Square-lattice toroidal phase-diagram conjecture

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For a zero-temperature square-lattice Potts antiferromagnet on toroidal strips, let qq be the Potts parameter, let q0(L)q_0(L) be the relevant real crossing, and let ℓ\ell denote the number of bridges. Square-lattice phase-diagram conjecture. At real qq, the phases are: (a) q∈(−∞,0)∪(q0(L),∞)q\in(-\infty,0)\cup(q_0(L),\infty), characterized by ℓ=0\ell=0 and amplitude b(0)=1b^{(0)}=1; (b) q∈(0,2)q\in(0,2), characterized by ℓ=1\ell=1 and amplitude b(1)=q−1b^{(1)}=q-1; and (c) q∈(2,q0(L))q\in(2,q_0(L)), characterized by ℓ=2\ell=2 and amplitude b1(2)=q(q−3)/2b^{(2)}_1=q(q-3)/2. The claim summarizes empirical limiting-curve data for widths 2≤L≤122\leq L\leq12, where 2≤q0(L)≤32\leq q_0(L)\leq3; no proof or resolution is given.

References

Primary source

Jesper Lykke Jacobsen and Jesus Salas, “Phase diagram of the chromatic polynomial on a torus”, arXiv:cond-mat/0703228 (2007).

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