Abstract

Recently new novel magnetic phases were shown to exist in the asymptotic steady states of spin systems coupled to dissipative environments at zero temperature. Tuning the different system parameters led to quantum phase transitions among those states. We study, here, a finite two-dimensional Heisenberg triangular spin lattice coupled to a dissipative Markovian Lindblad environment at finite temperature. We show how applying an inhomogeneous magnetic field to the system at different degrees of anisotropy may significantly affect the spin states, and the entanglement properties and distribution among the spins in the asymptotic steady state of the system. In particular, applying an inhomogeneous field with an inward (growing) gradient toward the central spin is found to considerably enhance the nearest neighbor entanglement and its robustness against the thermal dissipative decay effect in the completely anisotropic (Ising) system, whereas the beyond nearest neighbor ones vanish entirely. The spins of the system in this case reach different steady states depending on their positions in the lattice. However, the inhomogeneity of the field shows no effect on the entanglement in the completely isotropic (XXX) system, which vanishes asymptotically under any system configuration and the spins relax to a separable (disentangled) steady state with all the spins reaching a common spin state. Interestingly, applying the same field to a partially anisotropic (XYZ) system does not just enhance the nearest neighbor entanglements and their thermal robustness but all the long-range ones as well, while the spins relax asymptotically to very distinguished spin states, which is a sign of a critical behavior taking place at this combination of system anisotropy and field inhomogeneity.

Highlights

  • Quantum entanglement is considered to be the physical resource responsible for manipulating the linear superposition of the quantum states in many body quantum systems [1]

  • We studied a finite two-dimensional Heisenberg spin lattice with nearest-neighbor spin interaction coupled to a dissipative Lindblad environment in the presence of an external inhomogeneous magnetic field at finite temperature

  • The spin lattice consists of a central spin surrounded by 6 border spins distant form it in a triangular symmetric structure

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Summary

Introduction

Quantum entanglement is considered to be the physical resource responsible for manipulating the linear superposition of the quantum states in many body quantum systems [1]. Lee et al studied an anisotropic XYZ Heisenberg system of localized spins on a d-dimensional lattice at zero temperature under dissipative spin-flip process, associated with optical pumping They showed how the asymptotic behavior of the system can exhibit new novel magnetic phases, as the degree of anisotropy of the spin-spin interaction is varied in the absence of external magnetic fields [38]. We study the time evolution and the asymptotic steady state of the bipartite quantum entanglement and spin relaxation in a finite two-dimensional Heisenberg spin-1/2 triangular lattice, where a single central spin is surrounded by distant spins, with nearest-neighbor spin interaction under the influence of a dissipative Lindblad environment at zero and finite temperatures.

The Model
Dynamics of Entanglement
Ising System
XYZ System
XXX System
Conclusions
Full Text
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