2017
DOI: 10.1088/1612-202x/aa5adb
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Three-color entanglement generated by single-pass cascaded sum-frequency processes

Abstract: Three-color continuous-variable (CV) entangled beams can be produced by single-pass cascaded sum-frequency processes of third-harmonic generation by quasi-phase-matching technique in only one optical superlattice. Firstly, second-harmonic field is generated by the first double-frequency process of the fundamental field. Then, the third-harmonic field can be generated by the second cascaded sum-frequency process between the second-harmonic and the fundamental fields by quasi-phase-matching technique in the same… Show more

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Cited by 12 publications
(18 citation statements)
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“…1, for κ 1 = 10 −2 , κ 2 = 1.5κ 1 , and N 0 (0) = 10 4 . We note here that these solutions are not consistent with those given by Yu et al [28], which reach a steady state at ξ ≈ 6, after which the modes at ω 0 and ω 2 are totally depleted, leaving only the second harmonic. As we know that the term κ 1â1â † 2 0 in the Hamiltonian will act to down convert the second harmonic with no other modes present, and this is in fact what is responsible for the revivals of the fundamental seen in traveling-wave SHG [39], we have confidence in our solutions.…”
Section: B Cascaded Third-harmonic Generationcontrasting
confidence: 91%
See 3 more Smart Citations
“…1, for κ 1 = 10 −2 , κ 2 = 1.5κ 1 , and N 0 (0) = 10 4 . We note here that these solutions are not consistent with those given by Yu et al [28], which reach a steady state at ξ ≈ 6, after which the modes at ω 0 and ω 2 are totally depleted, leaving only the second harmonic. As we know that the term κ 1â1â † 2 0 in the Hamiltonian will act to down convert the second harmonic with no other modes present, and this is in fact what is responsible for the revivals of the fundamental seen in traveling-wave SHG [39], we have confidence in our solutions.…”
Section: B Cascaded Third-harmonic Generationcontrasting
confidence: 91%
“…Also, is the coherent pump amplitude, γ j is the cavity loss rate for mode j , and the η j are Gaussian random variables with the correlations η j (t) = 0 and η j (t)η k (t ) = δ jk δ(t − t ). Note that our noise terms are not exactly the same as those in Yu et al [27][28][29] and that this is due to the freedom available in the factorization of the diffusion matrix of the Fokker-Planck equation for the positive-P function of the system. We have chosen to use real rather than complex noise terms, which is a matter of taste since exactly the same physical system can be represented by either.…”
Section: B Cascaded Third-harmonic Generationmentioning
confidence: 97%
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“…Various entangled states, including two-color [19][20][21][22][23][24][25] and three-color [26][27][28] CV quantum-entangled states, have been generated. We have utilized a single ring resonator, which combines both the NOPA and non-degenerate optical parametric oscillator (NOPO), and prepared quantum-entangled states with a large wavelength difference.…”
Section: Introductionmentioning
confidence: 99%