2023
DOI: 10.1016/j.fmre.2022.07.009
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Phase-controlled photon blockade in optomechanical systems

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Cited by 12 publications
(5 citation statements)
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“…In addition, the coupling coefficient η c is assumed to be a constant, and the specific value η c = 1/2. Using the rotating wave approximation of the system, the full Hamiltonian o system, as shown in Figure 1, can be written as [26,27,32,34] Based on the Hamiltonian in Equation ( 1) and considering the damping of the cavity field and phonon field, the quantum dynamic evolution of the system can be described by the following Heisenberg-Langevin equation [33,35]:…”
Section: Theoretical Model and Equationsmentioning
confidence: 99%
See 1 more Smart Citation
“…In addition, the coupling coefficient η c is assumed to be a constant, and the specific value η c = 1/2. Using the rotating wave approximation of the system, the full Hamiltonian o system, as shown in Figure 1, can be written as [26,27,32,34] Based on the Hamiltonian in Equation ( 1) and considering the damping of the cavity field and phonon field, the quantum dynamic evolution of the system can be described by the following Heisenberg-Langevin equation [33,35]:…”
Section: Theoretical Model and Equationsmentioning
confidence: 99%
“…In recent years, there has been a growing interest in nonlinear optical-mechanical effects within cavity optomechanical systems. By considering the nonlinear interaction term in the dynamic equation of an optical-mechanical system, many interesting phenomena caused by nonlinear optical-mechanical interactions have been revealed, and the scope of cavity optical-mechanical systems has been expanded to topics such as the generation of second-order sidebands [28][29][30], sideband frequency combs [31], optical-mechanical chaos [32], photon-blockade effects [33,34] and carrier-envelope phase correlation effects [35,36]. Among these phenomena, OSS is the first non-linear sideband of the higher-order sidebands, and the generation of high-order sidebands stands out as a characteristic manifestation of nonlinear interactions.…”
Section: Introductionmentioning
confidence: 99%
“…UPB was firstly proposed in a system consisting two coupled quantum boxes in 2010 [30]. Subsequently, many systems were constructed to realize the UPB, such as coupled optomechanical systems [31][32][33], quantum dots coupled to dual-mode optical cavities [34,35], coupled nonlinear resonators [36], rotating cavities in degenerate optical parametric amplifiers [37][38][39].…”
Section: Introductionmentioning
confidence: 99%
“…Recently, much attention has been paid to the study of cavity optomechanical systems with linear coupling [18][19][20][21][22][23], comprising the radiation-induced pressure interaction between light and mechanical motion in the macroscopic scale. These types of systems possess a broad range of important applications, which include the ability to generate different bipartite [24] and tripartite [25] entanglements and sensitive measurements of mechanical motion [26][27][28], photon blockade [29][30][31], phonon blockade [32,33] and optical squeezing, which were investigated from both theoretical and experimental points of view [34][35][36]. An extension of such systems is an optomechanical system with second-order, i.e., quadratic coupling, wherein nonlinear interaction between photons and phonons provides conditions for performing many interesting phenomena, especially squeezing [37][38][39], photon blockade [40][41][42], which was first presented by Rabl et al [43,44], and phonon blockade [45][46][47][48][49].…”
Section: Introductionmentioning
confidence: 99%