AND A METHOD FOR CONTROLLING THE SPECTROMETER 审中-公开
    光谱仪和方法控制光谱仪

    公开(公告)号:EP2106537A1

    公开(公告)日:2009-10-07

    申请号:EP08701723.2

    申请日:2008-01-23

    Inventor: SAARI, Heikki

    CPC classification number: G01J3/10 G01J3/26 G01J3/433 G02B26/001

    Abstract: The invention relates to a spectrometer for material analysis and to a control method for a spectrometer. The spectrometer includes a radiant source (140) formed by multiple single radiation sources (141) having different central wavelengths, for generating a measuring signal, a measurement object (100) containing a material to be analyzed, at least one electrically tunable Fabry-Perot filter (120, 220) for the band pass filtering the measuring signal by at least two pass bands, and a detector (300, 400) for detecting said filtered measuring signals received from the measurement object (100). In accordance with the invention the spectrometer has means (312) for modulating each of the single radiation sources (141) and correspondingly means (307, 309) for demodulating the detected signals such that the signal from each single radiation source can be distinguished from each other in the detector (300, 400), and the spectrometer has means for detecting (300, 400) and demodulating (306, 307) multiple pass bands simultaneously.

    MULTISPECTRAL, MULTIFUSION, LASER-POLARIMETRIC OPTICAL IMAGING SYSTEM
    153.
    发明公开
    MULTISPECTRAL, MULTIFUSION, LASER-POLARIMETRIC OPTICAL IMAGING SYSTEM 审中-公开
    多个频谱,多种融合激光旋光LIGHT图象系统

    公开(公告)号:EP1636556A4

    公开(公告)日:2007-09-12

    申请号:EP04809374

    申请日:2004-05-13

    Applicant: UNIV AKRON

    Inventor: GIAKOS GEORGE C

    Abstract: A multi-energy polarization imaging method consisting of a multi-fusion, dual-rotating retarder / multiple-energy complete Mueller matrix-based polarimeter and dual-energy capabilities The system includes a light source (14) for illuminating a target (18) with a first quantity of light having a first wavelength and a second quantity of light having a second wavelength, the first and second wavelength being different. A polarization-state generator (22) generates a polarization state for each of the first and second quantities of light, and includes a first polarizer (26) through which the first and second quantities of light are transmitted before entering a first waveplate (32). A polarization-state receiver (44) evaluates a resulting polarization state of the first and second quantities of light following illumination of the target (18), the polarization-state receiver (44) including a second waveplate (48) through which the first and second quantities of light are transmitted before entering a second polarizer (51). An optical image-capture device captures a first image of the target illuminated by the first quantity of light and a second image of the target illuminated by the second quantity of light. A processing unit assigns a weighting factor to at least one of the first and second images and evaluates a weighted difference between the first and second images to generate a multi-energy image of the target (18).

    VARIABLE-WAVELENGTH SEMICONDUCTOR LASER AND GAS SENSOR USING SAME
    154.
    发明公开
    VARIABLE-WAVELENGTH SEMICONDUCTOR LASER AND GAS SENSOR USING SAME 审中-公开
    具有可变波长和气体传感器半导体激光器

    公开(公告)号:EP1717918A4

    公开(公告)日:2007-05-16

    申请号:EP05710105

    申请日:2005-02-10

    Applicant: ANRITSU CORP

    Abstract: A variable-wavelength semiconductor laser comprises an n-type semiconductor substrate, an active layer disposed over the n-type semiconductor substrate and capable of generating light, a p-type clad layer disposed over the active layer, and wavelength selection means for selectively oscillating a specific wavelength of the light generated in the active layer. The variable-wavelength semiconductor laser oscillates at the specific wavelength when a current is injected into the active layer, and the specific wavelength can be varied by varying the magnitude of the current. The device length representing the length in the direction of the propagation of the generated light ranges from about 200 to 500 mum, and the width of the active layer representing the length perpendicular to the direction of the propagation of the light and parallel to the substrate ranges from about 1 to 2 mum. The p-type clad layer includes a low-concentration clad sub-layer having a low impurity concentration and a high-concentration clad sub-layer having a high impurity concentration sequentially formed in order from the active layer side.

