Test method and device for rear beam splitting pupil laser differential confocal Brillouin-Raman spectrum
A technology of spectral testing and differential confocal, which is applied in measuring devices, analytical materials, scattering characteristics measurement, etc., can solve problems such as low spatial resolution and large limitations, and improve the spectral signal-to-noise ratio of the system and improve the system The effect of lateral resolution
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Embodiment 1
[0051] like image 3 As shown, a collection pupil 20 is placed on the pupil plane of the collection objective 19. The excitation beam emitted by the light source system 1 passes through the beam splitter prism 2 and the measurement objective lens 3, and then converges on the measured sample 4 to excite the Raman scattered light and Brillouin scattered light carrying the characteristic parameter information of the sample micro-area, and reflect at the same time. Rayleigh scattered light. Raman scattered light, Brillouin and Rayleigh scattered light are collected by the measuring objective lens, and after being reflected by the beam splitting prism 2, they are divided into two beams by the dichroic spectroscopic system 6, and the Rayleigh scattering light reflected by the dichroic spectroscopic system 6 The light and the Brillouin scattered light enter the spectroscopic system 12 , the Rayleigh scattered light and the Brillouin scattered light reflected by the spectroscopic sys...
Embodiment 2
[0060] In this embodiment, the light source system 1 adopts a 532 nm continuous laser, the dichroic spectroscopic system 6 adopts NotchFilter, the Raman spectrum detection unit 11 adopts a Raman spectrometer, and the Brillouin spectrum detection unit 17 adopts a Brillouin spectrometer.
[0061] like Figure 11 As shown, the post-pupil laser differential confocal Brillouin-Raman spectral detection process is as follows:
[0062]First, the laser light emitted from the light source system 1 formed by the laser is condensed by the fifth condensing mirror 30 into the third pinhole 31 , and then collimated and expanded by the sixth condensing mirror 32 to form a parallel excitation beam. After the excitation beam passes through the radial polarization conversion system 27 , the beam splitter prism 2 and the pupil filter 28 , the measured objective lens 3 converges on the measured sample 4 to excite the Raman scattered light carrying the micro-area characteristic parameters of the me...
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