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We would like to demonstrate statistical laws with minimal external randomness. Hence we think of an isolated system left to evolve with no contact with thermal reservoirs of any kind, since we would like to inspect how nonlinear interaction alone can control the ergodic properties of dynamics
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We would like to demonstrate statistical laws with minimal external randomness. Hence we think of an isolated system left to evolve with no contact with thermal reservoirs of any kind, since we would like to inspect how nonlinear interaction alone can control the ergodic properties of dynamics.
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For example, one may generally take (Formula presented) to be a a strong limit of trigonometric polynomials, (Formula presented), such as are the projection operators (Formula presented) according to the spectral theorem for unitary operators 11
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For example, one may generally take (Formula presented) to be a a strong limit of trigonometric polynomials, (Formula presented), such as are the projection operators (Formula presented) according to the spectral theorem for unitary operators 11.
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Precise conditions on the “generic” class of interactions are yet to be determined; here we show the conjecture for a particular specific example and quote few other results (Sec. VI). However, we should stress that we have in mind only purely deterministic systems and nonrandom interactions, so Hamiltonians (Formula presented) of infinite systems are supposed to be prescribed using a finite amount of information
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Precise conditions on the “generic” class of interactions are yet to be determined; here we show the conjecture for a particular specific example and quote few other results (Sec. VI). However, we should stress that we have in mind only purely deterministic systems and nonrandom interactions, so Hamiltonians (Formula presented) of infinite systems are supposed to be prescribed using a finite amount of information.
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A simpler and perhaps more powerful version of the method for autonomous Hamiltonian systems, which may be used also to give rigorous upper bounds on charge or spin stiffness, etc., will be presented elsewhere
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A simpler and perhaps more powerful version of the method for autonomous Hamiltonian systems, which may be used also to give rigorous upper bounds on charge or spin stiffness, etc., will be presented elsewhere.
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