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Quantum entanglement in the one-dimensional spin-orbital SU(2) directX XXZ model

机译:一维自旋轨道SU(2)directX XXZ模型中的量子纠缠

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摘要

We investigate the phase diagram and the spin-orbital entanglement of a one-dimensional SU(2) directX XXZ model with SU(2) spin exchange and anisotropic XXZ orbital exchange interactions and negative exchange coupling constant. As a unique feature, the spin-orbital entanglement entropy in the entangled ground states increases here linearly with system size. In the case of Ising orbital interactions, we identify an emergent phase with long-range spin-singlet dimer correlations triggered by a quadrupling of correlations in the orbital sector. The peculiar translational-invariant spin-singlet dimer phase has finite von Neumann entanglement entropy and survives when orbital quantum fluctuations are included. It even persists in the isotropic SU(2) directX SU(2) limit. Surprisingly, for finite transverse orbital coupling, the long-range spin-singlet correlations also coexist in the antiferromagnetic spin and alternating orbital phase making this phase also unconventional. Moreover, we also find a complementary orbital singlet phase that exists in the isotropic case but does not extend to the Ising limit. The nature of entanglement appears essentially different from that found in the frequently discussed model with positive coupling. Furthermore, we investigate the collective spin and orbital wave excitations of the disentangled ferromagnetic-spin/ferro-orbital ground state and explore the continuum of spin-orbital excitations. Interestingly, one finds among the latter excitations two modes of exciton bound states. Their spin-orbital correlations differ from the remaining continuum states and exhibit logarithmic scaling of the von Neumann entropy with increasing system size. We demonstrate that spin-orbital excitons can be experimentally explored using resonant inelastic x-ray scattering, where the strongly entangled exciton states can be easily distinguished from the spin-orbital continuum.
机译:我们研究一维SU(2)directX XXZ模型与SU(2)自旋交换和各向异性XXZ轨道交换相互作用以及负交换耦合常数的相图和自旋轨道纠缠。作为一个独特的特征,纠缠基态的自旋轨道纠缠熵在此随系统大小线性增加。在Ising轨道相互作用的情况下,我们确定了一个由远程自旋单二聚体相关性出现的新兴阶段,该相关性是由轨道部门中相关性的四倍引起的。特有的平移不变自旋单二聚体相具有有限的冯·诺依曼纠缠熵,并且在包含轨道量子涨落时仍然存在。它甚至在各向同性SU(2)directX SU(2)极限中仍然存在。出乎意料的是,对于有限的横向轨道耦合,反铁磁自旋和交替轨道相中也同时存在长距离自旋-单重相关,因此该相也不寻常。此外,我们还发现了各向同性情况下存在的互补轨道单重态相位,但没有扩展到Ising极限。纠缠的本质似乎与经常讨论的带有正耦合的模型中的纠缠本质不同。此外,我们研究了解缠的铁磁自旋/铁轨道基态的集体自旋和轨道波激发,并探讨了自旋轨道激发的连续性。有趣的是,在后面的激发中发现了激子束缚态的两种模式。它们的自旋轨道相关性不同于其余的连续状态,并且随着系统规模的增大,表现出冯·诺伊曼熵的对数尺度。我们证明,可以使用共振非弹性x射线散射通过实验探索自旋轨道激子,其中强纠缠激子态可以轻松地与自旋轨道连续体区分开。

著录项

  • 来源
    《Physical review》 |2015年第5期|054423.1-054423.19|共19页
  • 作者单位

    Max-Planck-Institut fuer Festkoerperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany,College of Physics, Optoelectronics and Energy, Soochow University, Suzhou, Jiangsu 215006, People's Republic of China;

    Max-Planck-Institut fuer Festkoerperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany;

    Max-Planck-Institut fuer Festkoerperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany,Marian Smoluchowski Institute of Physics, Jagiellonian University, prof. S. Lojasiewicza 11, PL-30348 Krakow, Poland;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    entanglement production, characterization, and manipulation; quantized spin models;

    机译:纠缠产生;表征和操纵;量化自旋模型;

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