2021
DOI: 10.1103/physrevb.104.235408
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Non-Hermitian spectrum and multistability in exciton-polariton condensates

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Cited by 13 publications
(7 citation statements)
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“…We consider an exciton-polariton BEC under nonresonant pumping, created in a wire-shaped microcavity [34] that bounds the polaritons to a quasi-onedimensional (1D) channel. In the mean field theory, the time evolution of the polariton field, described by the condensate order parameter ψ(x, t), is governed by an effectively 1D driven-dissipative GPE, coupled to a rate equation for the density n R (x, t) of reservoir polaritons [23,[35][36][37][38],…”
Section: The Theoretical Model and Lagrangian Approachmentioning
confidence: 99%
“…We consider an exciton-polariton BEC under nonresonant pumping, created in a wire-shaped microcavity [34] that bounds the polaritons to a quasi-onedimensional (1D) channel. In the mean field theory, the time evolution of the polariton field, described by the condensate order parameter ψ(x, t), is governed by an effectively 1D driven-dissipative GPE, coupled to a rate equation for the density n R (x, t) of reservoir polaritons [23,[35][36][37][38],…”
Section: The Theoretical Model and Lagrangian Approachmentioning
confidence: 99%
“…We consider an exciton–polariton BEC under nonresonant pumping, which is created in a wire-shaped microcavity [ 38 ] that bounds the polaritons to a quasi-one-dimensional (1D) channel. In the mean field theory, the time evolution of the polariton field is governed by an effectively 1D driven-dissipative GPE for the condensate order parameter , which is coupled to a rate equation for the density of reservoir polaritons [ 25 , 39 , 40 , 41 , 42 ], i.e., In Equations ( 1 ) and (2), the m is the effective mass of lower polaritons, P is the off-resonant continuous-wave pumping rate, and denote the lifetimes of the condensate and reservoir polaritons, respectively, R is the stimulated scattering rate of reservoir polaritons into the condensate, characterizes the strengths of the polariton interaction, while denotes the interaction strength between the reservoir and the polaritons. The impurity potential [ 39 , 43 ] is , with the strength .…”
Section: The Theoretical Model and Lagrangian Approachmentioning
confidence: 99%
“…Such intrinsic spontaneous PT -symmetry breaking occurs at the exceptional points (EP), at which both the eigenstates and eigenvalues coalesce [8][9][10][11][12][13][14][15][16]. The existence of EP leads to rich physics, such as the enhancement of precision in quantum sensors [17], the topological phase transition [18][19][20][21][22], the nonadiabatic transition [23,24], and the unidirectional propagation of light [25], just to name a few. Theoretical advances have enabled exponential realizations of PT symmetric systems in various fields, such as optical settings [26][27][28][29][30][31][32][33][34][35][36][37], electronic circuits [38], and optomechanical systems [39].…”
Section: Introductionmentioning
confidence: 99%