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Symmetries and conservation laws in quantum trajectories: Dissipative freezing

Abstract:
In driven-dissipative systems, the presence of a strong symmetry guarantees the existence of several steady states belonging to different symmetry sectors. Here we show that, when a system with a strong symmetry is initialized in a quantum superposition involving several of these sectors, each individual stochastic trajectory will randomly select a single one of them and remain there for the rest of the evolution. Since a strong symmetry implies a conservation law for the corresponding symmetry operator on the ensemble level, this selection of a single sector from an initial superposition entails a breakdown of this conservation law at the level of individual realizations. Given that such a superposition is impossible in a classical, stochastic trajectory, this is a a purely quantum effect with no classical analogue. Our results show that a system with a closed Liouvillian gap may exhibit, when monitored over a single run of an experiment, a behaviour completely opposite to the usual notion of dynamical phase coexistence and intermittency, which are typically considered hallmarks of a dissipative phase transition. We discuss our results with a simple, realistic model of squeezed superradiance.
Publication status:
Published
Peer review status:
Peer reviewed

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Publisher copy:
10.1103/physreva.100.042113

Authors


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Institution:
University of Oxford
Division:
MPLS Division
Department:
Physics
Sub department:
Atomic and Laser Physics
Role:
Author
ORCID:
0000-0001-8775-0135
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Role:
Author
ORCID:
0000-0003-1335-8637
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Role:
Author
ORCID:
0000-0002-9704-3941


Publisher:
American Physical Society
Journal:
Physical Review A More from this journal
Volume:
100
Issue:
4
Article number:
042113
Publication date:
2019-10-16
DOI:
EISSN:
2469-9934
ISSN:
2469-9926


Language:
English
Keywords:
Pubs id:
pubs:1048797
UUID:
uuid:121429cf-8b32-43c6-bd37-187ad9add803
Local pid:
pubs:1048797
Source identifiers:
1048797
Deposit date:
2019-10-18

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