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Topological fingerprints in Liouvillian gaps.
K Kavanagh1,2,3, J K Slingerland2,3, S Dooley2,4
1Department of Physics, Faculty of Mathematics and Physics, <a href="https://ror.org/05njb9z20">University of Ljubljana</a>, 1000 Ljubljana, Slovenia.
Topological properties in open quantum systems can be detected through relaxation rates, not just equilibrium states. This study reveals how dissipation affects topological fingerprints in the Kitaev chain model.
Area of Science:
- Condensed Matter Physics
- Quantum Information Theory
- Many-Body Physics
Background:
- Topology in many-body physics is typically associated with equilibrium quantum states.
- Open quantum systems offer a new paradigm for observing topological phenomena.
- The Kitaev chain model serves as a fundamental system with distinct topological phases.
Purpose of the Study:
- To investigate the emergence of topological fingerprints in the relaxation dynamics of open quantum systems.
- To analyze the behavior of the Liouvillian gap in the Kitaev chain model under varying dissipation strengths.
- To establish a connection between topological phases and dissipative properties.
Main Methods:
- Modeling an open quantum system using the Kitaev chain with introduced dissipation.
- Calculating the Liouvillian gap in both strong and weak dissipative regimes.
- Analyzing the influence of superconducting pairing and chemical potential on the Liouvillian gap.
Main Results:
- A non-zero superconducting pairing opens a persistent Liouvillian gap, independent of system size.
- In strong dissipation, the Liouvillian gap is largely insensitive to the Hamiltonian's ground state topology.
- Weak dissipation reveals a crucial role for topology, making the gap immune to chemical potential changes in the topological phase.
Conclusions:
- Topological properties can be imprinted on the relaxation rates of open quantum systems.
- The Liouvillian gap serves as a sensitive indicator of topological phases, particularly under weak dissipation.
- Dissipation provides a tunable knob to probe and potentially control topological states in quantum matter.
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