On the propagator related to an electron in a random potential

The authors provide physical and mathematical reasons by which propagators associated with non-local actions may not satisfy the composition property and may not be of the Van Vleck-Pauli formula either. Furthermore, they demonstrate that the Feynman and Schwinger principles, at least when applied to non-local quadratic actions, yield identical formulae. Via these formulae, they calculate the propagator associated with the action which is related to an electron gas in a random potential.

[1]  John R. Klauder,et al.  Path integrals from meV to MeV , 1989 .

[2]  D. Castrigiano,et al.  Radiation damping of a quantum harmonic oscillator , 1987 .

[3]  Weiss,et al.  Quantum decay rates for dissipative systems at finite temperatures. , 1987, Physical review. B, Condensed matter.

[4]  A. Nassar,et al.  Space-time-transformation technique in connection with the Schwinger action principle , 1987 .

[5]  A. Leggett,et al.  Dynamics of the dissipative two-state system , 1987 .

[6]  J. Bassalo,et al.  On the use of spacetime transformations in path integration , 1986 .

[7]  P. Hänggi Addendum and erratum , 1986 .

[8]  S. V. Lawande,et al.  Feynman path integrals: Some exact results and applications , 1986 .

[9]  Bhagwat,et al.  Functional integral approach to positionally disordered systems. , 1986, Physical review. B, Condensed matter.

[10]  B. Cheng,et al.  Path integration of the time-dependent forced oscillator with a two-time quadratic action , 1986 .

[11]  P. Hänggi Escape from a Metastable State , 1986 .

[12]  F. Zertuche,et al.  On the Pauli-Van Vleck formula for arbitrary quadratic systems with memory in one dimension , 1985 .

[13]  S. V. Lawande,et al.  Path integration of a two-time quadratic action , 1983 .

[14]  E. Bosco Comment on “path integration of a quadratic action with a generalized memory , 1983 .

[15]  S. V. Lawande,et al.  Path integration of an action related to an electron gas in a random potential , 1983 .

[16]  S. V. Lawande,et al.  Path integration of a quadratic action with a generalized memory , 1983 .

[17]  S. V. Lawande,et al.  Path integration of a Lagrangian related to an electron gas in a random potential , 1981 .

[18]  A. Maheshwari Comment on 'exact evaluation of a path integral relating to an electron gas in a random potential' , 1975 .

[19]  G. Papadopoulos Exact evaluation of a path integral relating to an electron gas in a random potential , 1974 .

[20]  V. Bezák The partition sum of an ideal gas in a random potential , 1971 .

[21]  V. Bezák Path-integral theory of an electron gas in a random potential , 1970, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.