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Chinese Physics Letters

Pairwise Entanglement and Quantum Phase Transitions in Spin Systems

顾世建, 田光善, 林海青

Published Jan 1, 2007• 0 citations
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Based on transfer-matrix density matrix renormalization group (TMRG) method, a general procedure to calculate the finite-temperature pairwise entanglement of low-dimensional quantum chains is proposed. The reduced pairwise density matrix is reconstructed with TMRG, and measures of quantum entanglement can be calculated from the pairwise density matrix. The finite-temperature entanglement of the diamond chain model and the spin trimerized model, which are two typical models revealing $1∕3$ plateaus in the magnetization curves, is calculated. For the diamond chain model, the anisotropy coefficient $\ensuremath{\Delta}$ is found to have a great effect on the appearance of the magnetization plateau, and the plateau disappears when $\ensuremath{\Delta}=0.5$. Moreover, our results show that the pairwise entanglement can provide information complementary to that obtained from bulk properties. For the trimerized model, the temperature dependence of the pairwise entanglement is calculated, and the threshold temperature ${T}_{c}$, above which the thermal entanglement vanishes, is found to be independent of the external magnetic field $B$. In addition, the scaling behavior of the thermal entanglement is calculated in the Trotter space. With the augmentation of the system in the Trotter direction, we find that the low-temperature entanglement shows obvious variation in the vicinity of quantum phase transition (QPT) point ${B}_{c}$ and converges fast in noncritical regions, which provides another way to identify QPT of one-dimensional quantum systems.

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Approach to the quantum phase transition of spin chains in terms of pair-wise entanglement

Kaoru Shimizu, Akira Kawaguchi

Physics Letters A•Feb 25, 2006•3 citations
The entanglement properties of a three-spin XXZ Heisenberg chain with three-spin interaction are studied by means of concurrence of pairwise entanglement. We show that ground-state pairwise entanglement, pairwise thermal entanglement, or quantum phase transition is not present in antiferromagnetic spin chain. For the ferromagnetic case, quantum phase transition takes place at Δ = 1 for anisotropic interaction and at some values of three-spin coupling strength, and pairwise thermal entanglement increases when the value of J / T increases and with anisotropic interaction and three-spin interaction decrease. In addition, we find that increasing the anisotropic interaction and the three-spin interaction will decrease critical temperature.
Based on transfer-matrix density matrix renormalization group (TMRG) method, a general procedure to calculate the finite-temperature pairwise entanglement of low-dimensional quantum chains is proposed. The reduced pairwise density matrix is reconstructed with TMRG, and measures of quantum entanglement can be calculated from the pairwise density matrix. The finite-temperature entanglement of the diamond chain model and the spin trimerized model, which are two typical models revealing 1∕31∕31∕3 plateaus in the magnetization curves, is calculated. For the diamond chain model, the anisotropy coefficient $\ensuremath{\Delta}$ is found to have a great effect on the appearance of the magnetization plateau, and the plateau disappears when $\ensuremath{\Delta}=0.5$. Moreover, our results show that the pairwise entanglement can provide information complementary to that obtained from bulk properties. For the trimerized model, the temperature dependence of the pairwise entanglement is calculated, and the threshold temperature Tc{T}_{c}Tc​, above which the thermal entanglement vanishes, is found to be independent of the external magnetic field BBB. In addition, the scaling behavior of the thermal entanglement is calculated in the Trotter space. With the augmentation of the system in the Trotter direction, we find that the low-temperature entanglement shows obvious variation in the vicinity of quantum phase transition (QPT) point Bc{B}_{c}Bc​ and converges fast in noncritical regions, which provides another way to identify QPT of one-dimensional quantum systems.