Method and device of dual-color single photon transverse super resolution imaging
A technology of super-resolution imaging and imaging device, which is applied in measurement devices, material analysis by optical means, and material analysis, etc., can solve problems such as expensive equipment and complicated processes, and achieve the effect of convenient operation and high fluorescence excitation efficiency.
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Embodiment 2
[0049] Optical path diagram such as figure 1 As shown, the sensitizing pupil 7 and the excitation pupil 12 are not added in the optical path, and the excitation dichroic mirror 13 is adjusted in the x-axis direction so that the two beams of light propagate in parallel and non-coaxially, but the two beams of light spot spread after being focused by the objective lens 3 The function center is at a distance of L=220nm in the x-axis. At this time, the fluorescence excitation of the reversible photosensitive fluorescent protein can only be realized in the overlapping region of the edge of the airy spot of the sensitizing light and the excitation light, and other non-overlapping regions cannot meet the fluorescence excitation conditions of the reversible photosensitive fluorescent protein without emitting fluorescence. The equivalent point spread function is as Figure 6 As shown, the x-axis full width at half maximum is 79nm, and the resolution in the x direction is increased by 2...
Embodiment 3
[0051] Optical path diagram such as figure 1 As shown, a sensitization pupil 7 and an excitation pupil 12 are added to the optical path, and the sensitization pupil 7 and the excitation pupil 12 are three-zone phase pupil filters, with three zones A, B, and C from inside to outside The phases are 0, π, 0 in sequence, and the normalized radius is 0.12:0.6:1 in sequence. The addition of the pupil changes the distribution of the original point spread function and enhances the maximum peak of the third-order diffraction. By adjusting the excitation dichroic mirror 13 in the x-axis direction, the two beams of light propagate in parallel and non-coaxially, and after being focused by the objective lens 3, the x-axis distance of the center of the point spread function of the two beams of light is L=1010 nm. At this time, the fluorescence excitation of the reversible photosensitive fluorescent protein can only be realized in the overlapping area of the focus edge of the third-order ...
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