2017
DOI: 10.1088/1612-202x/aa7d2f
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Quantum state conversion in opto-electro-mechanical systems via shortcut to adiabaticity

Abstract: Adiabatic process has found many important applications in modern physics, the distinct merit of which is that it does not need accurate control over the timing of the process. However, it is a slow process, which limits the application in quantum computation, due to the limited coherent times of typical quantum systems. Here, we propose a scheme to implement quantum state conversion in opto-electro-mechanical systems via shortcut to adiabaticity, where the process can be greatly speeded up while the precise t… Show more

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Cited by 20 publications
(12 citation statements)
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“…We restrict our state transfer protocol in a single excitation subspace formed by false{false|a1false⟩,false|bfalse⟩,false|a2false⟩false} in low temperatures, where false|a1=false[1,0,0false]T, false|a2=false[0,0,1false]T and false|bfalse⟩=[0,1,0]T represent the states with one excitation of the two optical cavities and the mechanical oscillator, respectively. [ 52,53 ] In this case, the Hamiltonian (3) describes an effective two‐mode system whose dynamics is governed by the Schrödinger equation itfalse|ψ(t)false⟩=trueĤnormalIfalse(tfalse)false|ψ(t)false⟩. The evolution state |ψ(t) can generally be parameterized in the {|c,|b} subspace (where bright state false|cfalse⟩=false(false|a1false⟩+false|a2false⟩false)/2) by two time‐dependent angles α(t) and β(t) as well as a global phase μ(t), given by ref.…”
Section: Photon State Transfer With Stamentioning
confidence: 99%
See 1 more Smart Citation
“…We restrict our state transfer protocol in a single excitation subspace formed by false{false|a1false⟩,false|bfalse⟩,false|a2false⟩false} in low temperatures, where false|a1=false[1,0,0false]T, false|a2=false[0,0,1false]T and false|bfalse⟩=[0,1,0]T represent the states with one excitation of the two optical cavities and the mechanical oscillator, respectively. [ 52,53 ] In this case, the Hamiltonian (3) describes an effective two‐mode system whose dynamics is governed by the Schrödinger equation itfalse|ψ(t)false⟩=trueĤnormalIfalse(tfalse)false|ψ(t)false⟩. The evolution state |ψ(t) can generally be parameterized in the {|c,|b} subspace (where bright state false|cfalse⟩=false(false|a1false⟩+false|a2false⟩false)/2) by two time‐dependent angles α(t) and β(t) as well as a global phase μ(t), given by ref.…”
Section: Photon State Transfer With Stamentioning
confidence: 99%
“…Very recently, the STA approach has been extended to optomechanical systems for fast quantum state conversion. [ 52–56 ] Despite less time and high fidelity features provided in these schemes, control errors in system parameters, which are always inevitable in real experiments, still impose detrimental impacts on robust operations. Fortunately, the combination of STA and optimal control technique (OCT) enables significantly enhanced robustness of population transfer by designing specifically shaped pulses.…”
Section: Introductionmentioning
confidence: 99%
“…To address this concern, we generalize the physical idea of the so-called shortcuts to adiabaticity (STA) [34][35][36][37][38][39][40][41][42][43] method to accelerate the cooling process but keep the merits of the adiabatic passage. The STA method constructs an explicitly auxiliary Hamiltonian Ĥcd (t) to eliminate nonadiabatic transitions and compel the system to follow the eigenstates of Ĥapp (t) [38,39], thus implementing perfect excitation transfer at finite evolution periods [44][45][46]. In particular, the STA method has been experimentally implemented in various platforms [47][48][49][50][51][52][53][54][55][56][57][58][59][60], including nitrogen-vacancy-center systems [47,50,58], trapped ions [48,54], cold-atom systems [49,52], superconducting circuits [51,53,56,57,59], and nuclearmagnetic-resonance systems [55,60].…”
Section: Introductionmentioning
confidence: 99%
“…Some effective protocols for state transfer between optical modes are reported with adiabatic methods [40][41][42], nonadiabatic approaches [42] and shortcuts to adiabaticity technique. [43,44]. By using optomechanical interactions [45][46][47][48][49][50][51][52], the protocols are completed successfully by tuning coupling strengths very well to satisfy technique constraints.…”
Section: Introductionmentioning
confidence: 99%