Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Uspekhi Fizicheskih Nauk

Collective states of excitons in semiconductors

Михаил Михайлович Глазов, Robert A. Suris

Published Oct 1, 2019• 5 citations
Publisher
DOI
10.3367/ufnr.2019.10.038663

Related papers

Collective properties of excitons in semiconductors

Leonid V. Keldysh, Andrey Nikolaevich Kozlov

WORLD SCIENTIFIC eBooks•Nov 1, 2023•150 citations

Third-order excitonic nonlinearity in semiconductors: the role of the transitions involving two-exciton states

Victor I. Klimov

European Quantum Electronics Conference (EQEC)•Jan 1, 1994•0 citations

Observation of non-classical light in semiconductor microcavities

Lebedev, Mikhail, A.L. Parakhonsky, A. A. Demenev

Semiconductor microcavities are widely used to study collective interactions of cavity exciton-polaritons leading to their condensation phenomenon. Exciton-light interaction is highly enhanced in such structures due to the resonance enhancement of the electromagnetic field inside the high quality cavity. Considerably lower interest is concerned to exciton states non-resonant with the cavity mode for which the exciton-photon interaction is strongly reduced due to the existence of the cavity. We point out here that these states are responsible for non-classical light generation in semiconductor microcavities.

arXiv:1407.4068•Jul 15, 2014•0 citations

Collective two-boson decay of excitons in a Bose-Einstein condensate and generation of coherent photon-phonon radiation

H. K. Avetissian, A. K. Avetissian, G. F. Mkrtchian +1 more

The collective decay of excitons from initial Bose-Einstein condensate state is investigated theoretically. As a practically more interesting case we consider excitons of the yellow series in the semiconductor cuprous oxide where we have collective photon and phonon-assisted decay of excitons. It is shown that because of intrinsic instability of recoilless two-boson decay of Bose-Einstein condensate, the spontaneously emitted bosonic pairs are amplified, leading to an exponential buildup of a macroscopic population into the certain modes. The collective decay rate has a nonlinear dependence on the excitonic density being comparable or larger than the Auger recombination loss rate up to the high densities, which makes obtainable its observation. The phenomenon considered can also be applied for the realization of a phonon laser.

arXiv:1704.01558•Physical review. B./Physical review. B•Jul 27, 2017•1 citation

Macroscopic coherent states of excitons in semiconductors

Leonid V. Keldysh

WORLD SCIENTIFIC eBooks•Nov 1, 2023•3 citations

Coherent states of excitons

Leonid V. Keldysh

WORLD SCIENTIFIC eBooks•Nov 1, 2023•1 citation
Semiconductor microcavities are widely used to study collective interactions of cavity exciton-polaritons leading to their condensation phenomenon. Exciton-light interaction is highly enhanced in such structures due to the resonance enhancement of the electromagnetic field inside the high quality cavity. Considerably lower interest is concerned to exciton states non-resonant with the cavity mode for which the exciton-photon interaction is strongly reduced due to the existence of the cavity. We point out here that these states are responsible for non-classical light generation in semiconductor microcavities.
The collective decay of excitons from initial Bose-Einstein condensate state is investigated theoretically. As a practically more interesting case we consider excitons of the yellow series in the semiconductor cuprous oxide where we have collective photon and phonon-assisted decay of excitons. It is shown that because of intrinsic instability of recoilless two-boson decay of Bose-Einstein condensate, the spontaneously emitted bosonic pairs are amplified, leading to an exponential buildup of a macroscopic population into the certain modes. The collective decay rate has a nonlinear dependence on the excitonic density being comparable or larger than the Auger recombination loss rate up to the high densities, which makes obtainable its observation. The phenomenon considered can also be applied for the realization of a phonon laser.