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arXiv:1405.1123

Renormalized quantum Fisher information manifestation of Berezinskii-Kosterlitz-Thouless phase transition for spin-1/2 XXZ chain

Qiang Zheng, Yao Yao, Xun‐Wei Xu, Yong Li

Published May 6, 2014• 2 citations
arXivHTMLPDF

Abstract

Combining the ideas of quantum Fisher information and quantum renormalization group method, the Berezinskii-Kosterlitz-Thouless quantum phase transition of spin- 1/2 XXZ chain is investigated. Quantum Fisher informations of the whole N sites and the partial N/3 sites are studied. They display very similar behaviors, even though their mathematical formulas are very different from each other. The universally critical exponent of quantum Fisher information is obtained as beta=0.47, which is consistent with the results obtained by the renormalized concurrence or discord. We also discuss the relationship between quantum Fisher information and entanglement

DOI
10.48550/arxiv.1405.1123

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Combining the ideas of quantum Fisher information and quantum renormalization group method, the Berezinskii-Kosterlitz-Thouless quantum phase transition of spin- 1/2 XXZ chain is investigated. Quantum Fisher informations of the whole N sites and the partial N/3 sites are studied. They display very similar behaviors, even though their mathematical formulas are very different from each other. The universally critical exponent of quantum Fisher information is obtained as beta=0.47, which is consistent with the results obtained by the renormalized concurrence or discord. We also discuss the relationship between quantum Fisher information and entanglement
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We investigate the one-dimensional Heisenberg XXZ\mathit{XXZ}XXZ model involving the Dzyaloshinskii-Moriya (DM) interaction from the viewpoint of quantum information. By using the density-matrix--renormalization-group technique, we study the Berezinskii-Kosterlitz-Thouless (BKT) phase transition using the ground-state fidelity, the fidelity susceptibility, and the entanglement entropy. We argue that the BKT phase transition can be well characterized in our model, and the critical line induced by the DM interaction can also be detected.
This study investigates quantum Fisher information (QFI) with respect to a class of nonlocal operators $\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{O}$ in one-dimensional quantum chains. Based upon the triangular matrix-product-operator theory, we establish a universal scaling behavior of QFI with respect to $\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{O}$ for general infinite matrix-product states (iMPSs): $\mathcal{F}\ensuremath{\sim}{\ensuremath{\varrho}}_{2}{N}^{2}+{\ensuremath{\varrho}}_{1}N+{\ensuremath{\varrho}}_{0}$, where the coefficients ${\ensuremath{\varrho}}_{i}$ can be efficiently identified by iMPS algorithms. Applied to a spin-1 Bilinear-Biquadratic model and an XXZ model, the scaling coefficients ${{\ensuremath{\varrho}}_{i}}$ distinguish various phases through distinct scaling behaviors: For instance, the topologically ordered Haldane phase exhibits characteristic quadratic scaling (${\ensuremath{\varrho}}_{2}\ensuremath{\ne}0$), while the trimer and dimer phases are featured with linear scaling (${\ensuremath{\varrho}}_{1}\ensuremath{\ne}0$). Notably, since the QFI scaling behavior undergoes fundamental changes between distinct phases, these coefficients provide signals at first-order, second-order, and Berezinskii-Kosterlitz-Thouless type quantum phase transitions in these models. Furthermore, finite bond-dimension (DDD) scaling analysis reveals a dichotomy. For gapped phases, the coefficients converge rapidly as DDD increases. Conversely, for critical systems, the coefficients exhibit DDD-scaling effects that depend on the specific model. By bypassing finite-size fittings with limited NNN, our approach accesses the thermodynamic-limit physics for QFI with respect to nonlocal operators, offering new avenues for characterizing exotic quantum phases in one-dimensional quantum systems.
We investigate the quantum Fisher information and quantum phase transitions of an XY spin chain with staggered Dzyaloshinskii-Moriya interaction using the quantum renormalization-group method. The quantum Fisher information, its first-derivatives, and the finite-size scaling behaviors are rigorously calculated respectively. The singularity of the derivatives at the phase transition point as a function of lattice size is carefully discussed and it is revealed that the scaling exponent for quantum Fisher information at the critical point can be used to describe the correlation length of this model, addressing the substantial role of staggered Dzyaloshinskii-Moriya interaction in modulating quantum phase transitions.