# Normal Typicality and von Neumann's Quantum Ergodic Theorem

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Sheldon Goldstein, Jul 28, 2015 Available from:-
- "Several papers with interesting discussions about this work appeared recently (see for instance [1], [2] and other papers which mention these two) "

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**ABSTRACT:**We present a simplified proof of the von Neumann's Quantum Ergodic Theorem. This important result was initially published in german by J. von Neumann in 1929. We are interested here in the time evolution $\psi_t$, $t\geq 0$, (for large times) under the Schrodinger equation associated to a given fixed Hamiltonian $H : \mathcal{H} \to \mathcal{H}$ and a general initial condition $\psi_0$. The dimension of the Hilbert space $\mathcal{H}$ is finite. -
- "This implies the same behavior for an arbitrary ρ(0). This behavior of isolated, macroscopic quantum systems is an instance of a phenomenon we call normal typicality [5], a version of which is expressed in von Neumann's quantum ergodic theorem [17]. However, our result falls outside the scope of von Neumann's theorem, because of the technical assumptions made in that theorem. "

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**ABSTRACT:**We consider an isolated macroscopic quantum system. Let H be a microcanonical "energy shell," i.e., a subspace of the system's Hilbert space spanned by the (finitely) many energy eigenstates with energies between E and E+deltaE . The thermal equilibrium macrostate at energy E corresponds to a subspace H(eq) of H such that dim H(eq)/dim H is close to 1. We say that a system with state vector psi is the element of H is in thermal equilibrium if psi is "close" to H(eq). We show that for "typical" Hamiltonians with given eigenvalues, all initial state vectors psi(0) evolve in such a way that psi(t) is in thermal equilibrium for most times t. This result is closely related to von Neumann's quantum ergodic theorem of 1929.Physical Review E 01/2010; 81(1 Pt 1):011109. DOI:10.1103/PhysRevE.81.011109 · 2.33 Impact Factor -
- "Recently there has been significant progress in understanding the fundamental principles of statistical mechanics [1] [2] [3] [4] [5] [6] [7] [8]. Underlying this progress is the realization that quantum mechanics allows individual quantum states to exhibit statistical properties, and that ensemble or time averages are not needed to obtain a mixed equilibrium state for the system under consideration . "

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**ABSTRACT:**We study the speed of fluctuation of a quantum system around its thermodynamic equilibrium state, and show that the speed will be extremely small for almost all times in typical thermodynamic cases. The setting considered here is that of a quantum system couples to a bath, both jointly described as a closed system. This setting, is the same as the one considered in [N. Linden et al., Phys. Rev. E 79:061103 (2009)] and the ``thermodynamic equilibrium state'' refers to a situation that includes the usual thermodynamic equilibrium case, as well as far more general situations.New Journal of Physics 07/2009; DOI:10.1088/1367-2630/12/5/055021 · 3.67 Impact Factor