2015
DOI: 10.1364/oe.23.004952
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Experimental generation of 84 dB entangled state with an optical cavity involving a wedged type-II nonlinear crystal

Abstract: Abstract:Entangled state of light is one of the essential quantum resources in quantum information science and technology. Especially, when the fundamental principle experiments have been achieved in labs and the applications of continuous variable quantum information in the real world are considered, it is crucial to design and construct the generation devices of entangled states with high entanglement and compact configuration. We have designed and built an efficient and compact light source of entangled sta… Show more

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Cited by 56 publications
(43 citation statements)
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“…The transmissivities of output coupler at 540 nm and 1080 nm are 0.5% and 12.5%, respectively. In our experiment, all NOPAs are operated at the parametric deamplification situation [62,63]. Under this condition, the coupled modes at +45 • and −45 • polarization directions are thex-squeezed andp-squeezed states, respectively [63].…”
Section: Details Of the Experimental Setupmentioning
confidence: 99%
“…The transmissivities of output coupler at 540 nm and 1080 nm are 0.5% and 12.5%, respectively. In our experiment, all NOPAs are operated at the parametric deamplification situation [62,63]. Under this condition, the coupled modes at +45 • and −45 • polarization directions are thex-squeezed andp-squeezed states, respectively [63].…”
Section: Details Of the Experimental Setupmentioning
confidence: 99%
“…The transmissivities of the front face of KTP crystal at 540 nm and 1080 nm are 21.2% and 0.04%, respectively. The end-face of KTP is cut to 1 • along y-z plane of the crystal and is antireflection coated for both 1080 nm and 540 nm [49]. The transmissivities of output coupler at 540 nm and 1080 nm are 0.5% and 12.5%, respectively.…”
Section: Details Of the Experimentsmentioning
confidence: 99%
“…The standard technique to generate quantum correlated beams and continuous-variable entangled states is by parametric down-conversion in a nonlinear crystal, with an optical parametric oscillator (OPO) or optical parametric amplifier. While very large amounts of quantum noise reduction have been achieved in this way [6,7], the central frequency and linewidth of the generated nonclassical states usually do not naturally match the transitions of matters, such as atoms and solid-state systems, which limits their applications in light-matter interactions.…”
Section: Introductionmentioning
confidence: 99%