Super-resolution laser polarization differential confocal imaging method and device
A differential confocal, imaging device technology, applied in the direction of using optical devices, measuring devices, instruments, etc., to achieve the effect of improving signal-to-noise ratio, improving linearity, and improving lateral resolution
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Embodiment 1
[0048] Such as figure 1 , image 3 , Figure 6 , Figure 7 As shown, a pure phase liquid crystal spatial light modulator is used in combination with a λ / 4 wave plate to generate radially polarized light, and combined with a concentric five-ring binary optical element to filter the radially polarized light, the method of the present invention is adopted Perform microscopic imaging with the device.
[0049] Such as figure 1 As shown, the principle of the super-resolution laser polarization differential confocal imaging method is as follows:
[0050] First, the light emitted from the laser 1 is modulated into radially polarized light by the beam expander 2 and the polarization state modulation system 3, and then focused onto the surface of the sample 7 to be measured by the pupil filter 4, the beam splitter 5, and the objective lens 6, and the surface of the sample 7 The reflected light passes through the objective lens 6 and the beam splitter 5 again, and the reflected ligh...
Embodiment 2
[0065] Such as figure 2 and Figure 8 Shown are schematic diagrams of embodiments of a super-resolution laser polarization differential confocal imaging method and device using a confocal system. Example 1 figure 1 and Figure 7 The differential confocal system in 8 is replaced by figure 2 and Figure 8 The confocal system 19 in the confocal system can constitute the super-resolution laser polarization differential confocal imaging method and device embodiment 2 using the confocal system. The difference from Embodiment 1 is that after the light enters the confocal system 19 , it is focused to the pinhole 17 by the lens 16 and detected by the detector 18 . All the other measuring methods and devices are the same as in Example 1.
[0066] Real-time example 3
[0067] Such as Figure 4 and Figure 7 As shown, the embodiment 1 Figure 7 The polarization modulation system in is replaced by Figure 4 The polarization state modulation system in , can constitute embodimen...
Embodiment 4
[0069] Such as Figure 5 and Figure 7 As shown, the embodiment 1 Figure 7 The polarization modulation system in is replaced by Figure 5 The polarization state modulation system in can constitute embodiment 4. The difference from Embodiment 1 is that after the light enters the polarization state modulation system 3, the incident laser beam is modulated into linearly polarized light by the polarization modulator 29, and then incident on the block λ / 2 wave plate spatially varying retarder 30 and modulated into a linearly polarized light beam. The polarized light is focused by the focusing lens 31 to the non-confocal Fabry-Perot interferometer 32 for mode selection and obtains radially polarized light with higher purity, which is collimated by the collimator lens 33 and then exits; block λ / 2 wave plate The spatially variable retarder 30 is spliced and combined by 4 or 8 λ / 2 wave plates with identical optical properties, and the included angles between its fast axis (or slo...
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