Coupling polyatomic molecules to lossy nanocavities: Lindblad vs Schrödinger description

Author:

Fábri Csaba12ORCID,Császár Attila G.13ORCID,Halász Gábor J.4ORCID,Cederbaum Lorenz S.5ORCID,Vibók Ágnes26ORCID

Affiliation:

1. HUN-REN–ELTE Complex Chemical Systems Research Group 1 , P.O. Box 32, H-1518 Budapest 112, Hungary

2. Department of Theoretical Physics, University of Debrecen 2 , P.O. Box 400, H-4002 Debrecen, Hungary

3. Laboratory of Molecular Structure and Dynamics, Institute of Chemistry, ELTE Eötvös Loránd University 3 , Pázmány Péter sétány 1/A, H-1117 Budapest, Hungary

4. Department of Information Technology, University of Debrecen 4 , P.O. Box 400, H-4002 Debrecen, Hungary

5. Theoretische Chemie, Physikalisch-Chemisches Institut, Universität Heidelberg 5 , D-69120 Heidelberg, Germany

6. ELI-ALPS, ELI-HU Non-Profit Ltd. 6 , Dugonics tér 13, H-6720 Szeged, Hungary

Abstract

The use of cavities to impact molecular structure and dynamics has become popular. As cavities, in particular plasmonic nanocavities, are lossy and the lifetime of their modes can be very short, their lossy nature must be incorporated into the calculations. The Lindblad master equation is commonly considered an appropriate tool to describe this lossy nature. This approach requires the dynamics of the density operator and is thus substantially more costly than approaches employing the Schrödinger equation for the quantum wave function when several or many nuclear degrees of freedom are involved. In this work, we compare numerically the Lindblad and Schrödinger descriptions discussed in the literature for a molecular example where the cavity is pumped by a laser. The laser and cavity properties are varied over a range of parameters. It is found that the Schrödinger description adequately describes the dynamics of the polaritons and emission signal as long as the laser intensity is moderate and the pump time is not much longer than the lifetime of the cavity mode. Otherwise, it is demonstrated that the Schrödinger description gradually fails. We also show that the failure of the Schrödinger description can often be remedied by renormalizing the wave function at every step of time propagation. The results are discussed and analyzed.

Funder

Nemzeti Kutatási, Fejlesztési és Innovaciós Alap

Deutsche Forschungsgemeinschaft

Cost Actions

HUNREN Hungarian Research Network

Publisher

AIP Publishing

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