    Solid state multi frequency fluorometric measurements system and method
    155.
    发明公开
    Solid state multi frequency fluorometric measurements system and method 审中-公开
    Fluormetrische Mehrfrequenz-Festkörpermesssystemeund Verfahren

    公开(公告)号:EP1746411A1

    公开(公告)日:2007-01-24

    申请号:EP06291172.2

    申请日:2006-07-19

    Abstract: A method of spectrographic measurement is disclosed. The method generates light energy using a solid state low capacitance excitation source, the light energy being caused to fall on a sample to be assayed, causing the sample to output an output optical signal. The method generates a plurality of modulation frequencies, and a plurality of heterodyne frequencies to form a set of heterodyne signals at the heterodyne frequencies. Each of the heterodyne frequencies is associated with one of the modulation frequencies. Coupling the modulation frequencies to the excitation source, causes the excitation source to generate excitation energy modulated in intensity in proportion to the modulation frequencies. A sampling a portion of the substantially incoherent excitation energy forms a reference substantially incoherent excitation signal.
    Focusing the output optical signal as an image modulated with the plurality of modulation frequencies on an image intensifier enables the formation of an intensified image modulated with the plurality of modulation frequencies, receiving the intensified image modulated with the plurality of modulation frequencies on a multielement optical detector.

    Abstract translation: 公开了一种光谱测量方法。 该方法使用固态低电容激励源产生光能,使光能落在要测定的样品上,导致样品输出输出光信号。 该方法产生多个调制频率和多个外差频率,以在外差频率上形成一组外差信号。 每个外差频率与调制频率之一相关联。 将调制频率耦合到激励源,使得激发源产生与调制频率成比例的强度调制的激发能。 基本上非相干激发能量的一部分的采样形成参考基本上非相干的激励信号。 将输出光信号聚焦成图像增强器上用多个调制频率调制的图像,能够形成用多个调制频率调制的增强图像,在多元素光学检测器上接收用多个调制频率调制的增强图像 。

    METHOD AND APPARATUS FOR SPECTRUM ANALYSIS AND ENCODER
    156.
    发明授权
    METHOD AND APPARATUS FOR SPECTRUM ANALYSIS AND ENCODER 有权
    方法和设备,频谱CODER

    公开(公告)号:EP1090276B1

    公开(公告)日:2006-05-10

    申请号:EP99931922.1

    申请日:1999-06-25

    Inventor: Hagler, Thomas

    Abstract: A disc serving as a spatial radiation modulator has dispersed radiation filters thereon. Each filter has a transmittance or reflectance modulation function of the form sin (m theta + p pi /4), where m is a positive integer and p has one of the four values 0, 1, 2, 3. A radiation beam including selected wavelength components is diffracted into an elongated image dispersed according to wavelength. Different wavelength components are focused onto different filters on the modulator and are encoded by corresponding filters. Since the modulation functions of the filters are orthogonal to one another, it is possible to extract the amplitude of each wavelength component after it has been encoded or modulated by corresponding filter from the total detected signal during one measurement.

    ACTIVE REMOTE SENSING USING A SPECTRAL LOCK-IN TECHNIQUE
    157.
    发明公开
    ACTIVE REMOTE SENSING USING A SPECTRAL LOCK-IN TECHNIQUE 有权
    ACTIVE远程测量使用光谱EINRASTTECHNIK

    公开(公告)号:EP1618355A2

    公开(公告)日:2006-01-25

    申请号:EP04760102.6

    申请日:2004-04-22

    CPC classification number: G01N21/39 G01J3/433 G01N21/3151 G01N2021/399

    Abstract: A system for sensing a characteristic of a sample may include a tunable source configured to emit optical radiation that varies over a wavelength range at a first frequency and a reference source configured to emit optical radiation that varies in amplitude at a second frequency. A detector may be configured to detect the optical radiation from the tunable source and the reference source after interaction with the sample and generate a science signal. A number of lock-in amplifiers may be respectively configured to generate components of the detected signal that are present at the first and second frequencies. A processor may be configured to determine a characteristic of the sample based on the components of the detected signal that are present at the first and second frequencies.

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