Tuning the Coherent Propagation of Organic Exciton-Polaritons through the Cavity Q-factor
Transport of excitons in organic materials can be enhanced through polariton formation when the interaction strength between these excitons and the confined light modes of an optical resonator exceeds their decay rates. While the polariton lifetime is determined by the Q(uality)-factor of the optica...
| Autores: | , , |
|---|---|
| Formato: | artículo |
| Fecha de publicación: | 2023 |
| País: | España |
| Recursos: | Universidad Autónoma de Madrid |
| Repositorio: | Biblos-e Archivo. Repositorio Institucional de la UAM |
| Idioma: | inglés |
| OAI Identifier: | oai:repositorio.uam.es:10486/713436 |
| Acesso em linha: | http://hdl.handle.net/10486/713436 https://dx.doi.org/10.1002/advs.202302650 |
| Access Level: | acceso abierto |
| Palavra-chave: | Fabry–Pérot cavity molecular dynamics polariton strong light–matter coupling excitation energy transfer Física |
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Tuning the Coherent Propagation of Organic Exciton-Polaritons through the Cavity Q-factorTichauer, Ruth ElenaSokolovskii, IliaGroenhof, GerritFabry–Pérot cavitymolecular dynamicspolaritonstrong light–matter couplingexcitation energy transferFísicaTransport of excitons in organic materials can be enhanced through polariton formation when the interaction strength between these excitons and the confined light modes of an optical resonator exceeds their decay rates. While the polariton lifetime is determined by the Q(uality)-factor of the optical resonator, the polariton group velocity is not. Instead, the latter is solely determined by the polariton dispersion. Yet, experiments suggest that the Q-factor also controls the polariton propagation velocity. To understand this observation, the authors perform molecular dynamics simulations of Rhodamine chromophores strongly coupled to Fabry–Pérot cavities with various Q-factors. The results suggest that propagation in the aforementioned experiments is initially dominated by ballistic motion of upper polariton states at their group velocities, which leads to a rapid expansion of the wavepacket. Cavity decay in combination with non-adiabatic population transfer into dark states, rapidly depletes these bright states, causing the wavepacket to contract. However, because population transfer is reversible, propagation continues, but as a diffusion process, at lower velocity. By controlling the lifetime of bright states, the Q-factor determines the duration of the ballistic phase and the diffusion coefficient in the diffusive regime. Thus, polariton propagation in organic microcavities can be effectively tuned through the Q-factorThis work was supported by the Academy of Finland (Grant 323996), the European Research Council (Grant No. ERC-2016-StG-714870 to Johannes Feist), and by the Spanish Ministry for Science, Innovation, Universities-Agencia Estatal de Investigación (AEI) through Grants (PID2021-125894NB-I00 and CEX2018-000805-M (through the María de Maeztu program for Units of Excellence in Research and Development)John Wiley and Sons IncDepartamento de Física Teórica de la Materia CondensadaFacultad de Ciencias20232023-11-24research articlehttp://purl.org/coar/resource_type/c_2df8fbb1VoRhttp://purl.org/coar/version/c_970fb48d4fbd8a85info:eu-repo/semantics/articleapplication/pdfhttp://hdl.handle.net/10486/713436https://dx.doi.org/10.1002/advs.202302650reponame:Biblos-e Archivo. Repositorio Institucional de la UAMinstname:Universidad Autónoma de MadridInglésengopen accesshttp://purl.org/coar/access_right/c_abf2Attribution 4.0 Internationalhttp://creativecommons.org/licenses/by/4.0/info:eu-repo/semantics/openAccessoai:repositorio.uam.es:10486/7134362026-06-23T12:46:27Z |
| dc.title.none.fl_str_mv |
Tuning the Coherent Propagation of Organic Exciton-Polaritons through the Cavity Q-factor |
| title |
Tuning the Coherent Propagation of Organic Exciton-Polaritons through the Cavity Q-factor |
| spellingShingle |
Tuning the Coherent Propagation of Organic Exciton-Polaritons through the Cavity Q-factor Tichauer, Ruth Elena Fabry–Pérot cavity molecular dynamics polariton strong light–matter coupling excitation energy transfer Física |
| title_short |
Tuning the Coherent Propagation of Organic Exciton-Polaritons through the Cavity Q-factor |
| title_full |
