2016
DOI: 10.1103/physrevb.94.195301
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Coherent and incoherent aspects of polariton dynamics in semiconductor microcavities

Abstract: The interaction between coherent polaritons and incoherent excitons plays an important role in polariton physics. Using resonant pump-probe spectroscopy with selective excitation of single polariton branches, we investigate the different dephasing mechanisms responsible for generating a long-lived exciton reservoir. As expected, pumping the upper polariton results in a strong dephasing process that leads to the generation of a long lived reservoir. Unexpectedly, we observe an efficient reservoir creation while… Show more

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Cited by 12 publications
(12 citation statements)
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“…3 A and C are due to dark-excitedstate population and occur after selective excitation of either polariton. The fact that response is qualitatively similar when exciting at the LP, UP, or even the dark-state frequency indicates that there are polariton-dark-state interactions that lead polaritonic excitations (either LP or UP) to transfer into dark states possibly via phonon scattering (26,27).…”
Section: Resultsmentioning
confidence: 98%
“…3 A and C are due to dark-excitedstate population and occur after selective excitation of either polariton. The fact that response is qualitatively similar when exciting at the LP, UP, or even the dark-state frequency indicates that there are polariton-dark-state interactions that lead polaritonic excitations (either LP or UP) to transfer into dark states possibly via phonon scattering (26,27).…”
Section: Resultsmentioning
confidence: 98%
“…The cause is that the model used here is fully coherent and neglects any long-lived population beyond the cavity lifetime. Inspired by previous works [19,49,50], we try to construct phenomenologically a set of coupled mode equations in-cluding an exciton reservoir:…”
Section: Discussionmentioning
confidence: 99%
“…where n R,↓ is the spin-down reservoir population and a long lifetime is assumed γ R = 0.01 meV [19]. Here we neglect the creation of a spin-up incoherent reservoir and a corresponding coherent population of polaritons, because the spin-up probe pulse is weak and, thus, contribute only by a small amount of spin-up excitons and polaritons to the incoherent reservoir and to the coherent population, respectively.…”
Section: Appendix A: Spinor Polariton Dynamicsmentioning
confidence: 99%
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“…System.-We consider a two-dimensional (2D) mixture of polaritons in spin states σ = {↓, ↑}, resulting from the coupling of two quantum light fields with counter-circular polarizations to the excitonic modes of a 2D semiconductor microcavity [22][23][24][25]32]. The Hamiltonian is…”
mentioning
confidence: 99%