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Relaxation under conditions of strong interaction

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Abstract

A method is developed for considering a nonequilibrium transition in an isolated system when the correlation time [2] and relaxation time are of the same order. The perturbation V in the Hamiltonian of (1.1) is not restricted in any way. The method is based on the assumption [4] that it is possible to use a representation in which the indeterminacy of the energy of a nonstationary system appears explicitly.

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References

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  2. V. M. Fain, UFN,79, 4, 641, 1963.

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  3. R. Kubo, Lectures in Theoretical Physics, v. 1, New York, 1959.

  4. W. Band, Am. J. Phys.,26, 440, 540, 1958.

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  5. L. I. Mandel'shtam and I. E. Tamm, Izv. AN SSSR, ser. fiz.,9, 122, 1945.

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  6. P. A. M. Dirac, The Principles of Quantum Mechanics [Russian translation], Fizmatgiz, 1961.

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Authors and Affiliations

  1. Moscow Electrotechnical Communications Institute, USSR

    L. P. Ginzburg

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  1. L. P. Ginzburg
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Ginzburg, L.P. Relaxation under conditions of strong interaction. Soviet Physics Journal 10, 71–74 (1967). https://doi.org/10.1007/BF00819994

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  • DOI: https://doi.org/10.1007/BF00819994

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