An Information-Theoretic Measure of Uncertainty due to Quantum and Thermal Fluctuations

Details An Information-Theoretic Measure of Uncertainty due to Quantum and Thermal Fluctuations An Information-Theoretic Measure of Uncertainty due to Quantum and Thermal Fluctuations

1993-04-18

arxiv.org/abs/gr-qc/9304025v3

Phys.Rev. D48 (1993) 2753-2765

Astronomy and Astrophysics

Astrophysics

General Relativity and Quantum Cosmology

36 pages (revised uncorrupted version), Report IC 92-93/25

Scientific paper

10.1103/PhysRevD.48.2753

We study an information-theoretic measure of uncertainty for quantum systems. It is the Shannon information $I$ of the phase space probability distribution $\la z | \rho | z \ra $, where $|z \ra $ are coherent states, and $\rho$ is the density matrix. The uncertainty principle is expressed in this measure as $I \ge 1$. For a harmonic oscillator in a thermal state, $I$ coincides with von Neumann entropy, $- \Tr(\rho \ln \rho)$, in the high-temperature regime, but unlike entropy, it is non-zero at zero temperature. It therefore supplies a non-trivial measure of uncertainty due to both quantum and thermal fluctuations. We study $I$ as a function of time for a class of non-equilibrium quantum systems consisting of a distinguished system coupled to a heat bath. We derive an evolution equation for $I$. For the harmonic oscillator, in the Fokker-Planck regime, we show that $I$ increases monotonically. For more general Hamiltonians, $I$ settles down to monotonic increase in the long run, but may suffer an initial decrease for certain initial states that undergo ``reassembly'' (the opposite of quantum spreading). Our main result is to prove, for linear systems, that $I$ at each moment of time has a lower bound $I_t^{min}$, over all possible initial states. This bound is a generalization of the uncertainty principle to include thermal fluctuations in non-equilibrium systems, and represents the least amount of uncertainty the system must suffer after evolution in the presence of an environment for time $t$.

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