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Stimulated Raman scattering imaging for studying specific species

机译:受激拉曼散射成像用于研究特定物种

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The stimulated Raman scattering (SRS) signal in diffuse light has been recorded using an optical imaging technique based on spatial modulation. A frequency doubled Q-switched Nd-YAG laser (wavelength 532 nm) has been used to pump a polymethyl methacrylate (PMMA) cylinder. The frequency tripled (355 nm) beam from the same laser is used to pump an optical parametric oscillator (OPO). The Stokes beam (from the OPO) has been tuned to 631.27 nm so that the frequency difference between the pump and the Stokes beams fits a Raman active vibrational mode of the PMMA molecule (2956 cm~(-1)). The two laser beams were overlapped in time and space on a PMMA cylinder resulting in a gain of the Stokes beam through the SRS process of about 4.0 %. For separating the SRS signal, the pump beam was spatially modulated with fringes produced in a Michelson interferometer. The gain of the Stokes beam due to SRS was separated from the Stokes beam background in the Fourier domain. The intensity image has been calculated from an inverse Fourier transform of the separated gain signal. The intensity image shows a gain of the Stokes beam at the area of overlap between the pump beam fringes and the Stokes beam compared to the undisturbed surrounding. The results show that spatial modulation of the pump beam is a promising method to separate the weak SRS signal from the Stokes beam background. This technique can be applied to pin-point specific species and record its spatial and temporal distribution.
机译:已经使用基于空间调制的光学成像技术记录了散射光中的受激拉曼散射(SRS)信号。倍频调Q的Nd-YAG激光(波长532 nm)已用于泵浦聚甲基丙烯酸甲酯(PMMA)圆柱体。来自同一激光器的三倍频(355 nm)光束用于泵浦光学参量振荡器(OPO)。 Stokes光束(来自OPO)已调至631.27 nm,以使泵浦和Stokes光束之间的频率差适合PMMA分子的拉曼主动振动模式(2956 cm〜(-1))。两条激光束在时间和空间上在PMMA圆柱体上重叠,从而通过SRS过程获得的斯托克斯束增益约为4.0%。为了分离SRS信号,泵浦光束通过在迈克尔逊干涉仪中产生的条纹在空间上进行了调制。 SRS引起的斯托克斯束增益在傅立叶域中与斯托克斯束背景分离。从分离的增益信号的傅立叶逆变换中计算出强度图像。强度图像显示了与未受干扰的周围环境相比,斯托克斯束在泵浦光束条纹和斯托克斯束之间的重叠区域处的增益。结果表明,抽运光束的空间调制是一种将较弱的SRS信号与斯托克斯光束背景分开的有前途的方法。该技术可用于查明特定物种并记录其空间和时间分布。

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