Existence of representative zero-energy states

Let HN(x,y)H_N(x,y) be the Hamiltonian on NN sites, with twist angle ϕ\phi, and let SN3S_N^3 denote the total third spin component. The representative singlet conjecture. For every NN and twist angle ϕ=π\phi=\pi, there exist parameters x,yx,y with xyx\ne y for which the Hamiltonian has exactly one zero-energy state in the sector SN3=0mod2S_N^3=0\bmod 2. For twist angle ϕ=0\phi=0, there exist parameters x,yx,y with xyx\ne y for which the Hamiltonian has no zero-energy states. If true, the symmetry and conjugation arguments imply the corresponding statements throughout the non-light-like region xy|x|\ne|y|.

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Primary source

Christian Hagendorf, “Spin chains with dynamical lattice supersymmetry”, arXiv:1207.0357 (2013).

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