2020
DOI: 10.1103/physreva.102.023712
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Quantum photonics with active feedback loops

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Cited by 9 publications
(11 citation statements)
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“…For the readers' convenience, we briefly recall the model developed in Ref. [30]. It is based on exponential operators of the form Ê(x) = x n = :e (x−1) n: and a two-mode squeezer with a gain γ = cosh 2 |ζ |, where |ζ | is the amplitude of squeezing parameter, being proportional to the square root of the pump power of a single pulse.…”
Section: Appendix A: Lossless Scenariomentioning
confidence: 99%
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“…For the readers' convenience, we briefly recall the model developed in Ref. [30]. It is based on exponential operators of the form Ê(x) = x n = :e (x−1) n: and a two-mode squeezer with a gain γ = cosh 2 |ζ |, where |ζ | is the amplitude of squeezing parameter, being proportional to the square root of the pump power of a single pulse.…”
Section: Appendix A: Lossless Scenariomentioning
confidence: 99%
“…With this approach from Ref. [30], we can model the DH and FH, including imperfections, such as losses, (excess) noise contributions, and the finite detector resolution.…”
Section: Appendix A: Lossless Scenariomentioning
confidence: 99%
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