Magnetization in a non-equilibrium quantum spin system
X. Z. Zhang

TL;DR
This paper reveals that in critical open quantum systems, the long-term dynamics and steady states can be effectively described by a non-Hermitian Hamiltonian, enabling better quantum control and understanding of non-equilibrium behaviors.
Contribution
It demonstrates that the effective non-Hermitian Hamiltonian accurately captures the long-term dynamics and steady states of critical open quantum systems, challenging conventional distinctions.
Findings
The NESS is identical to the coalescent state of the non-Hermitian Hamiltonian.
Local dissipation induces collective spin alignment controlled by quantum jumps.
The long-time coherence is maintained in the NESS, enabling quantum control.
Abstract
The dynamics described by the non-Hermitian Hamiltonian typically capture the short-term behavior of open quantum systems before quantum jumps occur. In contrast, the long-term dynamics, characterized by the Lindblad master equation (LME), drive the system towards a non-equilibrium steady state (NESS), which is an eigenstate with zero energy of the Liouvillian superoperator, denoted as . Conventionally, these two types of evolutions exhibit distinct dynamical behaviors. However, in this study, we challenge this common belief and demonstrate that the effective non-Hermitian Hamiltonian can accurately represent the long-term dynamics of a critical two-level open quantum system. The criticality of the system arises from the exceptional point (EP) of the effective non-Hermitian Hamiltonian. Additionally, the NESS is identical to the coalescent state of the effective…
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