2021
DOI: 10.1103/physreva.103.063512
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Quantum squeezing of slow-light solitons

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Cited by 9 publications
(13 citation statements)
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“…Such a correlation between Q1 and P1 leads to a position spreading of the SLDS, contributed by the Kerr nonlinearity (characterized by the nonlinear parameter g). However, photon-number and phase fluctuations are not predicted here, different from the case of bright solitons [66,83,84]. (ii) The quantum fluctuation of the continuum modes (characterized by the quantum number k) has only a simple effect, i.e.…”
Section: Quantum Squeezing Of Slow-light Dark Solitonsmentioning
confidence: 67%
See 2 more Smart Citations
“…Such a correlation between Q1 and P1 leads to a position spreading of the SLDS, contributed by the Kerr nonlinearity (characterized by the nonlinear parameter g). However, photon-number and phase fluctuations are not predicted here, different from the case of bright solitons [66,83,84]. (ii) The quantum fluctuation of the continuum modes (characterized by the quantum number k) has only a simple effect, i.e.…”
Section: Quantum Squeezing Of Slow-light Dark Solitonsmentioning
confidence: 67%
“…Similar to Ref. [66], by employing the perturbation expansion under weak-dispersion and weaknonlinearity approximations, one can obtain the following QNLS equation…”
Section: B Nonlinear Envelope Equation and The Existence Region Of Da...mentioning
confidence: 98%
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“…In recent studies [37,38], it has been shown that light squeezing can be realized in a three-level atomic gas working on the condition of a perturbed electromagnetically induced transparency (EIT) [39]. By introducing a non-zero but small two-photon detuning (which makes the system to deviate strict EIT condition slightly), the system supports giant optical Kerr nonlinearity and displays second-order dispersion effect, thereby allows the formation of (single-component) ultraslow weak-light solitons with very low loss [40,41].…”
Section: Introductionmentioning
confidence: 97%
“…By introducing a non-zero but small two-photon detuning (which makes the system to deviate strict EIT condition slightly), the system supports giant optical Kerr nonlinearity and displays second-order dispersion effect, thereby allows the formation of (single-component) ultraslow weak-light solitons with very low loss [40,41]. Due to the existence of the giant Kerr nonlinearity, the quantum squeezing of the slow-light solitons can be obtained [37,38].…”
Section: Introductionmentioning
confidence: 99%