Zero-location conjecture for fused transfer-matrix eigenvalues

Let uu be the parameter of the quantum transfer matrix, let r1r\geq 1, and let a{1,2,,r}a\in\{1,2,\dots,r\} and mZ1m\in\mathbb{Z}_{\geq 1}. Denote by T~m(a)(v)\widetilde{T}^{(a)}_{m}(v) the fused transfer-matrix eigenvalue and by {z~m(a)}\{\tilde{z}^{(a)}_{m}\} its zeros. The chemical potentials are μ1,μ2,,μr+1\mu_1,\mu_2,\dots,\mu_{r+1}. Zero-location conjecture. For small uu (u1|u|\ll 1), every zero {z~m(a)}\{\tilde{z}^{(a)}_{m}\} of T~m(a)(v)\widetilde{T}^{(a)}_{m}(v) is located near the lines

Imv=±m+a2\operatorname{Im}v=\pm\frac{m+a}{2}

at least when μ1=μ2==μr+1=0\mu_1=\mu_2=\dots=\mu_{r+1}=0. This describes the zero pattern underlying the proposed YY-system analysis of the one-string solution; the source provides numerical evidence for the claim, but no proof or resolution is given.

Sources & referencesView supporting material

Primary source

Zengo Tsuboi, “Nonlinear integral equations for thermodynamics of the sl(r+1) Uimin-Sutherland model”, arXiv:cond-mat/0212280 (2002).

Additional references

3 papers in this index state this conjecture (1999–2002). The statement above is taken from the most recent of them; the others are arXiv:math-ph/0209024, arXiv:math-ph/9912014.

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