Zero distribution conjecture for the second-largest spinless-fermion eigenvalue

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Let p0∈2Zp_0\in 2\mathbb{Z}, and let Tn−1(2)(v)T^{(2)}_{n-1}(v) denote the corresponding fused transfer-matrix eigenvalue for the second-largest eigenvalue in the sector Ne=N/2−1N_{\rm e}=N/2-1. The physical strip is Im⁡v∈[−1,1]\operatorname{Im}v\in[-1,1].

Zero distribution conjecture. Tn−1(2)(v)T^{(2)}_{n-1}(v) has one real zero ζn−1\zeta_{n-1} for nn even with 2≤n≤p0−12\leq n\leq p_0-1, and two real zeros ζn−1\zeta_{n-1} and −ζn−1′-\zeta'_{n-1} for nn odd with 2<n<p0/22<n<p_0/2. All other zeros are outside the physical strip.

This conjecture describes the analyticity pattern needed to derive the nonlinear integral equations for the second-largest eigenvalue. It is based on numerical studies, and the supplied passage gives no resolution beyond that numerical evidence.

References

Primary source

Kazumitsu Sakai, “Excited state TBA and functional relations in spinless Fermion model”, arXiv:cond-mat/9903112 (1999).

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