Fidelity and entanglement entropy for infinite-order phase transitions

• URL: http://arxiv.org/abs/2108.09966v1
• Date: Mon, 23 Aug 2021 06:28:50 GMT
• Title: Fidelity and entanglement entropy for infinite-order phase transitions
• Authors: Jin Zhang
• Abstract summary: We study the fidelity and the entanglement entropy for the ground states of quantum systems that have infinite-order quantum phase transitions. In particular, we consider the quantum O(2) model with a spin-$S$ truncation, where there is an infinite-order Gaussian (IOG) transition for $S = 1$. We show that the height of the peak in the fidelity susceptibility ($chi_F$) converges to a finite thermodynamic value as a power law of $1/L$ for the IOG transition and as $1/ln(L)$ for BKT transitions.
• Score: 4.453923176362749
• License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
• Abstract: We study the fidelity and the entanglement entropy for the ground states of quantum systems that have infinite-order quantum phase transitions. In particular, we consider the quantum O(2) model with a spin-$S$ truncation, where there is an infinite-order Gaussian (IOG) transition for $S = 1$ and there are Berezinskii-Kosterlitz-Thouless (BKT) transitions for $S \ge 2$. We show that the height of the peak in the fidelity susceptibility ($\chi_F$) converges to a finite thermodynamic value as a power law of $1/L$ for the IOG transition and as $1/\ln(L)$ for BKT transitions. The peak position of $\chi_F$ resides inside the gapped phase for both the IOG transition and BKT transitions. On the other hand, the derivative of the block entanglement entropy with respect to the coupling constant ($S^{\prime}_{vN}$) has a peak height that diverges as $\ln^{2}(L)$ [$\ln^{3}(L)$] for $S = 1$ ($S \ge 2$) and can be used to locate both kinds of transitions accurately. We include higher-order corrections for finite-size scalings and crosscheck the results with the value of the central charge $c = 1$. The crossing point of $\chi_F$ between different system sizes is at the IOG point for $S = 1$ but is inside the gapped phase for $S \ge 2$, while those of $S^{\prime}_{vN}$ are at the phase-transition points for all $S$ truncations. Our work elaborates how to use the finite-size scaling of $\chi_F$ or $S^{\prime}_{vN}$ to detect infinite-order quantum phase transitions and discusses the efficiency and accuracy of the two methods.

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