A unified theory for excited-state, fragmented, and equilibrium-like Bose condensation in pumped photonic many-body systems
Daniel Vorberg, Roland Ketzmerick, Andr\'e Eckardt

TL;DR
This paper develops a unified kinetic theory for nonequilibrium Bose condensation in photonic systems, explaining various condensation phenomena, including equilibrium-like, fragmented, and excited-state condensates, with predictions matching experimental observations.
Contribution
It introduces a comprehensive kinetic framework that captures multiple Bose condensation regimes in pumped photonic systems, highlighting the role of pump power and reservoir coupling.
Findings
Sequence of nonequilibrium phase transitions with increasing pump power.
Identification of a sharp criterion for state selection to host a condensate.
Prediction of reservoir occupation being clamped at a constant value with odd number of condensates.
Abstract
We derive a theory for Bose condensation in nonequilibrium steady states of bosonic quantum gases that are coupled both to a thermal heat bath and to a pumped reservoir (or gain medium), while suffering from loss. Such a scenario describes photonic many-body systems such as exciton-polariton gases. Our analysis is based on a set of kinetic equations for a gas of noninteracting bosons. By identifying a dimensionless scaling parameter controlling the boson density, we derive a sharp criterion for which system states become selected to host a macroscopic occupation. We show that with increasing pump power, the system generically undergoes a sequence of nonequilibrum phase transitions. At each transition a state either becomes or ceases to be Bose selected (i.e. to host a condensate): The state which first acquires a condensate when the pumping exceeds a threshold is the one with the…
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