2020
DOI: 10.1016/j.physleta.2020.126705
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Using coherent feedback loop for high quantum state transfer in optomechanics

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Cited by 14 publications
(3 citation statements)
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“…is the modified cavity decay rate and ∆ f b = ∆ a + 2γ a τ sin β is the effective detuning with ∆ a = ω a − ω 0 are respectively the effective cavity decay rate and the detuning with Here, the quantities ψ, τ denote the transmission and reflection coefficients respectively and β describes the phase shift generated by the reflectivity of the output field on the mirrors [52]. The operator a in f b describes the effective input noise operator in the presence of coherent feedback and corresponding description is based on input-output theory [53].…”
Section: Modelmentioning
confidence: 99%
“…is the modified cavity decay rate and ∆ f b = ∆ a + 2γ a τ sin β is the effective detuning with ∆ a = ω a − ω 0 are respectively the effective cavity decay rate and the detuning with Here, the quantities ψ, τ denote the transmission and reflection coefficients respectively and β describes the phase shift generated by the reflectivity of the output field on the mirrors [52]. The operator a in f b describes the effective input noise operator in the presence of coherent feedback and corresponding description is based on input-output theory [53].…”
Section: Modelmentioning
confidence: 99%
“…To our understanding, measurement feedback control has been studied intensively and well recorded in [5], [202], and [203]. In contrast, coherent feedback control is still a bit new to many researchers in the quantum control community, though it has advantages in many applications [204,1,205,206,207,208,209,210,211,212,213,214,215,25,216,217,218,219,34,9,8,220,221,222,223,224,10,225,50,11,29,30,226,227,228,229,230]. Thus, in this section, we describe briefly linear quantum coherent feedback networks and use a recent experiment as demonstration.…”
Section: Feedback Control Of Quantum Linear Systemsmentioning
confidence: 99%
“…The cavity is also driven by an electromagnetic field through an asymmetric beam splitter (BS) with amplitude ψE . We denote the transmission and reflection coefficients by ψ and τ respectively, and the phase shift generated by the reflectivity of the output field on the mirrors by β [44,59]. The photons and magnons of the cavity are coupled by dipole magnetic interaction, and the magnons and phonons are coupled by magnetostrictive interaction.…”
Section: Introductionmentioning
confidence: 99%