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Raman scattering light measurement method and Raman scattering light measurement apparatus

机译:拉曼散射光测量方法和拉曼散射光测量设备

摘要

PROBLEM TO BE SOLVED: To measure an intensity of Raman peak with a known distribution wavelength while eliminating fluorescent light without using a spectrometer and with a simple configuration.SOLUTION: A Raman scattered light measuring method uses: wavelength selection means (c1) for irradiating a measuring object 10 with an excitation laser beam having a narrow line width and selecting light in a specific wavelength region from radiation light emitted from the measuring object; and a detector e1 for measuring an intensity of light. The measuring method performs: one measurement of irradiating the measuring object with an excitation laser beam a1 so as to allow the wavelength selection means to select at least a part of a Raman peak r3, and measuring an intensity of light d1 selected by the wavelength selection means with the detector; and other measurement of irradiating the measuring object with an excitation laser beam a2 that is wavelength-shifted from the excitation laser beam at the one measurement so that a selected amount of the Raman peak by the wavelength selection means is different from that at the one measurement and measuring an intensity of light d2 selected by the wavelength selection means with the detector. A difference between measured values obtained at the one measurement and the other measurement is calculated as a Raman peak intensity.
机译:解决的问题:在不使用分光仪且结构简单的情况下消除荧光的情况下测量具有已知分布波长的拉曼峰的强度解决方案:拉曼散射光测量方法使用:波长选择装置(c1)辐照用具有窄线宽的激发激光束从被测物发射的辐射光中选择特定波长区域的光;检测器e1用于测量光强度。所述测量方法执行以下操作:一种测量:用激发激光束a1照射测量对象,以便允许波长选择装置选择拉曼峰r3的至少一部分,并测量通过波长选择而选择的光的强度d1。与检测器一起;以及在另一次测量中,用从一次测量中的激发激光束发生波长偏移的激发激光束a2照射测量对象,以使波长选择装置所选择的拉曼峰的量与一次测量时不同用检测器测量由波长选择装置选择的光的强度d2。计算一次测量和另一次测量获得的测量值之间的差作为拉曼峰强度。

著录项

  • 公开/公告号JP6248666B2

    专利类型

  • 公开/公告日2017-12-20

    原文格式PDF

  • 申请/专利权人 コニカミノルタ株式会社;

    申请/专利号JP20140022136

  • 发明设计人 田尾 祥一;

    申请日2014-02-07

  • 分类号G01N21/65;

  • 国家 JP

  • 入库时间 2022-08-21 13:07:46

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