RADIATION RESISTANT SPECTORMETER INTERFACE
    11.
    发明公开
    RADIATION RESISTANT SPECTORMETER INTERFACE 审中-公开
    STRAHLUNGSRESISTENTE SPEKTROMETERSCHNITTSTELLE

    公开(公告)号:EP2470872A4

    公开(公告)日:2017-06-14

    申请号:EP10827305

    申请日:2010-09-17

    Abstract: Devices, systems, and methods for measuring tissue oxygen saturation are disclosed. An illustrative spectrometer for interfacing an optical sensor with a display unit includes a number of measurement radiation sources, a number of radiation source fibers each optically coupled to one of the measurement radiation sources, a reflected radiation fiber optically coupled to the optical sensor, a measurement radiation output fiber including an image fiber, and a radiation mixing bar intermediate the radiation source fibers and the measurement radiation output fiber.

    Abstract translation: 公开了用于测量组织氧饱和度的装置,系统和方法。 用于将光学传感器与显示单元接口连接的示例性光谱仪包括多个测量辐射源,多个辐射源光纤,每个光源耦合到测量辐射源中的一个,光学耦合到光学传感器的反射辐射光纤,测量 包括图像光纤的辐射输出光纤以及辐射源光纤和测量辐射输出光纤中间的辐射混合棒。

    A METHOD FOR DETERMINING THE SPECTRAL SCALE OF A SPECTROMETER AND APPARATUS
    12.
    发明公开
    A METHOD FOR DETERMINING THE SPECTRAL SCALE OF A SPECTROMETER AND APPARATUS 审中-公开
    方法用于频谱光谱仪和设备的确定比额表

    公开(公告)号:EP3161436A1

    公开(公告)日:2017-05-03

    申请号:EP15811041.1

    申请日:2015-06-29

    Abstract: A method for determining spectral calibration data (λcal(Sd), Sd,cal(λ)) of a Fabry-Perot interferometer (100) comprises: - forming a plurality of filtered spectral peaks (P'1, P'2) by filtering input light (LB1) with a Fabry-Perot etalon (50) such that a first filtered peak (Ρ'1) corresponds to a first transmittance peak (P1) of the etalon (50), and such that a second filtered peak (P'2) corresponds to a second transmittance peak (P2) of the etalon (50), - using the Fabry-Perot interferometer (100) for measuring a spectral intensity distribution (M(Sd)) of the filtered spectral peaks (Ρ'1, P'2), wherein the spectral intensity distribution (M(Sd)) is measured by varying the mirror gap (dFP) of the Fabry-Perot interferometer (100), and by providing a control signal (Sd) indicative of the mirror gap (dFP), and - determining the spectral calibration data (λcal(Sd), Sd,cal(λ)) by matching the measured spectral intensity distribution (M(Sd)) with the spectral transmittance (ΤΕ(λ)) of the etalon (50).

    Abstract translation: 一种用于确定性采矿光谱校准数据的方法(λcal(SD),SD,CAL(λ))法布里 - 珀罗干涉仪(100)的步骤包括: - 通过过滤形成过滤谱峰的多个(P'1,P'2) 输入光(LB1)配有一个法布里 - 珀罗标准具(50)检测做了第一滤波峰(Ρ'1)对应于标准具(50)的第一透射率峰(P1),并且这样做了第二经滤波的峰值(P “2)对应于第二峰的透射率(标准具的P2)(50), - 使用用于测量的光谱强度分布(M(SD法布里 - 珀罗干涉仪(100))的滤波谱峰)(Ρ'1 ,P'2)worin光谱强度分布(M(SD))通过改变法布里 - 珀罗干涉仪(100)的镜间隙(DFP)测量,并且通过提供控制信号(SD)表示反射镜的 间隙(DFP),以及 - 确定性采矿光谱校正数据(λcal(SD),SD,CAL(λ))通过匹配所测量的光谱强度分布(M(SD))与光谱透射率(ΤΕ(λ)) 的标准具(50)。

