2020
DOI: 10.1103/physreva.101.013817
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Fermionic formalism for driven-dissipative multilevel systems

Abstract: We present a fermionic description of non-equilibrium multi-level systems. Our approach uses the Keldysh path integral formalism and allows us to take into account periodic drives, as well as dissipative channels. The technique is based on the Majorana fermion representation of spin-1/2 models which follows earlier applications in the context of spin and Kondo systems. We apply this formalism to problems of increasing complexity: a dissipative two-level system, a driven-dissipative multi-level atom, and a gene… Show more

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Cited by 27 publications
(20 citation statements)
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“…This trend resembles the behavior predicted for the counterrotating (also known as inverted) and regular lasing regimes using a generalization of the Dicke model reported in Refs. [27][28][29]34]. Furthermore, the counterrotating lasing occurs below the population inversion d 0 < 0 and has a phase boundary with the superradiant state.…”
Section: B Second-moment Analysismentioning
confidence: 99%
See 1 more Smart Citation
“…This trend resembles the behavior predicted for the counterrotating (also known as inverted) and regular lasing regimes using a generalization of the Dicke model reported in Refs. [27][28][29]34]. Furthermore, the counterrotating lasing occurs below the population inversion d 0 < 0 and has a phase boundary with the superradiant state.…”
Section: B Second-moment Analysismentioning
confidence: 99%
“…The Dicke model provides a fundamental model of cavity QED and has been studied in a context of superradiant phase transition in both equilibrium and nonequilibrium regimes [27]. Its generalized version with imbalanced rotating and counterrotating terms has revealed a rich phase diagram allowing for the superradiant and various lasing states [27][28][29].…”
Section: Introductionmentioning
confidence: 99%
“…In this article, we use the Majorana Fermion representation of spin 1/2 systems [49][50][51][52][53] in combination with the diagrammatic method of Ref. 54 to compute λ L throughout the phase diagram to leading order in 1/N .…”
Section: Introductionmentioning
confidence: 99%
“…While these observed scaling dependencies for the first burst peak of photon production from vacuum coincide with those for Dicke superradiant bursts 24 , they are not properly a superradiant phase however 32,36,40 . In order to understand better the nature of this enhanced vacuum photon production phase, it is informative to apply the unitary transformation U ¼ expðiπJ x =2Þ to the master Eq.…”
Section: Tls Defectsmentioning
confidence: 58%