Dissipation induced extended-localized transition

Abstract

Mobility edge (ME), representing the critical energy that distinguishes between extended and localized states, is a key concept in understanding the transition between extended (metallic) and localized (insulating) states in disordered and quasiperiodic systems. Here we explore the impact of dissipation on a quasiperiodic system featuring MEs by calculating steady-state density matrix and analyzing quench dynamics with sudden introduction of dissipation, and demonstrate that dissipation can lead the system into specific states predominantly characterized by either extended or localized states, irrespective of the initial state. Our results establish the use of dissipation as a new avenue for inducing transitions between extended and localized states, and for manipulating dynamic behaviors of particles.

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Cited by in corpus (17)

• Universal non-Hermitian transport in disordered systems
• Emergent Continuous Time Crystal in Dissipative Quantum Spin System without Driving
• The fundamental localization phases in quasiperiodic systems: A unified framework and exact results
• Hidden self-duality and exact mobility edges in quasiperiodic network models
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• Exploring Multifractal Critical Phases in Two-Dimensional Quasiperiodic Systems
• Dissipation induced transition between delocalization and localization in the three-dimensional Anderson model
• Manipulating the Relaxation Time of Boundary-Dissipative Systems through Bond Dissipation
• Emergence of the Gibbs ensemble as a steady state in Lindbladian dynamics
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• Digital Quantum Simulation of the Lindblad Master Equation and Its Nonlinear Extensions via Quantum Trajectory Averaging
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• Supercorrelated decay in a quasiperiodic nonlinear waveguide: From Markovian to non-Markovian transitions
• Dissipation-Driven Transition of Particles from Dispersive to Flat Bands