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WORLD SCIENTIFIC eBooks

Canonical Typicality

Sheldon Goldstein, Joel L. Lebowitz, Roderich Tumulka, Nino Zanghı̀

Published Aug 1, 2025• 0 citations
Publisher
DOI
10.1142/9789819819560_0024

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Canonical Typicality for Other Ensembles than Micro-canonical

Stefan Teufel, Roderich Tumulka, Cornelia Vogel

Abstract We generalize Lévy’s lemma, a concentration-of-measure result for the uniform probability distribution on high-dimensional spheres, to a much more general class of measures, so-called GAP measures. For any given density matrix $$\rho $$ ρ on a separable Hilbert space $${\mathcal {H}}$$ H , $${\textrm{GAP}}(\rho )$$ GAP ( ρ ) is the most spread-out probability measure on the unit sphere of $${\mathcal {H}}$$ H that has density matrix $$\rho $$ ρ and thus forms the natural generalization of the uniform distribution. We prove concentration-of-measure whenever the largest eigenvalue $$\Vert \rho \Vert $$ ‖ ρ ‖ of $$\rho $$ ρ is small. We use this fact to generalize and improve well-known and important typicality results of quantum statistical mechanics to GAP measures, namely canonical typicality and dynamical typicality. Canonical typicality is the statement that for “most” pure states $$\psi $$ ψ of a given ensemble, the reduced density matrix of a sufficiently small subsystem is very close to a $$\psi $$ ψ -independent matrix. Dynamical typicality is the statement that for any observable and any unitary time evolution, for “most” pure states $$\psi $$ ψ from a given ensemble the (coarse-grained) Born distribution of that observable in the time-evolved state $$\psi _t$$ ψ t is very close to a $$\psi $$ ψ -independent distribution. So far, canonical typicality and dynamical typicality were known for the uniform distribution on finite-dimensional spheres, corresponding to the micro-canonical ensemble, and for rather special mean-value ensembles. Our result shows that these typicality results hold also for $${\textrm{GAP}}(\rho )$$ GAP ( ρ ) , provided the density matrix $$\rho $$ ρ has small eigenvalues. Since certain GAP measures are quantum analogs of the canonical ensemble of classical mechanics, our results can also be regarded as a version of equivalence of ensembles.

Annales Henri Poincaré•Jul 2, 2024•7 citations

Canonical transformation

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Canonical Typicality of Energy Eigenstates of an Isolated Quantum System

Anatoly Y. Dymarsky, Hong Liu

Currently there are two main approaches to describe how quantum statistical physics emerges from an isolated quantum many-body system in a pure state: Canonical Typicality (CT) and Eigenstate Thermalization Hypothesis (ETH). These two approaches has different but overlapping areas of validity, phenomenology and set of physical outcomes. In this paper we discuss the relation between CT and ETH and propose a formulation of ETH in terms of the reduced density matrix. We provide strong numerical evidences for the proposal. This article has been withdrawn as it is superseded by arXiv:1611.08764

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The Structure of Typicality

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Quantum thermodynamics and canonical typicality

Paolo Facchi A, Giancarlo Garnero

We present here a set of lecture notes on quantum thermodynamics and canonical typicality. Entanglement can be constructively used in the foundations of statistical mechanics. An alternative version of the postulate of equal a priori probability is derived making use of some techniques of convex geometry.

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Scaling parameter and universality

Antonio Coniglio A

Physica•Apr 1, 1972•17 citations
Abstract We generalize Lévy’s lemma, a concentration-of-measure result for the uniform probability distribution on high-dimensional spheres, to a much more general class of measures, so-called GAP measures. For any given density matrix ρ\rho ρ ρ on a separable Hilbert space H{\mathcal {H}}H H , GAP(ρ){\textrm{GAP}}(\rho )GAP(ρ) GAP ( ρ ) is the most spread-out probability measure on the unit sphere of H{\mathcal {H}}H H that has density matrix ρ\rho ρ ρ and thus forms the natural generalization of the uniform distribution. We prove concentration-of-measure whenever the largest eigenvalue ∥ρ∥\Vert \rho \Vert ∥ρ∥ ‖ ρ ‖ of ρ\rho ρ ρ is small. We use this fact to generalize and improve well-known and important typicality results of quantum statistical mechanics to GAP measures, namely canonical typicality and dynamical typicality. Canonical typicality is the statement that for “most” pure states ψ\psi ψ ψ of a given ensemble, the reduced density matrix of a sufficiently small subsystem is very close to a ψ\psi ψ ψ -independent matrix. Dynamical typicality is the statement that for any observable and any unitary time evolution, for “most” pure states ψ\psi ψ ψ from a given ensemble the (coarse-grained) Born distribution of that observable in the time-evolved state ψt\psi _tψt​ ψ t is very close to a ψ\psi ψ ψ -independent distribution. So far, canonical typicality and dynamical typicality were known for the uniform distribution on finite-dimensional spheres, corresponding to the micro-canonical ensemble, and for rather special mean-value ensembles. Our result shows that these typicality results hold also for GAP(ρ){\textrm{GAP}}(\rho )GAP(ρ) GAP ( ρ ) , provided the density matrix ρ\rho ρ ρ has small eigenvalues. Since certain GAP measures are quantum analogs of the canonical ensemble of classical mechanics, our results can also be regarded as a version of equivalence of ensembles.
Currently there are two main approaches to describe how quantum statistical physics emerges from an isolated quantum many-body system in a pure state: Canonical Typicality (CT) and Eigenstate Thermalization Hypothesis (ETH). These two approaches has different but overlapping areas of validity, phenomenology and set of physical outcomes. In this paper we discuss the relation between CT and ETH and propose a formulation of ETH in terms of the reduced density matrix. We provide strong numerical evidences for the proposal. This article has been withdrawn as it is superseded by arXiv:1611.08764