The Sixth-Moment Sum Rule For the Pair Correlations of the Two-Dimensional One-Component Plasma: Exact Result

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dc.creatorKalinay, P.
dc.creatorMarkos, P.
dc.creatorSamaj, L.
dc.creatorTravenec, I.
dc.date1999-07-02
dc.date.accessioned2026-07-07T03:13:48Z
dc.date.available2026-07-07T03:13:48Z
dc.descriptionThe system under consideration is a two-dimensional one-component plasma in fluid regime, at density n and at arbitrary coupling Gamma=beta e^2 (e=unit charge, beta = inverse temperature). The Helmholtz free energy of the model, as the generating functional for the direct pair correlation c, is treated in terms of a convergent renormalized Mayer diagrammatic expansion in density. Using specific topological transformations within the bond-renormalized Mayer expansion we prove that the nonzero contributions to the regular part of the Fourier component of c up to the k^2-term originate exclusively from the ring diagrams (unable to undertake the bond-renormalization procedure) of the Helmholtz free energy. In particular, c(k)=-Gamma/k^2 + Gamma/(8 pi n) - k^2/[96(pi n)^2] + O(k^4). This result fixes via the Ornstein-Zernike relation, besides the well-known zeroth-, second- and fourth- moment sum rules, the new six-momnt condition for the truncated pair correlation h, n(pi Gamma n/2)^3 Integral r^6 h(r) d^2 r = 3(Gamma-6)(8-3 Gamma)/4.
dc.description24 pages
dc.identifierhttps://arxiv.org/abs/cond-mat/9907024
dc.identifierhttp://arxiv.org/abs/cond-mat/9907024
dc.identifierJ. Stat. Phys. 98 (2000) 639
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/29443
dc.subjectStatistical Mechanics
dc.titleThe Sixth-Moment Sum Rule For the Pair Correlations of the Two-Dimensional One-Component Plasma: Exact Result
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