Exploring dynamical quantum phase transition from pure states to mixed states through generalized Su-Schrieffer-Heeger models

• URL: http://arxiv.org/abs/2501.06794v1
• Date: Sun, 12 Jan 2025 12:28:34 GMT
• Title: Exploring dynamical quantum phase transition from pure states to mixed states through generalized Su-Schrieffer-Heeger models
• Authors: Kaiyuan Cao, Jian Wang,
• Abstract summary: We investigate dynamic quantum phase transitions (DQPTs) in both pure and mixed states within the framework of the generalized SSH model.<n>We find that the SSH-3 model, characterized by a chiral-like point symmetry rather than true chiral symmetry, supports robust localized edge states associated with its topological properties.<n>For mixed states, DQPT behavior is consistent at low temperatures, but significant changes are observed at high temperatures, resulting in the emergence of multiple critical times.
• Score: 2.301751790183628
• License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
• Abstract: We investigate dynamic quantum phase transitions (DQPTs) in both pure and mixed states within the framework of the generalized SSH model, specifically analyzing the SSH-3 and SSH-4 models, which exhibit different symmetries. We find that the SSH-3 model, characterized by a chiral-like point symmetry rather than true chiral symmetry, supports robust localized edge states associated with its topological properties. Our results show that DQPTs for pure states occur following a quench that crosses the topological transition, even with an open energy band gap. For mixed states, DQPT behavior is consistent at low temperatures, but significant changes are observed at high temperatures, resulting in the emergence of multiple critical times. In contrast, the SSH-4 model, which possesses chiral symmetry, allows for the analysis of two distinct energy spectrum configurations. We conclude that the occurrence of DQPTs for pure states in the SSH-4 model necessitates a quench from an initial state without a band gap while crossing the critical point of the topological transition, whereas DQPTs are absent for mixed states at elevated temperatures.

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