Determination of the critical exponents in dissipative phase transitions: Coherent anomaly approach
arXiv:2103.07255 · doi:10.1103/PhysRevB.104.214301
Abstract
We propose a generalization of the coherent anomaly method to extract the critical exponents of a phase transition occurring in the steady-state of an open quantum many-body system. The method, originally developed by Suzuki [J. Phys. Soc. Jpn. {\bf 55}, 4205 (1986)] for equilibrium systems, is based on the scaling properties of the singularity in the response functions determined through cluster mean-field calculations. We apply this method to the dissipative transverse-field Ising model and the dissipative XYZ model in two dimensions obtaining convergent results already with small clusters.
Accepted version, 9 pages, 7 figures
References in corpus (13)
- Cold atoms in cavity-generated dynamical optical potentials
- Quantum trajectories and open many-body quantum systems
- Dynamical Phase Transitions and Instabilities in Open Atomic Many-Body Systems
- Observation of a dissipative phase transition in a one-dimensional circuit QED lattice
- Neural-Network Approach to Dissipative Quantum Many-Body Dynamics
- Variational Quantum Monte Carlo Method with a Neural-Network Ansatz for Open Quantum Systems
- Variational neural network ansatz for steady states in open quantum systems
- Variational principle for steady states of dissipative quantum many-body systems
- Constructing neural stationary states for open quantum many-body systems
- Universal non-equilibrium properties of dissipative Rydberg gases
- Linked cluster expansions for open quantum systems on a lattice
- Cluster mean-field approximations with the coherent-anomaly-method analysis for the driven pair contact process with diffusion
- Generating function, path integral representation, and equivalence for stochastic exclusive particle systems