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Communications in Theoretical Physics

Multipartite Entanglement of a Tetrahedron Lattice

Rong Zhang, Zhu Shi-Qun, Hao Xiang

Published Nov 1, 2006• 1 citation
Publisher

Abstract

Three-dimensional Heisenberg model in the form of a tetrahedron lattice is investigated. The concurrence and multipartite entanglement are calculated through 2-concurrence C and 4-concurrence C 4 . The concurrence C and multipartite entanglement C 4 depend on different coupling strengths J i and are decreased when the temperature T is increased. For a symmetric tetrahedron lattice, the concurrence C is symmetric about J 1 when J 2 is negative while the multipartite entanglement C 4 is symmetric about J 1 when J 2 <2. For a regular tetrahedron lattice, the concurrence C of ground state is 1/3 for ferromagnetic case while C = 0 for antiferromagnetic case. However, there is no multipartite entanglement since C 4 = 0 in a regular tetrahedron lattice. The external magnetic field B can increase the maximum value of the concurrence C B and induce two or three peaks in C B . There is a peak in the multipartite entanglement C 4 B when C 4 B is varied as a function of the temperature T . This peak is mainly induced by the magnetic field B .

DOI
10.1088/0253-6102/46/5/020

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Three-dimensional Heisenberg model in the form of a tetrahedron lattice is investigated. The concurrence and multipartite entanglement are calculated through 2-concurrence C and 4-concurrence C 4 . The concurrence C and multipartite entanglement C 4 depend on different coupling strengths J i and are decreased when the temperature T is increased. For a symmetric tetrahedron lattice, the concurrence C is symmetric about J 1 when J 2 is negative while the multipartite entanglement C 4 is symmetric about J 1 when J 2 <2. For a regular tetrahedron lattice, the concurrence C of ground state is 1/3 for ferromagnetic case while C = 0 for antiferromagnetic case. However, there is no multipartite entanglement since C 4 = 0 in a regular tetrahedron lattice. The external magnetic field B can increase the maximum value of the concurrence C B and induce two or three peaks in C B . There is a peak in the multipartite entanglement C 4 B when C 4 B is varied as a function of the temperature T . This peak is mainly induced by the magnetic field B .
The effects of anisotropy and magnetic field on multipartite entanglement of ground state in Heisenberg XY model are investigated. The multipartite entanglement increases as a function of the inverse strength of the external field when the degree of anisotropy is finite. There are two peaks when the degree of anisotropy is γ = ±1. When the degree of anisotropy increases further, the multipartite entanglement will decrease and tend to a constant. The threshold of the inverse strength of the external field for generating multipartite entanglement generally decreases with the increasing of qubits.
The energy spectrum, ground-state phase diagram, pair correlation functions, and concurrence are exactly calculated for a spin-1/2 quantum Heisenberg distorted tetrahedron in a magnetic field.The ground-state phase diagram in the interaction ratio versus magnetic field plane totally involves five different ground states, which differ from one another by the total spin, local pair correlation functions, and/or concurrence.In addition to the classical fully polarized ferromagnetic ground state there also appear four outstanding quantum ground states, two of which belong to a singlet sector and another two to a triplet sector.A degree of bipartite entanglement quantified through the concurrence is examined as a function of magnetic field, temperature, and the interaction ratio.
Exchange interactions in spin systems can give rise to quantum entanglement in the ground and thermal states of the systems. We consider a spin tetramer, with spins of magnitude 12\frac{1}{2}21​, in which the spins interact via nearest-neighbor, diagonal, and four-spin interactions of strength J1{J}_{1}J1​, J2{J}_{2}J2​, and KKK, respectively. The ground- and thermal-state entanglement properties of the tetramer are calculated analytically in the various limiting cases. Both bipartite and multipartite entanglements are considered and a signature of the quantum phase transition (QPT), in terms of the entanglement ratio, is identified. The first-order QPT is accompanied by discontinuities in the nearest-neighbor and diagonal concurrences. The magnetic properties of a S=12S=\frac{1}{2}S=21​ antiferromagnetic polyoxovanadate compound V12 are well explained by tetramers, with J2=0{J}_{2}=0J2​=0, K=0K=0K=0, in which the spins interact via the isotropic Heisenberg exchange interaction Hamiltonian. Treating the magnetic susceptibility $\ensuremath{\chi}$ as an entanglement witness (EW), an estimate of the lower bound of the critical entanglement temperature Tc{T}_{c}Tc​ below which entanglement is present in the experimental compound, is determined. Two other cases considered include the symmetric tetramer---i.e., tetrahedron (J1=J2,K=0)({J}_{1}={J}_{2},K=0)(J1​=J2​,K=0)---and the symmetric trimer. In both the cases, there is no entanglement between a pair of spins in the thermal state but multipartite entanglement is present. A second EW based on energy provides an estimate of the entanglement temperature TE{T}_{E}TE​ below which the thermal state is definitely entangled. This EW detects bipartite entanglement in the case of the tetramer describing a square of spins (the case of V12 ) and multipartite entanglement in the cases of the tetrahedron and symmetric trimer.
The entanglement quantum properties of a spin-1/2 Ising-Heisenberg model on a symmetrical diamond chain were analyzed. Due to the separable nature of the Ising-type exchange interactions between neighboring Heisenberg dimers, calculation of the entanglement can be performed exactly for each individual dimer. Pairwise thermal entanglement was studied in terms of the isotropic Ising-Heisenberg model and analytical expressions for the concurrence (as a measure of bipartite entanglement) were obtained. The effects of external magnetic field H and next-nearest neighbor interaction J(m) between nodal Ising sites were considered. The ground state structure and entanglement properties of the system were studied in a wide range of coupling constant values. Various regimes with different values of ground state entanglement were revealed, depending on the relation between competing interaction strengths. Finally, some novel effects, such as the two-peak behavior of concurrence versus temperature and coexistence of phases with different values of magnetic entanglement, were observed.
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.