Abstract
We theoretically investigate a Bose-condensed exciton gas out of equilibrium. Within the framework of the combined BCS-Leggett strong-coupling theory with the non-equilibrium Keldysh formalism, we show how the Bose–Einstein condensation (BEC) of excitons is suppressed to eventually disappear, when the system is in the non-equilibrium steady state. The supply of electrons and holes from the bath is shown to induce quasi-particle excitations, leading to the partial occupation of the upper branch of Bogoliubov single-particle excitation spectrum. We also discuss how this quasi-particle induction is related to the suppression of exciton BEC, as well as the stability of the steady state.
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Notes
We briefly note that, some exciton systems with long carrier lifetime (e.g., excitons in Si) can be regarded as (quasi-)equilibrium system. We also note that cold atom systems always have some decay of atoms from the trap, although they are negligible.
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Acknowledgments
We thank M. Yamaguchi, R. Okuyama, D. Inotani, H. Tajima, and A. Edelman for useful discussions. RH was supported by a Grand-in-Aid for JSPS fellows. This work was supported by KiPAS project in Keio University. YO was also supported by Grant-in-Aid for Scientific research from MEXT and JSPS in Japan (25400418, 15H00840). Work at Argonne National Laboratory is supported by the U.S. Department of Energy, Office of Basic Energy Sciences under Contract No. DE-AC02-06CH11357.
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Hanai, R., Littlewood, P.B. & Ohashi, Y. Non-equilibrium Properties of a Pumped-Decaying Bose-Condensed Electron–Hole Gas in the BCS–BEC Crossover Region. J Low Temp Phys 183, 127–135 (2016). https://doi.org/10.1007/s10909-016-1552-6
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DOI: https://doi.org/10.1007/s10909-016-1552-6