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arXiv:hep-th/9508076 · Nuclear Physics B

Generalized quantum dynamics as pre-quantum mechanics

Stephen L. Adler, Andrew C. Millard

Published Aug 1, 1996• 53 citations
arXivHTMLPDF
DOI
10.1016/0550-3213(96)00253-2

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Generalized quantum dynamics as pre-quantum mechanics

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We address the issue of when generalized quantum dyanmics, based on a total trace Hamiltonian {\\bf H}, reduces to Heisenberg picture complex quantum mechanics. We begin by showing that when {\\bf H}={\\rm{\\bf Tr}} H_{OP}, with H_{OP} a Weyl ordered operator Hamiltonian, then the generalized quantum dynamics operator equations of motion agree with those obtained from H_{OP} in the Heisenberg picture by using canonical commutation relations. Hence generalized quantum dynamics conicides with complex quantum mechanics in this case, provided the initial values of the operators obey the canonical algebra. The remainder of the paper is devoted to a study of when this initial value condition is satisfied. We first show that for any total trace Hamiltonian which involves no noncommutative constants, there is a conserved operator \\tilde C which is closely related to the canonical algebra. We demonstrate that for a system in equilbrium, the equilbrium ensemble of initial values is governed by the distribution exp(-|\\tilde C|/\\kappa). An argument analogous to that for equipartition of energy, together with the assumption that ensemble averages of products can be replaced by products of ensemble averages, then implies that the ensemble averaged operator initial values obey the standard canonical commutation relations of complex quantum mechanics, with the imaginary unit I identified as -\\tilde C / |\\tilde C|, and with the constant \\kappa playing the role of the reduced Planck constant \\hbar. Thus there is a well--defined sense in which complex quantum mechanics and quantum field theory emerge as a statistical approximation to generalized quantum dynamics.

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Generalized quantum dynamics

Stephen L. Adler

arXiv:hep-th/9306009•Nuclear Physics B•Feb 1, 1994•85 citations
We propose an alternate version of the "shadow world" hypothesis for the origin of dark matter. Instead of postulating that the shadow world is a "mirror" world under parity or charge-parity reflection, we suggest that the existence of a shadow world arises from the fact that i or –i can be the imaginary unit in complex quantum mechanics. This mechanism is a natural consequence of "trace dynamics" pre-quantum theory, from which quantum mechanics over the complex number field emerges as a statistical mechanical approximation. Because the pre-quantum dynamics does not pick out a preferred imaginary unit, the emergent quantum dynamics contains two sectors, one based on i and the other on –i, with both sectors coupled to gravity.
In this work a connection between dynamical quantum mechanical systems and scalar quantum field theory is built. Is verified that the Covariance Matrixs determinant is a time conserved quantity for Gaussian Systems under non autonomous Hamiltonians, and the generalizations for N and infinity dimensions is presented. Two cosmological models for the pre-heating period are treated, and a close connection between the Wigner function, squeezing and particle creation is found. A geometrical interpretation for the dynamics of the pre-heating is made possible, just as a experimental set up for testing cosmological hypothesis.
We address the issue of when generalized quantum dyanmics, based on a total trace Hamiltonian {\\bf H}, reduces to Heisenberg picture complex quantum mechanics. We begin by showing that when {\\bf H}={\\rm{\\bf Tr}} H_{OP}, with H_{OP} a Weyl ordered operator Hamiltonian, then the generalized quantum dynamics operator equations of motion agree with those obtained from H_{OP} in the Heisenberg picture by using canonical commutation relations. Hence generalized quantum dynamics conicides with complex quantum mechanics in this case, provided the initial values of the operators obey the canonical algebra. The remainder of the paper is devoted to a study of when this initial value condition is satisfied. We first show that for any total trace Hamiltonian which involves no noncommutative constants, there is a conserved operator \\tilde C which is closely related to the canonical algebra. We demonstrate that for a system in equilbrium, the equilbrium ensemble of initial values is governed by the distribution exp(-|\\tilde C|/\\kappa). An argument analogous to that for equipartition of energy, together with the assumption that ensemble averages of products can be replaced by products of ensemble averages, then implies that the ensemble averaged operator initial values obey the standard canonical commutation relations of complex quantum mechanics, with the imaginary unit I identified as -\\tilde C / |\\tilde C|, and with the constant \\kappa playing the role of the reduced Planck constant \\hbar. Thus there is a well--defined sense in which complex quantum mechanics and quantum field theory emerge as a statistical approximation to generalized quantum dynamics.