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Volumn 60, Issue 17, 1999, Pages 12045-12050

High-permittivity ionic glass predicted from mode-coupling calculations

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EID: 0038673666     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.60.12045     Document Type: Article
Times cited : (6)

References (25)
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    • North-Holland, Amsterdam J. Zinn-Justin J.P. Hansen D. Levesque
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    • (1991) Liquids, Freezing, and the Glass Transition , vol.1 , pp. 287
    • Götze, W.1
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    • Materials Research Society, Pittsburgh MRS Symposia Proceedings No. 407 H.E. Stanley D.L. Johnson D.J. Durian H.Z. Cummins
    • M. Fuchs, in Disordered Materials and Interfaces, edited by H.Z. Cummins, D.J. Durian, D.L. Johnson, and H.E. Stanley,MRS Symposia Proceedings No. 407 (Materials Research Society, Pittsburgh, 1996).
    • (1996) Disordered Materials and Interfaces
    • Fuchs, M.1
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    • 85037893027 scopus 로고    scopus 로고
    • L.D. Landau and E.M. Lifschitz, Statistische Physik, Lehrbuch der Theoretischen Physik Vol. 5 (Akademie-Verlag, Berlin, 1971).
    • L.D. Landau and E.M. Lifschitz, Statistische Physik, Lehrbuch der Theoretischen Physik Vol. 5 (Akademie-Verlag, Berlin, 1971).
  • 25
    • 85037890712 scopus 로고    scopus 로고
    • Since there is a delicate cancellation of the (Formula presented) terms in the numerator and in the denominator of Eq. (14), we checked our extrapolation results by an alternative method of calculation. Inserting (Formula presented) and (Formula presented) into Eq. (14) and taking the zero-wave-number limit, we find from Eq. (13) an expression for (Formula presented) in terms of the coefficient matrices stf, and g, which is easily evaluated, once the expansion coefficients have been determined by fitting. The values of ε derived via either route for representative thermodynamic states differed by less than 10%.
    • Since there is a delicate cancellation of the (Formula presented) terms in the numerator and in the denominator of Eq. (14), we checked our extrapolation results by an alternative method of calculation. Inserting (Formula presented) and (Formula presented) into Eq. (14) and taking the zero-wave-number limit, we find from Eq. (13) an expression for (Formula presented) in terms of the coefficient matrices s, t, f, and g, which is easily evaluated, once the expansion coefficients have been determined by fitting. The values of ε derived via either route for representative thermodynamic states differed by less than 10%.


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