High-order quasi-phase matching cross-correlation-based single signal-to-noise ratio measurement method and device thereof
A single-measurement, cross-correlation technique applied in the laser field to achieve high-resolution results
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Embodiment 1
[0027] figure 1 (a) A novel crystal design based on high-order quasi-phase matching (QPM), on a large lithium niobate substrate (length L 1 +L 2 ) only polarizes part of it (length L 1 ), the rest is not polarized (length L 2 ). The period of the polarization region is Λ, and the corresponding lattice vector is , m is an odd number ≥3.
[0028] Taking the measurement of 1054nm neodymium glass laser as an example, the sampling light is its frequency doubled light of 527nm. The 1054nm laser light 1 emitted by the neodymium glass laser is split into two beams by the beam splitter 2 . One beam, as the beam 3 to be measured, passes through the periscope 10 in order to be polarized, the second reflector 11, the third reflector 12, and the first beam expander 13 (expanding the beam to be equivalent to the width of the crystal), and vertically by the cylindrical concave mirror 14 Focus directly onto the 25-wide end facet of the crystal. Another bundle of 4 pump frequency mult...
Embodiment 2
[0031] figure 1 (b) is another novel configuration based on higher-order QPM. Taking the measurement of 800nm Ti:sapphire laser as an example, using 3.4μm long-wavelength sampling light, the corresponding prototype experimental device is as follows: 800nm laser 1 emitted by Ti:sapphire laser is divided into two beams by beam splitter 2. One beam, as the beam 3 to be measured, passes through the periscope 10 in order to be polarized, the second reflector 11, the third reflector 12, and the first beam expander 13 (expanding the beam to be equivalent to the width of the crystal), and vertically by the cylindrical concave mirror 14 Focus directly onto the 25-wide end facet of the crystal. Another beam of 4 pumps mid-infrared light parametric amplifier 5 to generate 3.4 μm long-wavelength sampling light 6 , passes through first mirror 7 and time delay line 8 , and is focused by concave mirror 9 onto the narrow end surface of crystal 15 . The sum-frequency cross-correlation be...
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