The Generalized Tavis—Cummings Model with Cavity Damping
In this Communication, we consider a generalised Tavis–Cummings model when the damping process is taken into account. We show that the quantum dynamics governed by a non-Hermitian Hamiltonian is exactly solvable using the Quantum Inverse Scattering Method, and the Algebraic Bethe Ansatz. The leakage...
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2021
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oai:doaj.org-article:ae3d863d1a184e95a4d5abe818258da92021-11-25T19:06:54ZThe Generalized Tavis—Cummings Model with Cavity Damping10.3390/sym131121242073-8994https://doaj.org/article/ae3d863d1a184e95a4d5abe818258da92021-11-01T00:00:00Zhttps://www.mdpi.com/2073-8994/13/11/2124https://doaj.org/toc/2073-8994In this Communication, we consider a generalised Tavis–Cummings model when the damping process is taken into account. We show that the quantum dynamics governed by a non-Hermitian Hamiltonian is exactly solvable using the Quantum Inverse Scattering Method, and the Algebraic Bethe Ansatz. The leakage of photons is described by a Lindblad-type master equation. The non-Hermitian Hamiltonian is diagonalised by state vectors, which are elementary symmetric functions parametrised by the solutions of the Bethe equations. The time evolution of the photon annihilation operator is defined via a corresponding determinant representation.Nikolai M. BogoliubovAndrei V. RybinMDPI AGarticleopen quantum systemBethe AnsatzLindblad equationMathematicsQA1-939ENSymmetry, Vol 13, Iss 2124, p 2124 (2021) |
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open quantum system Bethe Ansatz Lindblad equation Mathematics QA1-939 |
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open quantum system Bethe Ansatz Lindblad equation Mathematics QA1-939 Nikolai M. Bogoliubov Andrei V. Rybin The Generalized Tavis—Cummings Model with Cavity Damping |
description |
In this Communication, we consider a generalised Tavis–Cummings model when the damping process is taken into account. We show that the quantum dynamics governed by a non-Hermitian Hamiltonian is exactly solvable using the Quantum Inverse Scattering Method, and the Algebraic Bethe Ansatz. The leakage of photons is described by a Lindblad-type master equation. The non-Hermitian Hamiltonian is diagonalised by state vectors, which are elementary symmetric functions parametrised by the solutions of the Bethe equations. The time evolution of the photon annihilation operator is defined via a corresponding determinant representation. |
format |
article |
author |
Nikolai M. Bogoliubov Andrei V. Rybin |
author_facet |
Nikolai M. Bogoliubov Andrei V. Rybin |
author_sort |
Nikolai M. Bogoliubov |
title |
The Generalized Tavis—Cummings Model with Cavity Damping |
title_short |
The Generalized Tavis—Cummings Model with Cavity Damping |
title_full |
The Generalized Tavis—Cummings Model with Cavity Damping |
title_fullStr |
The Generalized Tavis—Cummings Model with Cavity Damping |
title_full_unstemmed |
The Generalized Tavis—Cummings Model with Cavity Damping |
title_sort |
generalized tavis—cummings model with cavity damping |
publisher |
MDPI AG |
publishDate |
2021 |
url |
https://doaj.org/article/ae3d863d1a184e95a4d5abe818258da9 |
work_keys_str_mv |
AT nikolaimbogoliubov thegeneralizedtaviscummingsmodelwithcavitydamping AT andreivrybin thegeneralizedtaviscummingsmodelwithcavitydamping AT nikolaimbogoliubov generalizedtaviscummingsmodelwithcavitydamping AT andreivrybin generalizedtaviscummingsmodelwithcavitydamping |
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