Polynomial-coefficient conjecture for the difference of special-boundary transfer-matrix eigenvalues

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Let mm be the lattice-width parameter, let qq be the Potts-model state parameter, and let λ⋆,=(m)\lambda_{\star,=}(m) and λ⋆,≠(m)\lambda_{\star,\neq}(m) denote the dominant transfer-matrix eigenvalues for the == and ≠\neq boundary conditions, respectively. For each positive integer ℓ\ell, let DℓD_\ell be a polynomial in mm. Polynomial-coefficient conjecture. There exist polynomials D1,D2,…D_1,D_2,\ldots with rational coefficients, with deg⁡Dℓ=ℓ\deg D_\ell=\ell, such that

λ⋆,=(m)−λ⋆,≠(m)=(−1)m+1[1+∑ℓ=1m−1(−1)ℓDℓ(m)q−ℓ]+O(q−m).\lambda_{\star,=}(m)-\lambda_{\star,\neq}(m)=(-1)^{m+1}\left[1+\sum_{\ell=1}^{m-1}(-1)^\ell D_\ell(m)q^{-\ell}\right]+O(q^{-m}).

This conjecture formalizes the empirical observation that the coefficients in the asymptotic expansion of the eigenvalue difference are polynomial in mm, with the coefficient at order q−ℓq^{-\ell} having degree exactly ℓ\ell. The authors report verification for the corresponding computations discussed in the paper; the general assertion remains open.

References

Primary source

Jesús Salas and Alan D. Sokal, “Transfer matrices and partition-function zeros for antiferromagnetic Potts models. VI. Square lattice with special boundary conditions”, arXiv:1002.3761 (2011).

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