ArXiv TLDR

Revealing the physical structure of the general quantum master equation

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2604.14382

Eugenia Pyurbeeva, Ronnie Kosloff

quant-phcond-mat.mes-hallcond-mat.stat-mech

TLDR

General quantum dynamics can be expressed through free evolution, generalized charge exchanges, and pure dephasing, revealing a novel physical structure.

Key contributions

  • Reveals the physical structure of the general quantum master equation without assumptions.
  • Shows general quantum dynamics as free evolution, generalized charge exchange, and pure dephasing.
  • Demonstrates strong coupling, particle exchange, and non-Abelian effects share a common origin.
  • Identifies a previously unconsidered non-commutation term in the generalized Gibbs state.

Why it matters

This paper offers a novel, assumption-free perspective on quantum master equations by breaking down dynamics into fundamental physical processes. It unifies various complex quantum phenomena and introduces a crucial new term for generalized Gibbs states, advancing our understanding of open quantum systems.

Original Abstract

The Lindblad (GKLS) master equation, which represents the mathematical form for the general evolution of a density matrix, is a versatile and widely-used tool in open quantum systems. In contrast with the typical approach of imposing additional conditions on the system, such as weak coupling or energy conservation, we explore the structure of the equation with no assumptions. We demonstrate that general quantum dynamics can be expressed through a combination of free evolution, exchanges of some physical quantities (generalised charges), not necessarily commuting with the Hamiltonian, between the system and the bath, and pure dephasing. This result comprises a novel perspective on quantum master equations, employing physical processes as elemental parts. We use it to explore the dynamics and stationary states of a two-level system and show that strong coupling, particle exchange, and non-Abelian effects all share the same physical origin. Moreover, we demonstrate that the generalised Gibbs state for all three cases contains a non-commutation term, which has not been previously considered.

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