Universal finite-size amplitude and anomalous entanglement entropy of quantum Lifshitz criticalities in topological chains
arXiv:2110.08305 · doi:10.21468/SciPostPhys.12.4.134
Abstract
We consider Lifshitz criticalities with dynamical exponent that emerge in a class of topological chains. There, such a criticality plays a fundamental role in describing transitions between symmetry-enriched conformal field theories (CFTs). We report that, at such critical points in one spatial dimension, the finite-size correction to the energy scales with system size, , as , with universal and anomalously large coefficient. The behavior originates from the specific dispersion around the Fermi surface, . We also show that the entanglement entropy exhibits at the criticality a non-logarithmic dependence on , where is the length of the sub-system. In the limit of , the maximally-entangled ground state has the entropy, . Here is some non-universal entropy originating from short-range correlations and is half-integer or integer depending on the degrees of freedom in the model. We show that the novel entanglement originates from the long-range correlation mediated by a zero mode in the low energy sector. The work paves the way to study finite-size effects and entanglement entropy around Lifshitz criticalities and offers an insight into transitions between symmetry-enriched criticalities.
22 pages, 4 figures
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