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0041477866
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Note that a band of negative ε(k) was first obtained in a computer simulation of molten salts [A. Fasolino, M. Parinello and M. P. Tosi, Phys. Lett. 66A, 119 (1978); M. Rovere, R. Miniero, M. Parinello and M. P. Tosi, Phys. Chem. Liq. 9, 11 (1979)].
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Note that a band of negative ε(k) was first obtained in a computer simulation of molten salts [A. Fasolino, M. Parinello and M. P. Tosi, Phys. Lett. 66A, 119 (1978); M. Rovere, R. Miniero, M. Parinello and M. P. Tosi, Phys. Chem. Liq. 9, 11 (1979)].
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0041810331
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note
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Apart from the nominator in equation (15), which affects the asymptotic law at high k, the second contribution to the medium response, χ2(k), coincides with the approximation suggested in [26] on the basis of oscillating spatial correlation functions for polarization fluctuations.
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33
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0000940720
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A. K. Soper, J. Chem. Phys. 101, 6888 (1994); A. K. Soper and J. Turner, Int. J. Mod. Phys. B7, 3049 (1993).
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Soper, A.K.1
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35
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0042812226
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note
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-1 only three data points for ε(k) were available. A decisive conclusion may only be drawn from computer simulations using larger molecular systems, in order to get a better resolution in k-space (the interval on the k-axis is given by Δk = 2π/L, which also determines the smallest wave number, accessible by simulation. L is the length of the simulation box).
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36
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0041309678
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note
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The phase shift of the oscillations is due to a changing effective radius of the ion, ie due to conservation of the absolute value of the amount of charge, the center of mass of the charge distribution moves to larger radii.
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38
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0010884753
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R. A. Marcus, J. Chem. Phys. 24, 966 (1956); R. A. Marcus, Disc. Faraday. Soc. 29, 21 (1960).
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R. A. Marcus, J. Chem. Phys. 24, 966 (1956); R. A. Marcus, Disc. Faraday. Soc. 29, 21 (1960).
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Marcus, R.A.1
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0039549328
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R. R. Dogonadze, A. A. Kornyshev and A. M. Kuznetsov, Tear. Mat. Fiz. 15, 127 (1973); Theoret. Math. Phys. (USSR), 15, 407 (1973).
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Dogonadze, R.R.1
Kornyshev, A.A.2
Kuznetsov, A.M.3
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41
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0041810330
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R. R. Dogonadze, A. A. Kornyshev and A. M. Kuznetsov, Tear. Mat. Fiz. 15, 127 (1973); Theoret. Math. Phys. (USSR), 15, 407 (1973).
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43
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84906361028
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The result, formally the same as that of the Lorentzian model, was obtained for the dipole orientational part of E, within the framework of a molecular theory of the hard sphere dipolar liquid: D. V. Matyushov, Mol. Phys. 79, 795 (1993).
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Mol. Phys.
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Matyushov, D.V.1
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44
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0041810332
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note
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In associated liquids the role of the scalar order parameter may be played by the density of hydrogen bonds.
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45
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0042812227
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note
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Of course, there are no harmonically varying static electric fields in nature. However, the field produced by an ion may be described as a superposition of sinusoidal fields with different wavelengths (harmonic analysis), to which the surrounding medium (solvent) will respond.
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