A reference beam splitting method and special device for space angle division multiplexing holography based on Wollaston prism
A Wollaston prism and special device technology, applied in optics, optical components, instruments, etc., can solve problems such as complex adjustment mechanism, insufficient utilization of space bandwidth of recording devices, unreasonable spatial distribution of reference light, etc., and achieve stability Improve and adjust the effect of step simplification
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Embodiment 1
[0035] See attached figure 1 , the present invention is based on the special device of the reference beam splitting method of the space angle division multiplexing holography of the Wollaston prism comprising:
[0036] Two sets of delay lines; two depolarized light-splitting flat films; two sets of double-lens converging systems; two Wollaston prisms, the surfaces of the Wollaston prisms are all coated with anti-reflection coatings; wherein,
[0037] The first depolarized beam splitter 1 (BS 1 ), which is used to split the ultrashort laser double pulse of the circular polarization state into pulses emitted in two directions;
[0038]The first delay line structure 2 (DL 1 ), located in the first depolarized beam splitter plate 1 (BS 1 ) on the reflected light path, used to adjust the optical path of the reflected light path, so as to adjust the pulse interval of two pairs of double pulses;
[0039] Located in the first delay line structure 2 (DL 1 The rotatable Wollaston p...
Embodiment 2
[0045] combined with figure 1 , the present invention is based on the reference beam splitting method of the spatial angle division multiplexing holography of the Wollaston prism:
[0046] 1. The pulsed laser is incident on the first depolarized beam splitter 1 (BS 1 ) for beam splitting;
[0047] 2. In the first depolarized beam splitter 1 (BS 1 ) The reflected light beam is incident on the first delay line structure 2 (DL 1 ) and the second delay line structure 3 (DL 2 );
[0048] 3. The beam passing through the two delay lines passes through the second depolarized beam splitter 4 (BS 2 ) on the bundle;
[0049] 4. In the second depolarized beam splitter 4 (BS 2 ) with two mirrors and depolarization beam combiner 11 (BS 3 ) to form a Mach-Zendr interference system, in which the depolarization beam combiner 11 (BS 3 ) position and angle, so that the two beams of light are combined on the CCD target surface at an angle of θ, where θ is the beam splitting angle of the ...
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