Bi-self-trapping of excitons via the long-living phonon mode and their superfluorescent markers

• URL: http://arxiv.org/abs/2501.16874v1
• Date: Tue, 28 Jan 2025 11:56:03 GMT
• Title: Bi-self-trapping of excitons via the long-living phonon mode and their superfluorescent markers
• Authors: Vladimir Al. Osipov,
• Abstract summary: Room-temperature superfluorescence recently observed in hybrid excitations at high concentrations of perovskites lacks comprehensive theoretical framework.<n>We offer the two-step mechanism: formation of two self-trapped excitons entangled via the same long-living phonon mode, and their rearrangement into a superradiating mirror symmetric configuration.<n>Our findings indicate that the self-trapped excitons are described by the stable phase-locked steadystate solution of the equations of motion, and at elevated exciton concentrations, they compete with the bi-self-trapped excitons.
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• License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
• Abstract: Understanding the origin of the system response offers guidance for designing single-component material devices with required properties. A notable phenomenon of room-temperature superfluorescence recently observed in hybrid perovskites at high concentrations of excitations lacks of comprehensive theoretical framework. Addressing this gap necessitates a discussion grounded in non-linear and multiparticle theories. In this study, we offer the two-step mechanism: formation of two self-trapped excitons entangled via the same long-living phonon mode, and their rearrangement into a superradiating mirror symmetric configuration. Based on the semiclassical equations of motion we examine the criteria for the high-temperature self-trapping and bi-self trapping of excitons. Our findings indicate that the self-trapped excitons are described by the stable phase-locked steadystate solution of the equations of motion, and at elevated exciton concentrations, they compete with the bi-self-trapped excitons. The latter is described by the Dicke model and is thus responsible for the generation of the superfluorescent spectral peak. The obtained theoretical spectra are in good agreement with the experimental observation.

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