    OPTIMISATION OF THE LASER OPERATING POINT IN A LASER ABSORPTION SPECTROMETER
    14.
    发明公开
    OPTIMISATION OF THE LASER OPERATING POINT IN A LASER ABSORPTION SPECTROMETER 审中-公开
    EINEM LASERABSORPTIONSPEKTROMETER中的OPTIMIERUNG DES LASERARBEITSPUNKTES

    公开(公告)号:EP3139456A1

    公开(公告)日:2017-03-08

    申请号:EP16186892.2

    申请日:2016-09-01

    Abstract: An operating value of a first laser parameter of a laser device in a laser absorption spectrometer is optimised. The wavelength of laser device emitted light is adjusted by the first or a second laser parameter. The laser absorption spectrometer comprises a light intensity detector measuring the laser light intensity from the laser device. For each of multiple values of the first laser parameter: the light intensity detector measures light intensity obtained across a range of second laser parameter values, and an extremum in the light intensity measure and a peak position for the extremum are identified. A range of first laser parameter values is identified within the values of the first laser parameter for which there is a continuous trend in changes to the identified peak position with changes to the first laser parameter. The first laser parameter operating value is set to be within the identified range.
    The laser device is either a mid-infrared LD or the difference frequency generated in a PPNL (250) using the output of two near infrared telecommunication laser diodes (210,220) having for example a DFB (220). The wavelength sweep is realized by a corresponding control of temperature and bias current provided to the LD while the absorption peaks of the isotopes to be detected should be in the middle of the individual sweep ranges.

    Abstract translation: 激光吸收光谱仪中的激光装置的第一激光参数的操作值被优化。 通过第一或第二激光参数来调节激光器发射光的波长。 激光吸收光谱仪包括测量来自激光装置的激光强度的光强度检测器。 对于第一激光参数的多个值中的每一个,光强度检测器测量在第二激光参数值的范围内获得的光强度,并且确定光强测量中的极值和极值的峰值位置。 在第一激光参数的值内识别出一系列第一激光参数值,在第一激光参数的值中,随着对第一激光参数的改变,对所识别的峰位置的变化存在连续趋势。 第一激光参数工作值设定在识别范围内。 使用具有例如DFB(220)的两个近红外通信激光二极管(210,220)的输出,激光装置是中红外LD或PPNL(250)中产生的差频。 波长扫描通过对LD提供的温度和偏置电流的相应控制来实现,而待检测的同位素的吸收峰应在各个扫描范围的中间。

    QUANTUM METER
    17.
    发明公开
    QUANTUM METER 审中-公开
    QUANTENMESSVORRICHTUNG

    公开(公告)号:EP2995915A1

    公开(公告)日:2016-03-16

    申请号:EP14794594.3

    申请日:2014-05-07

    CPC classification number: G01J3/0264 A01G7/045 G01J3/027 G01J3/0294 Y02P60/146

    Abstract: [Problem] A practicable quantum meter capable of knowing the photosynthetic photon flux density at each wavelength in real time is presented.
    [Solution] Measurement light made incident on a dispersive element 12 by an incident optical system 13 in a spectroscope unit 1 is dispersed by the dispersive element 12, and converted to photoelectric signal on the detector 14. Each photoelectric signal at each wavelength (spectral data) is transmitted to the processing unit 2, which is a general use computer, via interface members 16 and 26. The processing unit 2, to which a photosynthetic photon flux density measurement program 4 and a special device driver 262 have been installed, calculates the distribution of the photosynthetic photon flux density at each wavelength by processing the received spectral data, and displays it on display 24.

