“…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 .…”