Characterizing the Yang-Lee zeros of the classical Ising model through dynamic quantum phase transitions
arXiv:2412.07800 · doi:10.1103/PhysRevA.111.042204
Abstract
In quantum dynamics, the Loschmidt amplitude is analogous to the partition function in the canonical ensemble. Zeros in the partition function indicate a phase transition, while the presence of zeros in the Loschmidt amplitude indicates a dynamical quantum phase transition. Based on the classical-quantum correspondence, we demonstrate that the partition function of a classical Ising model is equivalent to the Loschmidt amplitude in non-Hermitian dynamics, thereby mapping an Ising model with variable system size to the non-Hermitian dynamics. It follows that the Yang-Lee zeros and the Yang-Lee edge singularity of the classical Ising model correspond to the critical times of the dynamic quantum phase transitions and the exceptional point of the non-Hermitian Hamiltonian, respectively. Our work reveals an inner connection between Yang-Lee zeros and non-Hermitian dynamics, offering a dynamic characterization of the former.
References in corpus (10)
- Making Sense of Non-Hermitian Hamiltonians
- The physics of exceptional points
- Observation of Lee-Yang zeros
- Lee-Yang theory of criticality in interacting quantum many-body systems
- Entanglement Dynamics in Anti--Symmetric Systems
- Experimental observation of the Yang-Lee quantum criticality in open systems
- Infinite cascades of phase transitions in the classical Ising chain
- Dynamical signatures of the Yang-Lee edge singularity in non-Hermitian systems
- Yang-Lee Zeros in Quantum Phase Transition: An Entanglement Perspective
- Synthetic topology and Floquet dynamic quantum phase transition in a periodically driven Raman lattice