Nature of the intermediate phase of the antiferromagnetic Kitaev model in a field · revision history

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Title
Nature of the intermediate phase of the antiferromagnetic Kitaev model in a field
Plain
Numerical studies of the ideal antiferromagnetic Kitaev model in a field along the cube diagonal find an extra phase between the low-field spin liquid and the high-field polarized state. Its identity, possibly a gapless spin liquid with a Fermi surface of neutral particles, is disputed.
Precise
Model: H = K sum_<ij>_gamma S^gamma_i S^gamma_j - h sum_i (S^x_i + S^y_i + S^z_i)/sqrt(3), $K > 0$, $S = 1/2$, honeycomb lattice. For the window h_c1 < h < h_c2 found numerically, determine whether the ground state is a gapless $U(1)$ spin liquid with a spinon Fermi surface, a gapped chiral spin liquid of different Chern number, or another phase. An answer gives the classification, its boundaries in $h/K$, and the supporting entanglement and spectral evidence.
Settled by
Large-cylinder DMRG, iPEPS or neural-network variational calculations that agree on the gap, entanglement scaling and topological invariants of the intermediate phase.
Kind
well-posed
Answer type
classification
References
(empty)
Literature status
contested
Status note
(empty)
Posed since
2018