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Electric Transport in Liquid Metals

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Amorphous Solids and the Liquid State

Part of the book series: Physics of Solids and Liquids ((PSLI))

Abstract

A metal is a two-component system of ions of charge Ze and valence electrons, described by the following Hamiltonian:

$$H = {H_{el}} + {H_{ion}} + {H_{el - ion}}$$
(9.1.1)
$${H_{el}} = \sum\limits_i {\frac{{p_i^2}}{{2m}} + \frac{1}{2}\sum\limits_{i,j} {\frac{{{e^2}}}{{\left| {\left. {{r_i} - {r_j}} \right|} \right.}}} } $$
(9.1.2)
$${H_{ion}} = \sum\limits_n {\frac{{P_n^2}}{{2{M_n}}}} + \frac{1}{2}\sum\limits_{n,m} {\frac{{{{(Ze)}^2}}}{{\left| {\left. {{R_n} - {R_m}} \right|} \right.}}} $$
(9.1.3)
$${H_{el - ion}} = \sum\limits_{i,n} {V({r_i} - {R_n})} + \sum\limits_{i,n} {J({r_i} - {R_n}){\sigma _i} \cdot {S_n}} $$
(9.1.4)

Here and in the following P n , R n , and S n denote ionic momenta, positions, and spins, respectively, while position, momentum, and spin of the i th electron are denoted by r i , p i , and σ i . Before specifying the electron-ion interaction in more detail, we shall outline the aims of a comprehensive theory of liquid metals.

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Beck, H. (1985). Electric Transport in Liquid Metals. In: March, N.H., Street, R.A., Tosi, M.P. (eds) Amorphous Solids and the Liquid State. Physics of Solids and Liquids. Springer, Boston, MA. https://doi.org/10.1007/978-1-4757-9156-3_9

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  • DOI: https://doi.org/10.1007/978-1-4757-9156-3_9

  • Publisher Name: Springer, Boston, MA

  • Print ISBN: 978-1-4757-9158-7

  • Online ISBN: 978-1-4757-9156-3

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