Conjecture on regular, physical singular, and strange solutions for the spin-5 Heisenberg chain

Let ss be the spin, NN the system size, and ellell the number of Bethe roots. A solution is called regular if it is a regular solution of the Bethe ansatz equations, physical singular if it is a singular solution satisfying the physicality condition, and strange if some components coincide and hence violate the Pauli principle. Define

λ0()=(0,,0),if N1(mod2),\lambda^{(\ell)}_0=(\underbrace{0,\ldots,0}_{\ell}),\qquad \text{if }N\equiv\ell-1\pmod 2,

and

λ±()=(±s,,±s),if N22(mod4).\lambda^{(\ell)}_\pm=(\underbrace{\pm s,\ldots,\pm s}_{\ell}),\qquad \text{if }N\equiv 2\ell-2\pmod 4.

Let Nstrange(N,)\mathcal{N}_{\mathrm{strange}}(N,\ell) and Nsp(N,)\mathcal{N}_{\mathrm{sp}}(N,\ell) denote, respectively, the total numbers of strange and physical singular solutions corresponding to NN and \ell. The conjecture. (1) If 2s1(mod2)2s\equiv1\pmod2, the total number of states consists of regular or physical singular solutions, except possibly for sporadic physical solutions; such solutions do occur, namely λ0(2)\lambda^{(2)}_0 for N=3N=3 and λ±(2)\lambda^{(2)}_\pm for N=6N=6. (2) If 2s0(mod2)2s\equiv0\pmod2, then for odd \ell the total number of states is a union of regular and physical singular solutions, while for even \ell the total number of solutions is a union of regular and strange solutions. (3) If 2s0(mod2)2s\equiv0\pmod2, then

Nstrange(2N,2)=Nsp(2N1,21).\mathcal{N}_{\mathrm{strange}}(2N,2\ell)=\mathcal{N}_{\mathrm{sp}}(2N-1,2\ell-1).

The conjecture is based on numerical data for the spin-ss generalized Heisenberg chain. The exceptional sporadic physical solutions are explicitly known, while the proposed classification and counting relation are not established in the source.

Sources & referencesView supporting material

Primary source

Anatol N. Kirillov and Reiho Sakamoto, “Some Remarks On Nepomechie–Wang Eigenstates For Spin 1/2 XXX Model”, arXiv:1406.1958 (2015).

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