2023
DOI: 10.1103/prxquantum.4.040310
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Experimental Optical Simulator of Reconfigurable and Complex Quantum Environment

P. Renault,
J. Nokkala,
G. Roeland
et al.
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Cited by 5 publications
(2 citation statements)
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“…where i = √ −1, a j and a † j are the annihilation and creation operators, respectively, indexed by mode and satisfying the commutator relation [a j , a † l ] = δ jl . The reservoir is a complex network [47,48] with (real) couplings g jl and h jl . Following [41] they are random numbers uniformly distributed as g jl ∈ [0.1, 0.3] and h jl ∈ [0.2, 0.4], scaled with the modes frequencies (ω j = 1); these parameters are consistent with squeezing levels of state-of-the-art experiments.…”
Section: Methodsmentioning
confidence: 99%
“…where i = √ −1, a j and a † j are the annihilation and creation operators, respectively, indexed by mode and satisfying the commutator relation [a j , a † l ] = δ jl . The reservoir is a complex network [47,48] with (real) couplings g jl and h jl . Following [41] they are random numbers uniformly distributed as g jl ∈ [0.1, 0.3] and h jl ∈ [0.2, 0.4], scaled with the modes frequencies (ω j = 1); these parameters are consistent with squeezing levels of state-of-the-art experiments.…”
Section: Methodsmentioning
confidence: 99%
“…The problem of experimental realization of random quantum harmonic oscillator networks has been recently solved in a multimode quantum optics platform [192], where a shaped pulse train pumps an optical parametric process, creating squeezed modes, which can then be measured in a suitable basis to complete the mapping of the network dynamics to that of the optical modes. This has already been used to experimentally realize non-Markovian open system dynamics [193,194].…”
Section: Structured Environments and Probingmentioning
confidence: 99%