Tuning the Coherent Propagation of Organic Exciton-Polaritons through the Cavity Q-factor |
| title_fullStr |
Tuning the Coherent Propagation of Organic Exciton-Polaritons through the Cavity Q-factor |
| title_full_unstemmed |
Tuning the Coherent Propagation of Organic Exciton-Polaritons through the Cavity Q-factor |
| title_sort |
Tuning the Coherent Propagation of Organic Exciton-Polaritons through the Cavity Q-factor |
| dc.creator.none.fl_str_mv |
Tichauer, Ruth Elena Sokolovskii, Ilia Groenhof, Gerrit |
| author |
Tichauer, Ruth Elena |
| author_facet |
Tichauer, Ruth Elena Sokolovskii, Ilia Groenhof, Gerrit |
| author_role |
author |
| author2 |
Sokolovskii, Ilia Groenhof, Gerrit |
| author2_role |
author author |
| dc.contributor.none.fl_str_mv |
Departamento de Física Teórica de la Materia Condensada Facultad de Ciencias |
| dc.subject.none.fl_str_mv |
Fabry–Pérot cavity molecular dynamics polariton strong light–matter coupling excitation energy transfer Física |
| topic |
Fabry–Pérot cavity molecular dynamics polariton strong light–matter coupling excitation energy transfer Física |
| description |
Transport of excitons in organic materials can be enhanced through polariton formation when the interaction strength between these excitons and the confined light modes of an optical resonator exceeds their decay rates. While the polariton lifetime is determined by the Q(uality)-factor of the optical resonator, the polariton group velocity is not. Instead, the latter is solely determined by the polariton dispersion. Yet, experiments suggest that the Q-factor also controls the polariton propagation velocity. To understand this observation, the authors perform molecular dynamics simulations of Rhodamine chromophores strongly coupled to Fabry–Pérot cavities with various Q-factors. The results suggest that propagation in the aforementioned experiments is initially dominated by ballistic motion of upper polariton states at their group velocities, which leads to a rapid expansion of the wavepacket. Cavity decay in combination with non-adiabatic population transfer into dark states, rapidly depletes these bright states, causing the wavepacket to contract. However, because population transfer is reversible, propagation continues, but as a diffusion process, at lower velocity. By controlling the lifetime of bright states, the Q-factor determines the duration of the ballistic phase and the diffusion coefficient in the diffusive regime. Thus, polariton propagation in organic microcavities can be effectively tuned through the Q-factor |
| publishDate |
2023 |
| dc.date.none.fl_str_mv |
2023 2023-11-24 |
| dc.type.none.fl_str_mv |
research article http://purl.org/coar/resource_type/c_2df8fbb1 VoR http://purl.org/coar/version/c_970fb48d4fbd8a85 |
| dc.type.openaire.fl_str_mv |
info:eu-repo/semantics/article |
| format |
article |
| dc.identifier.none.fl_str_mv |
http://hdl.handle.net/10486/713436 https://dx.doi.org/10.1002/advs.202302650 |
| url |
http://hdl.handle.net/10486/713436 https://dx.doi.org/10.1002/advs.202302650 |
| dc.language.none.fl_str_mv |
Inglés eng |
| language_invalid_str_mv |
Inglés |
| language |
eng |
| dc.rights.none.fl_str_mv |
open access http://purl.org/coar/access_right/c_abf2 Attribution 4.0 International http://creativecommons.org/licenses/by/4.0/ |
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info:eu-repo/semantics/openAccess |
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open access http://purl.org/coar/access_right/c_abf2 Attribution 4.0 International http://creativecommons.org/licenses/by/4.0/ |
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openAccess |
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application/pdf |
| dc.publisher.none.fl_str_mv |
John Wiley and Sons Inc |
| publisher.none.fl_str_mv |
John Wiley and Sons Inc |
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reponame:Biblos-e Archivo. Repositorio Institucional de la UAM instname:Universidad Autónoma de Madrid |
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Universidad Autónoma de Madrid |
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Biblos-e Archivo. Repositorio Institucional de la UAM |
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Biblos-e Archivo. Repositorio Institucional de la UAM |
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15.812429 |