Laser stimulated emission depletion (STED) and three-dimensional superresolving spectral pupil differential confocal imaging method and device
A laser stimulated emission, differential confocal technology, applied in the direction of using optical devices, measuring devices, instruments, etc., can solve problems such as limited applications
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Embodiment 1
[0046] Such as figure 1 As shown, the laser stimulated emission loss microscopic three-dimensional super-resolution split pupil differential confocal imaging method, the test steps are as follows:
[0047] First, the wavelength emitted from the excitation laser system 1 is λ 1 After being reflected by the first dichroic mirror 2, the parallel light beam passes through the second dichroic mirror 17, the quarter wave plate 3 and the illumination pupil 5, and is focused on the surface of the measured sample 7 by the measuring objective lens 4, and the measured sample 7 reflects The light with sample information (or excited fluorescence) passes through the collection pupil 6 of the measurement objective 4, the quarter wave plate 3, the second dichroic mirror 17 and the first dichroic mirror 2, and enters the split pupil differential common Focus detection system 9; Confocal lens 10 and image acquisition system 11 are placed successively in the sub-pupil differential confocal dete...
Embodiment 2
[0053] Such as figure 2 As shown, replacing the beam shaping system 16 in Embodiment 1 with the annular beam shaping system 20 can constitute a stimulated emission loss split pupil three-dimensional super-resolution differential confocal imaging method and device using the annular beam shaping system, and the annular beam shaping system The system 20 can be an annular pupil filter, a binary optical diffraction device with an annular phase distribution, etc., and shapes the quenched laser beam into an annular beam 21 .
[0054] figure 2 Among them, the illumination pupil can be a circular pupil, a D-shaped pupil or a pupil of other shapes; it can also be a ring pupil, which directly replaces the ring beam shaping system and shapes the incident beam into a ring beam.
[0055] All the other measuring methods are the same as in Example 1.
Embodiment 3
[0057] Such as image 3 As shown, a schematic diagram of an embodiment of a laser stimulated emission loss three-dimensional super-resolution split-pupil differential confocal imaging device, the principle of which is:
[0058] First, the sample 7 to be tested is placed on the scanning table 23. The scanning table 23 adopts a macro-micro combination method, and a micro-displacement two-dimensional table based on a piezoelectric ceramic driver PZT and a capacitive sensor is integrated on the x-y macro table. , start the measurement software in the main control computer 24.
[0059] The parallel light beam emitted by the excitation laser system 1 is reflected by the first dichroic mirror 2, passes through the second dichroic mirror 17, the quarter-wave plate 3 and the illumination pupil 5, and is focused on the measured sample 7 by the measuring objective lens 4. The light with sample information (or excited fluorescence) reflected by the sample 7 passes through the collection ...
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