Single photon detector based on polarization unrelated frequency up-conversion
A single-photon detector and frequency technology, applied in the field of optoelectronics, can solve problems such as polarization sensitivity, and achieve the effect of simple production process and completely polarization-independent effect.
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Embodiment 1
[0035] In order to ensure that the single photon detector works in the communication band, set the signal light wavelength to 1550nm and the light intensity to 0.2MW / cm 2 , the pump light wavelength is 1064nm, and the light intensity is 10MW / cm 2 . According to the quasi-phase matching condition, the reciprocal lattice vector provided by the periodic structure of the first and fourth parts is used to compensate the wave vector mismatch of the frequency up-conversion, setting l A =11.62μm; the reciprocal lattice vector provided by the periodic structure in the second part is used to compensate the wavevector mismatch of the polarization coupling of the signal light, setting l B =20.48μm; the reciprocal lattice vector provided by the periodic structure in the third part is used to compensate the wavevector mismatch of the polarization coupling with frequency light, setting l C = 7.27 μm. To completely convert signal light into sum frequency light, set N A =500, the length of...
Embodiment 2
[0037] In order to ensure that the single photon detector works in the communication band, set the signal light wavelength to 1550nm and the light intensity to 0.2MW / cm 2 , the pump light wavelength is 1064nm, and the light intensity is 10MW / cm 2 . According to the quasi-phase matching condition, the reciprocal lattice vector provided by the periodic structure of the first and fourth parts is used to compensate the wave vector mismatch of the frequency up-conversion, setting l A =11.62μm; the reciprocal lattice vector provided by the periodic structure in the second part is used to compensate the wavevector mismatch of the polarization coupling of the signal light, setting l B =20.48μm; the reciprocal lattice vector provided by the periodic structure in the third part is used to compensate the wavevector mismatch of the polarization coupling with frequency light, setting l C = 7.27 μm. To completely convert signal light into sum frequency light, set N A =500, the length of...
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