2020
DOI: 10.1103/physrevlett.124.030401
|View full text |Cite
|
Sign up to set email alerts
|

Reservoir-Mediated Quantum Correlations in Non-Hermitian Optical System

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
2

Citation Types

0
32
1

Year Published

2020
2020
2023
2023

Publication Types

Select...
6
2

Relationship

0
8

Authors

Journals

citations
Cited by 44 publications
(34 citation statements)
references
References 47 publications
0
32
1
Order By: Relevance
“…Thus, the loss-induced increase in average photon number of the cavities in absence of any coherent drive is a feature possible only in a non-Hermitian system with a gain medium having quantum fluctuations. This feature of the nonequilibrium steady state thereby distinguishes our proposed setup from previous experiments involving gain in classical systems [35][36][37][38][39], as well as the existing experiments in the quantum regime which do not feature a gain medium [60][61][62][63][64][65][66][67][68][69].…”
Section: B Loss-induced Lasing and Amplificationmentioning
confidence: 76%
See 2 more Smart Citations
“…Thus, the loss-induced increase in average photon number of the cavities in absence of any coherent drive is a feature possible only in a non-Hermitian system with a gain medium having quantum fluctuations. This feature of the nonequilibrium steady state thereby distinguishes our proposed setup from previous experiments involving gain in classical systems [35][36][37][38][39], as well as the existing experiments in the quantum regime which do not feature a gain medium [60][61][62][63][64][65][66][67][68][69].…”
Section: B Loss-induced Lasing and Amplificationmentioning
confidence: 76%
“…(Note that in other setups loss-induced lasing can occur without any exceptional point [111].) This explicitly requires a gain medium and cannot be observed in the existing experiments in the quantum regime [60][61][62][63][64][65][66][67][68][69], none of which features a gain medium. The real and imaginary parts of the eigenvalues of H eff as a function of κ 2 are plotted in Fig.…”
Section: B Loss-induced Lasing and Amplificationmentioning
confidence: 99%
See 1 more Smart Citation
“…While their introduction dates back to the early age of quantum mechanics [2], only in recent years it was realized and experimentally confirmed that systems described by NH Hamiltonians can exhibit under suitable conditions a variety of exotic phenomena [3,4]. Among these are: coalescence of eigenstates at exceptional points [5], unconventional geometric phase [6], failure of bulk-edge correspondence [7], critical behavior of quantum correlations around exceptional points [8][9][10], non-Hermitian skin effect [11]. As a typical consequence, traditional tenets of Physics such as the Bloch theory of bands and even the very notion of "bulk" may require a non-trivial revision in the non-Hermitian realm [12].…”
Section: Introductionmentioning
confidence: 99%
“…On the contrary, APT symmetry does not need gain but can still exhibit EP with entirely imaginary eigenvalues in the symmetric phase (see Fig. 1(a)) [9], which has been extensively explored both in experiments [10,[17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33] and in theories . This striking difference provides us a variety of novel opportunities to explore APT effects in atomic systems [10,17], photonic or magnonic devices [18][19][20][21][22], and thermal structures [23,24].…”
Section: Introductionmentioning
confidence: 99%