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Polylogarithm Identities in a Conformal Field Theory in Three Dimensions

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arxiv hep-th/9305131 v1 pith:76ULKBO2 submitted 1993-05-25 hep-th cond-mat

classification hep-thcond-mat
keywords theorytildeconformalidentitiesresultcitedimensionsfield
verification ladder T0 review T1 audit T2 compute T3 formal

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abstract

The $N=\infty$ vector $O(N)$ model is a solvable, interacting field theory in three dimensions ($D$). In a recent paper with A. Chubukov and J. Ye~\cite{self}, we have computed a universal number, $\tilde{c}$, characterizing the size dependence of the free energy at the conformally-invariant critical point of this theory. The result~\cite{self} for $\tilde{c}$ can be expressed in terms of polylogarithms. Here, we use non-trivial polylogarithm identities to show that $\tilde{c}/N = 4/5$, a rational number; this result is curiously parallel to recent work on dilogarithm identities in $D=2$ conformal theories. The amplitude of the stress-stress correlator of this theory, $c$ (which is the analog of the central charge), is determined to be $c/N=3/4$, also rational. Unitary conformal theories in $D=2$ always have $c = \tilde{c}$; thus such a result is clearly not valid in $D=3$.

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Cited by 3 Pith papers

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  1. CFTs on Squashed Spheres and the Thermal Effective Action

    hep-th 2026-06 unverdicted novelty 7.0 of 10

    Derives universal quadratic response of 3D CFT free energy to S^3 squashing proportional to c_T and constructs thermal effective action for high-T Seifert manifolds with explicit Wilson coefficients.

  2. The large $N$ vector model on $S^1\times S^2$

    hep-th 2024-11 conditional novelty 6.0 of 10

    The authors compute the leading finite-size corrections to thermal observables of the large-N critical O(N) model on S^1 x S^2 using a perturbative expansion in beta/r.

  3. Boulder Lectures on Thermal Dynamics and Hydrodynamic EFTs

    hep-th 2026-06 unverdicted novelty 2.0 of 10

    Lectures summarizing the construction of hydrodynamic EFTs through strong-to-weak symmetry breaking, with examples from spin chains to relativistic QFTs and UV/IR constraints on transport coefficients.

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