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arXiv 1507.07166quant-ph
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有限自旋系统中的非横因子分解场和纠缠

Non-transverse factorizing fields and entanglement in finite spin systems

M. Cerezo, R. Rossignoli, N. Canosa

摘要:

本文确定了具有任意范围各向异性XYZ耦合的一般自旋阵列中存在非横向因子分解磁场的条件。首先证明了只有平行于主平面的场${h}_s$在场空间中形成四条直线时,才能存在均匀的最大取向完全可分本征态,其取向方向与${h}_s$的取向方向不同,并由各向异性决定.在铁磁(FM)和反铁磁(AFM)型系统中,这种状态总是成为沿着这些线足够强(但有限)的场的非简并基态(GS)。在原子力显微镜链,这个领域共存的非横向分解领域${h}'_s$与退化的Néel型可分离的GS,这是出现在一个有限的链中的水平交叉。它还表明,任意自旋的成对纠缠达到全范围附近的${h}_s$和${h}'_s$,消失在${h}_s$,但接近小而有限的侧限在${h}'_s$,这是解析确定的。分析了块熵和纠缠谱在它们附近的行为。

英文摘要:

We determine the conditions for the existence of non-transverse factorizing magnetic fields in general spin arrays with anisotropic XYZ couplings of arbitrary range. It is first shown that a uniform maximally aligned completely separable eigenstate can exist just for fields ${h}_s$ parallel to a principal plane and forming four straight lines in field space, with the alignment direction different from that of ${h}_s$ and determined by the anisotropy. Such state always becomes a non-degenerate ground state (GS) for sufficiently strong (yet finite) fields along these lines, in both ferromagnetic (FM) and antiferromagnetic (AFM) type systems. In AFM chains, this field coexists with the non-transverse factorizing field ${h}'_s$ associated with a degenerate Néel-type separable GS, which is shown to arise at a level crossing in a finite chain. It is also demonstrated for arbitrary spin that pairwise entanglement reaches full range in the vicinity of both ${h}_s$ and ${h}'_s$, vanishing at ${h}_s$ but approaching small yet finite side-limits at ${h}'_s$, which are analytically determined. The behavior of the block entropy and entanglement spectrum in their vicinity is also analyzed.

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