Laser differential confocal LIBS, Raman spectrum-mass spectrum imaging method and Raman spectrum-mass spectrum imaging device
A differential confocal and Raman spectroscopy technology, applied in measurement devices, Raman scattering, material excitation analysis, etc., can solve problems such as drift, low spatial resolution of mass spectrometry detection, and restricting the accurate and complete acquisition of sample component information. , to achieve the effect of compressing size and improving spatial resolution
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Embodiment 1
[0053] The embodiment of the present invention is based on Figure 4 The shown high spatial resolution laser differential confocal spectrum-mass spectrometer imaging device includes a laser point light source system 24, a collimator lens 25 placed along the optical axis, an outgoing beam attenuator 38, a ring light generation system 3, and a beam splitter The mirror 5, the center hole beam splitter 6 and the center hole measurement objective lens 7 which is located in the refraction direction of the optical axis and focuses the light beam reflected by the center hole color splitter 6 to the measured sample 8, including the focused light spot reflection light of the center hole measurement objective lens 7 The intensity signal is a differential confocal light intensity detection system composed of a dichroic beam splitter 40, a detection beam attenuator 39, and a differential confocal light intensity detector 2, which is used to detect the Raman spectrum 43 excited by the focuse...
Embodiment 2
[0076] like Figure 5 As shown, in the high spatial resolution laser differential confocal induced breakdown and Raman spectrum-mass spectrometer imaging device of embodiment 1, the ring light generation system 3 can be generated by a vector beam placed along the optical axis to generate a vector beam The system 21 and the pupil filter 22 are replaced to generate an annular light beam 23 , which is reflected by the center hole color separator 6 and focused by the center hole measurement objective lens 7 to irradiate the measured sample 8 with a tiny spot exceeding the diffraction limit.
[0077] The remaining imaging measurement methods are the same as in Example 1.
Embodiment 3
[0079] like Figure 5 As shown, in the high spatial resolution laser differential confocal induced breakdown and Raman spectrum-mass spectrometer imaging device of Embodiment 1, the computer 10 can control the two-dimensional scanning galvanometer system 37 to align the middle hole measurement objective lens 7 The next area to be tested of the sample 8 to be tested.
[0080] The remaining imaging measurement methods are the same as in Example 1.
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