    Abstract translation: [问题]提出了一种能够实时了解每个波长的光合光子通量密度的实用量子计。 [解决方案]通过分光单元1中的入射光学系统13入射在分散元件12上的测量光被分散元件12分散,并在检测器14上转换为光电信号。每个波长的每个光电信号(光谱数据 )经由接口部件16和26被发送到作为一般使用的计算机的处理单元2.已经安装了光合光子通量密度测量程序4和专用设备驱动器262的处理单元2计算出 通过处理所接收的光谱数据分布各波长的光合光子通量密度,并将其显示在显示器24上。

    FOURIER TRANSFORM INFRARED SPECTROMETER
    19.
    发明公开
    FOURIER TRANSFORM INFRARED SPECTROMETER 审中-公开
    傅立叶变换红外光谱仪

    公开(公告)号:EP2963400A1

    公开(公告)日:2016-01-06

    申请号:EP13876680.3

    申请日:2013-02-28

    Inventor: FUKUDA, Hisato

    Abstract: A Fourier transform infrared spectrophotometer that is free from an effect of interference condition change resulting from an accessory being mounted and has a high measurement accuracy is provided. A Fourier transform infrared spectrophotometer according to the present invention is a Fourier transform infrared spectrophotometer including a common base on which a sample chamber 2 and an interference optical system are mounted, where an accessory 20 can be detachably in the sample chamber, the Fourier transform infrared spectrophotometer including: accessory information reading means 22 for reading accessory information provided to the accessory 20 when the accessory 20 is mounted in the sample chamber 2; and setting condition changing means (controller 30) for changing a setting condition for the interference optical system based on the accessory information read by the accessory information reading means 22, the setting condition varying depending on, e.g., a difference in weight between respective accessories 20.

    Abstract translation: 本发明提供一种傅里叶变换红外分光光度计,其不会由于安装附件而导致干涉条件变化的影响,并且具有高测量精度。 根据本发明的傅里叶变换红外分光光度计是傅里叶变换红外分光光度计,其包括其上安装有样品室2和干涉光学系统的共同基座,其中附件20可以可拆卸地安装在样品室中,傅里叶变换红外 分光光度计,包括:附件信息读取装置22,用于读取当附件20安装在样品室2中时提供给附件20的附件信息; 以及根据附件信息读取装置22读取的附件信息改变干涉光学系统的设置条件的设置条件改变装置(控制器30),该设置条件根据例如各个附件20之间的重量差而变化 。

    GAS ABSORPTION SPECTROSCOPY DEVICE AND GAS ABSORPTION SPECTROSCOPY METHOD
    20.
    发明公开
    GAS ABSORPTION SPECTROSCOPY DEVICE AND GAS ABSORPTION SPECTROSCOPY METHOD 有权
    GASABSORPTIONSSPEKTROSKOPIESYSTEM UND GASABSORPTIONSSPEKTROSKOPIEVERFAHREN

    公开(公告)号:EP2942616A1

    公开(公告)日:2015-11-11

    申请号:EP13869899.8

    申请日:2013-12-25

    Abstract: Provided is a gas absorption spectroscopic system and gas absorption spectroscopic method capable of accurately measuring the concentration or other properties of gas even in high-speed measurements. Laser light with a varying wavelength is cast into target gas. A spectrum profile representing a change in the intensity of the laser light transmitted through the target gas with respect to wavelength is determined. For this spectrum profile, polynomial approximation is performed at each wavelength point within a predetermined wavelength width, using an approximate polynomial. Based on the coefficients of the terms in the approximate polynomial at each point, an nth order derivative curve, where n is an integer of zero or larger, of the spectrum profile is created. A physical quantity of the target gas is determined based on the thus created nth order derivative curve.

    Abstract translation: 提供了即使在高速测量中也能够精确地测量气体的浓度或其它性质的气体吸收光谱系统和气体吸收光谱法。 具有不同波长的激光被投射到目标气体中。 确定表示相对于波长透过目标气体的激光的强度变化的光谱分布。 对于该频谱分布,使用近似多项式在预定波长宽度内的每个波长点处执行多项式近似。 基于每个点处的近似多项式中的项的系数,产生频谱分布中n为零或更大的整数的n阶微分曲线。 基于由此产生的n阶导数曲线确定目标气体的物理量。

Patent Agency Ranking