Competition between collective and individual conical intersection dynamics in an optical cavity

Light-induced nonadiabatic phenomena arise when molecules or molecular ensembles are exposed to resonant external electromagnetic fields. The latter can either be classical laser or quantized cavity radiation fields, which can couple to either the electronic, nuclear or rotational degrees of freedom...

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Main Authors: András Csehi, Oriol Vendrell, Gábor J Halász, Ágnes Vibók
Format: Article
Language:English
Published: IOP Publishing 2022-01-01
Series:New Journal of Physics
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/ac7df7
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author András Csehi
Oriol Vendrell
Gábor J Halász
Ágnes Vibók
author_facet András Csehi
Oriol Vendrell
Gábor J Halász
Ágnes Vibók
author_sort András Csehi
collection DOAJ
description Light-induced nonadiabatic phenomena arise when molecules or molecular ensembles are exposed to resonant external electromagnetic fields. The latter can either be classical laser or quantized cavity radiation fields, which can couple to either the electronic, nuclear or rotational degrees of freedom of the molecule. In the case of quantized radiation fields, the light–matter coupling results in the formation of two new hybrid light–matter states, namely the upper and lower ‘polaritons’. Light-induced avoided crossings and light-induced conical intersections (CIs) between polaritons exist as a function of the vibrational and rotational coordinates of single molecules. For ensembles of N molecules, the N − 1 dark states between the two optically active polaritons feature, additionally, so-called collective CIs, involving the coordinates of more than one molecule to form. Here, we study the competition between intramolecular and collective light-induced nonadiabatic phenomena by comparing the escape rate from the Franck–Condon region of a single molecule and of a molecular ensemble coupled to a cavity mode. In situations where the polaritonic gap would be large and the dark-state decay channels could not be reached effectively, the presence of a seam of light-induced CI between the polaritons facilitates again the participation of the dark manifold, resulting in a cooperative effect that determines the overall non-radiative decay rate from the upper into the lower polaritonic states.
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spelling doaj.art-3f266ac694e249e2822eeceff874de832023-08-09T14:26:26ZengIOP PublishingNew Journal of Physics1367-26302022-01-0124707302210.1088/1367-2630/ac7df7Competition between collective and individual conical intersection dynamics in an optical cavityAndrás Csehi0https://orcid.org/0000-0002-8794-6610Oriol Vendrell1https://orcid.org/0000-0003-4629-414XGábor J Halász2https://orcid.org/0000-0002-7010-4302Ágnes Vibók3https://orcid.org/0000-0001-6821-9525Department of Theoretical Physics, Faculty of Science and Technology, University of Debrecen , H-4002 Debrecen, PO Box 400, HungaryTheoretical Chemistry, Institute of Physical Chemistry, Heidelberg University , Im Neuenheimer Feld 229, 69120 Heidelberg, GermanyDepartment of Information Technology, Faculty of Informatics, University of Debrecen , H-4002 Debrecen, PO Box 400, HungaryDepartment of Theoretical Physics, Faculty of Science and Technology, University of Debrecen , H-4002 Debrecen, PO Box 400, Hungary; ELI-ALPS, ELI-HU Non-Profit Ltd. , H-6720 Szeged, Dugonics tér 13, HungaryLight-induced nonadiabatic phenomena arise when molecules or molecular ensembles are exposed to resonant external electromagnetic fields. The latter can either be classical laser or quantized cavity radiation fields, which can couple to either the electronic, nuclear or rotational degrees of freedom of the molecule. In the case of quantized radiation fields, the light–matter coupling results in the formation of two new hybrid light–matter states, namely the upper and lower ‘polaritons’. Light-induced avoided crossings and light-induced conical intersections (CIs) between polaritons exist as a function of the vibrational and rotational coordinates of single molecules. For ensembles of N molecules, the N − 1 dark states between the two optically active polaritons feature, additionally, so-called collective CIs, involving the coordinates of more than one molecule to form. Here, we study the competition between intramolecular and collective light-induced nonadiabatic phenomena by comparing the escape rate from the Franck–Condon region of a single molecule and of a molecular ensemble coupled to a cavity mode. In situations where the polaritonic gap would be large and the dark-state decay channels could not be reached effectively, the presence of a seam of light-induced CI between the polaritons facilitates again the participation of the dark manifold, resulting in a cooperative effect that determines the overall non-radiative decay rate from the upper into the lower polaritonic states.https://doi.org/10.1088/1367-2630/ac7df7conical intersectionsradiation fieldcollective effectlight-induced nonadiabatic phenomena
spellingShingle András Csehi
Oriol Vendrell
Gábor J Halász
Ágnes Vibók
Competition between collective and individual conical intersection dynamics in an optical cavity
New Journal of Physics
conical intersections
radiation field
collective effect
light-induced nonadiabatic phenomena
title Competition between collective and individual conical intersection dynamics in an optical cavity
title_full Competition between collective and individual conical intersection dynamics in an optical cavity
title_fullStr Competition between collective and individual conical intersection dynamics in an optical cavity
title_full_unstemmed Competition between collective and individual conical intersection dynamics in an optical cavity
title_short Competition between collective and individual conical intersection dynamics in an optical cavity
title_sort competition between collective and individual conical intersection dynamics in an optical cavity
topic conical intersections
radiation field
collective effect
light-induced nonadiabatic phenomena
url https://doi.org/10.1088/1367-2630/ac7df7
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AT oriolvendrell competitionbetweencollectiveandindividualconicalintersectiondynamicsinanopticalcavity
AT gaborjhalasz competitionbetweencollectiveandindividualconicalintersectiondynamicsinanopticalcavity
AT agnesvibok competitionbetweencollectiveandindividualconicalintersectiondynamicsinanopticalcavity