All-fiber bright compressed state light source based on optical parametric down-conversion
A technology of optical parameters and squeezed states, which is applied in the fields of quantum optics and quantum information, can solve the problems of low nonlinear conversion efficiency and compression, and achieve high nonlinear conversion efficiency, avoid mode matching problems, and high compression
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Embodiment 1
[0038] Such as figure 1 As shown, it is a schematic structural diagram of an all-fiber bright squeezed light source based on optical parameter down-conversion in the present invention, including a laser, an isolator, a beam splitter, a frequency doubling medium, a wavelength division multiplexer, and a phase modulator. phase modulator two, beam combiner, circulator, incident grating one, outgoing grating two and optical parametric down conversion medium.
[0039] The laser is a single-frequency fiber laser or a single-frequency semiconductor laser, which is used to output a laser beam in a linearly polarized manner. Preferably, a low-noise single-frequency laser is used. The lower the noise of the laser, the better the output effect. In this embodiment, a 1064nm low-noise single-frequency laser is used.
[0040] The isolator is a fiber-optic isolation device with one-way passage of the beam, connected to the output end of the laser, and used to prevent the laser beam reflect...
Embodiment 2
[0053] Such as figure 2 As shown, it is a schematic structural diagram of an all-fiber bright squeezed light source based on optical parameter down-conversion in the second embodiment of the present invention, including a laser, an isolator, a beam splitter, a circulator, a frequency doubling medium, a phase modulator, and a phase modulation Two, three phase modulators, beam combiner, two circulators, one incident grating, two exit gratings, three incident gratings, four exit gratings and an optical parameter down conversion medium.
[0054] Different from the technical solution of the implementation case 1, the same resonant cavity structure is added for the frequency doubling process in the implementation case 2, which can obtain more usable pump light by improving the frequency doubling efficiency when the output power of the laser is limited.
[0055] In this embodiment, the laser emits 1550nm low-noise single-frequency laser, and enters the beam splitter after passing th...
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