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SHORT-WAVELENGTH LASER CHIRAL RAMAN SPECTROMETER

机译:短波长激光手性拉曼光谱仪

摘要

A short-wavelength laser-excitation chiral Raman Spectrometer (A short-wavelength laser-excitation Raman Optical Activity Spectrometer) comprises a laser-excitation light source between 325nm and 532nm, the linear polarized homogeneous system, circularly polarized light converter, sample cell holder, circularly polarized light splitter, double beam bifurcated optical fiber, Rayleigh line filter, imaging spectrometer, CCD sensitive to short-wavelength range and data processing system. The laser coming from laser-excitation light source goes through the linear polarized homogeneous system then exposures to the sample cell, or the laser coming from laser-excitation light source goes through the linear polarized homogeneous system and circularly polarized light converter then exposures to the sample cell. The left/right circularly polarized Raman signals coming from sample cell go through the Rayleigh line filter, then enter into the incidence end of Y-type double-beam optical fiber, divided into two beams of polarized light via circularly polarized light splitter, present as a linear array on the other end of the optical fiber, then enter into the incident slit of imaging spectrograph. The Raman signals are separated by the imaging spectrograph then enter the CCD on the exit of spectrograph which is sensitive in a wide range of short wavelength, and incident upon the top half and the bottom of it. CCD's acquisition system collects the light signals of the top half and the bottom half, that is, the right and the left ciculaly polarized Raman signals, converting them into electrical signals and transmitting the signals to the computer. After data processing, the sum of right and left circularly polarized Raman signals is counted as the total Raman signal, and the difference between right and left circularly polarized Raman signals as the circularly polarized Raman difference signal, that is, the Raman optical activity signal, and One acquisition when normalized difference of circular polarization intensity is computed as the circularly polarized Raman difference signal divided by the total Raman signal. The short-wavelength chiral Raman Spectrometer that can be applied to confirmation of chiral molecules' and biomolecules' absolute configurations, is a powerful tool for determination of absolute configuration and conformation of chiral molecules in wide region of chemistry, biology and medicine.
机译:短波长激光激发手性拉曼光谱仪(一种短波长激光激发拉曼光学活性光谱仪)包括一个介于325nm和532nm之间的激光激发光源,线性偏振均匀系统,圆偏振光转换器,样品池支架,圆偏振光分束器,双光束分叉光纤,瑞利线滤波器,成像光谱仪,对短波长范围敏感的CCD和数据处理系统。来自激光激发光源的激光穿过线性偏振均质系统然后暴露于样品池,或者来自激光激发光源的激光穿过线性偏振均质系统和圆偏振光转换器然后暴露于样品细胞。来自样品池的左/右圆偏振拉曼信号经过瑞利线滤波器,然后进入Y型双光束光纤的入射端,通过圆偏振分光器分成两束偏振光,以在光纤另一端的线性阵列,然后进入成像光谱仪的入射狭缝。拉曼信号被成像光谱仪分离,然后在光谱仪的出口进入CCD,该光谱仪在很短的波长范围内敏感,并入射到其上半部和下半部。 CCD的采集系统收集上半部分和下半部分的光信号,即左右两极偏振拉曼信号,将它们转换成电信号并将其传输到计算机。经过数据处理后,将左右圆偏振拉曼信号之和计为总拉曼信号,将左右圆偏振拉曼信号之差作为圆偏振拉曼差信号,即拉曼光学活性信号,当圆极化拉曼差信号除以总拉曼信号时,计算圆极化强度的归一化差时的一次采集。短波手性拉曼光谱仪可用于确认手性分子和生物分子的绝对构型,是测定化学,生物学和医学领域中手性分子的绝对构型和构象的有力工具。

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