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W. Wilkins, Phys. Rev. (to appear). 11. This work was reviewed by D. C. Langreth in Nobel Symposia- Medicine and Natural Sciences, Academic Press, New York and London, Vol. 24, p. 210, 1973. 12. J. T. Yue and S. Doniach, Phys. Rev. B8, 4578 (1973). 13. T. McMullen and B. Bergersen, Can. J. Phys. 1002 (1972). 14. P. Nozi~res and E. Abrahams, Phys. Rev. BlO, 3099 (1974). 15. For the band case where E ~ p /2m see D. Langreth, Phys. Rev. 148,P707 (1966). 16. D. C. Langreth, Phys. Rev. see Eq. (8). 17.

C. Langreth, Phys. Rev. B5, 3512 (1972). 18. J. J. Chang and D. C. Langreth, Bull. Am. Phys. Soc. 18, 55 (1973); Phys. Rev. B8, 4638 (1973). 19. C. Caroli, D. Lederer-Rozenblatt, B. Roulet and S. Saint-James, Phys. Rev. B8, 4552 (1973). 2 ~' C. Lett. J. , Universitaire Installing Antwerpen,Wilrijk,Belgium I. INTRODUCTION In these lectures we shall sketch the philosophy behind nonequilibrium Statistical Physics and illustrate the procedure using an exactly soluble model. We shall concentrate on the question of direct conductivity and mean energy.

Physik 44, 196 (1914). , J. Phys. A6, 1479 (1973). C. , 30, 137 (:1957). , Tables of Integrals, Series and Products, Academic Press, p. 419 (London,1965l. ASPECTS OF LINEAR AND NONLINEAR ELECTRONIC CONDUCTION IN DISSIPATIVE MEDIA K. K. A. ABSTRACT We review a general approach to the calculation of electronic transport properties under steady-state but nonequilibrium conditions. Of particular interest is the velocity acquired by an electron in a finite electric field in a polar crystal as a (nonlinear) function of the applied electric field.

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