Do mixed states exhibit deep thermalisation?
- URL: http://arxiv.org/abs/2507.14135v1
- Date: Fri, 18 Jul 2025 17:59:02 GMT
- Title: Do mixed states exhibit deep thermalisation?
- Authors: Alan Sherry, Sthitadhi Roy,
- Abstract summary: We introduce a new paradigm of deep thermalisation for mixed states, fundamentally distinct from that for pure-state ensembles.<n>We demonstrate such ensembles emerge dynamically in generic, locally interacting chaotic systems.<n>Our results lead to fundamental insights into how maximum entropy principles and deep thermalisation manifest themselves in unitary dynamics of states with finite entropy.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: The notion of $deep$ $thermalisation$, where ensembles of pure states on a local subsystem, conditioned on measurement outcomes on its complement, approach universal maximum-entropy ensembles constrained only by conservation laws, represents a stronger form of ergodicity than conventional thermalisation. We show that this framework fails dramatically for mixed initial states, evolved unitarily, even with infinitesimal initial mixedness. To address this, we introduce a new paradigm of deep thermalisation for mixed states, fundamentally distinct from that for pure-state ensembles. In our formulation, the deep thermal ensemble arises by tracing out auxiliary degrees of freedom from a maximum-entropy ensemble defined on an augmented system, with the ensemble structure depending explicitly on the entropy of the initial state. We demonstrate that such ensembles emerge dynamically in generic, locally interacting chaotic systems. For the self-dual kicked Ising chain, which we show to be exactly solvable for a class of mixed initial states, we find exact emergence of the so-defined mixed-state deep thermal ensemble at finite times. Our results therefore lead to fundamental insights into how maximum entropy principles and deep thermalisation manifest themselves in unitary dynamics of states with finite entropy.
Related papers
- Thermal state preparation by repeated interactions at and beyond the Lindblad limit [41.94295877935867]
We study the nature of thermalization dynamics and the associated preparation (simulation) time under the repeated interaction protocol.<n>We observe a Mpemba-like effect: Starting from a maximally mixed state, thermalization to an intermediate-temperature state takes longer than to a lower-temperature one.
arXiv Detail & Related papers (2025-06-13T18:34:49Z) - Symmetries, Conservation Laws and Entanglement in Non-Hermitian Fermionic Lattices [37.69303106863453]
Non-Hermitian quantum many-body systems feature steady-state entanglement transitions driven by unitary dynamics and dissipation.<n>We show that the steady state is obtained by filling single-particle right eigenstates with the largest imaginary part of the eigenvalue.<n>We illustrate these principles in the Hatano-Nelson model with periodic boundary conditions and the non-Hermitian Su-Schrieffer-Heeger model.
arXiv Detail & Related papers (2025-04-11T14:06:05Z) - Thermodynamic Roles of Quantum Environments: From Heat Baths to Work Reservoirs [49.1574468325115]
Environments in quantum thermodynamics usually take the role of heat baths.
We show that within the same model, the environment can take three different thermodynamic roles.
The exact role of the environment is determined by the strength and structure of the coupling.
arXiv Detail & Related papers (2024-08-01T15:39:06Z) - A Maximum Entropy Principle in Deep Thermalization and in Hilbert-Space Ergodicity [3.404409295403274]
We report universal statistical properties displayed by ensembles of pure states that naturally emerge in quantum many-body systems.
Our results generalize the notions of Hilbert-space ergodicity to time-independent Hamiltonian dynamics and deep thermalization.
arXiv Detail & Related papers (2024-03-18T17:09:04Z) - Nonlocality of Deep Thermalization [0.0]
We study the role of global system topology in governing deep thermalization.<n>Deep thermalization is achieved exponentially quickly in the presence of either periodic or open boundary conditions.
arXiv Detail & Related papers (2023-05-15T08:32:05Z) - Generalized Deep Thermalization for Free Fermions [0.0]
In non-interacting isolated quantum systems out of equilibrium, local subsystems typically relax to non-thermal stationary states.
In the standard framework, information on the rest of the system is discarded, and such states are described by a Generalized Gibbs Ensemble (GGE)
Here we show that the latter also completely characterize a recently introduced projected ensemble (PE), constructed by performing projective measurements on the rest of the system.
arXiv Detail & Related papers (2022-07-27T16:43:19Z) - Quantum coherence controls the nature of equilibration in coupled
chaotic systems [0.0]
Quantum coherence of the initial product states in the uncoupled eigenbasis can be viewed as a resource for equilibration and approach to thermalization.
Results are given for four distinct perturbation strength regimes, the ultra-weak, weak, intermediate, and strong regimes.
Maximally coherent initial states thermalize for any perturbation strength in spite of the fact that in the ultra-weak perturbative regime the underlying eigenstates of the system have a tensor product structure and are not at all thermal-like.
arXiv Detail & Related papers (2022-04-15T17:33:44Z) - Maximum entropy quantum state distributions [58.720142291102135]
We go beyond traditional thermodynamics and condition on the full distribution of the conserved quantities.
The result are quantum state distributions whose deviations from thermal states' get more pronounced in the limit of wide input distributions.
arXiv Detail & Related papers (2022-03-23T17:42:34Z) - Fast Thermalization from the Eigenstate Thermalization Hypothesis [69.68937033275746]
Eigenstate Thermalization Hypothesis (ETH) has played a major role in understanding thermodynamic phenomena in closed quantum systems.
This paper establishes a rigorous link between ETH and fast thermalization to the global Gibbs state.
Our results explain finite-time thermalization in chaotic open quantum systems.
arXiv Detail & Related papers (2021-12-14T18:48:31Z) - Open-system approach to nonequilibrium quantum thermodynamics at
arbitrary coupling [77.34726150561087]
We develop a general theory describing the thermodynamical behavior of open quantum systems coupled to thermal baths.
Our approach is based on the exact time-local quantum master equation for the reduced open system states.
arXiv Detail & Related papers (2021-09-24T11:19:22Z) - Uhlmann Fidelity and Fidelity Susceptibility for Integrable Spin Chains
at Finite Temperature: Exact Results [68.8204255655161]
We show that the proper inclusion of the odd parity subspace leads to the enhancement of maximal fidelity susceptibility in the intermediate range of temperatures.
The correct low-temperature behavior is captured by an approximation involving the two lowest many-body energy eigenstates.
arXiv Detail & Related papers (2021-05-11T14:08:02Z) - Emergent eigenstate solution for generalized thermalization [5.122644673465354]
We study the emergent eigenstate that describes the quantum dynamics of hard-core bosons in one dimension (1D)
Specifically, we study the emergent eigenstate that describes the quantum dynamics of hard-core bosons in one dimension (1D)
arXiv Detail & Related papers (2021-03-08T19:00:04Z) - Exact many-body scars and their stability in constrained quantum chains [55.41644538483948]
Quantum scars are non-thermal eigenstates characterized by low entanglement entropy.
We study the response of these exact quantum scars to perturbations by analysing the scaling of the fidelity susceptibility with system size.
arXiv Detail & Related papers (2020-11-16T19:05:50Z)
This list is automatically generated from the titles and abstracts of the papers in this site.
This site does not guarantee the quality of this site (including all information) and is not responsible for any consequences.