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The term with k = 0 conceals with the terms describing the self-interaction of the compensating background and interaction of the background with particles.
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The ideal-gas cumulants, Eq.(11), may be easily computed using the standard technique; in application to fluids, see, e.g. T. Morita, and K. Hiroike, Progr.Theor.Phys., 25, 537 (1961), or I. R. Yukhnovskii and M. F. Golovko, Statistical Theory of Classical Equilibrium Systems, (in Russian) (Naukova Dumka, Kiev, 1980), where these are explicitely given.
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85153298016
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The self-energy is equal to the energy of interactions of two charges at vanishing distance. This divergency does not affect the final result and may be removed considering the lattice version of the problem [36, 38], or (equivalently) implying an infinitesimally small hard-core for interacting particles.
-
-
-
-
66
-
-
85153205866
-
-
note
-
k* does not reduce the total number of physically different modes, since the modes with the wave-vectors k and -k correspond to that spreading in the opposite directions.
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