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Generalized isotropic Lipkin-Meshkov-Glick models: ground state entanglement and quantum entropies

机译:广义各向同性Lipkin-Meshkov-Glick模型:基态纠缠和量子熵

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摘要

We introduce a new class of generalized isotropic Lipkin–Meshkov–Glick models with su(m+1) spin and long-range non-constant interactions, whose non-degenerate ground state is a Dicke state of su(m+1) type. We evaluate in closed form the reduced density matrix of a block of Lspins when the whole system is in its ground state, and study the corresponding von Neumann and Rényi entanglement entropies in the thermodynamic limit. We show that both of these entropies scale as a log L when L tends to infinity, where the coefficient a is equal to (m  −  k)/2 in the ground state phase with k vanishing magnon densities. In particular, our results show that none of these generalized Lipkin–Meshkov–Glick models are critical, since when L-->∞ their Rényi entropy R_q becomes independent of the parameter q. We have also computed the Tsallis entanglement entropy of the ground state of these generalized su(m+1) Lipkin–Meshkov–Glick models, finding that it can be made extensive by an appropriate choice of its parameter only when m-k≥3. Finally, in the su(3) case we construct in detail the phase diagram of the ground state in parameter space, showing that it is determined in a simple way by the weights of the fundamental representation of su(3). This is also true in the su(m+1) case; for instance, we prove that the region for which all the magnon densities are non-vanishing is an (m  +  1)-simplex in R^m whose vertices are the weights of the fundamental representation of su(m+1).
机译:我们介绍了一类具有su(m + 1)自旋和长距离非恒定相互作用的广义各向同性Lipkin-Meshkov-Glick模型,其非简并基态是su(m + 1)类型的Dicke态。当整个系统处于基态时,我们以封闭形式评估Lspins块的密度矩阵,并研究在热力学极限下相应的冯·诺依曼和Rényi纠缠熵。我们显示,当L趋于无穷大时,这两个熵都按对数L进行缩放,其中在基态相中系数a等于(m -k)/ 2,k磁子密度消失。特别是,我们的结果表明,这些广义Lipkin–Meshkov–Glick模型都不是关键模型,因为当L->∞时,其Rényi熵R_q变得独立于参数q。我们还计算了这些广义su(m + 1)Lipkin–Meshkov–Glick模型的基态的Tsallis纠缠熵,发现只有当m-k≥3时,才可以通过适当选择其参数来使其扩展。最后,在su(3)情况下,我们详细构建了参数空间中基态的相图,表明它是通过su(3)基本表示的权重简单确定的。在su(m + 1)情况下也是如此。例如,我们证明了所有磁振子密度都没有消失的区域是R ^ m中的(m + 1)-单纯形,其顶点是su(m + 1)的基本表示的权重。

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