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首页> 外文期刊>Physical review >Incommensurability effects in odd length J_1- J_2 quantum spin chains: On-site magnetization and entanglement
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Incommensurability effects in odd length J_1- J_2 quantum spin chains: On-site magnetization and entanglement

机译:奇长J_1-J_2量子自旋链中的不可通约性效应:现场磁化和纠缠

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摘要

For the antiferromagnetic J_1-J_2 quantum spin chain with an even number of sites, the point J_2~d = J_1/2 is a disorder point. It marks the onset of incommensurate real space correlations for J_2 > J_2~d At a distinct larger value of J_2 = 0.520 36(6)J_1, the Lifshitz point, the peak in the static structure factor begins to move away from k = π. Here, we focus on chains with an odd number of sites. In this case, the disorder point is also at J_2~d = J_1/2 but the behavior close to the Lifshitz point, J_2~L ≈ 0.5387J_1, is quite different: starting at J_2~L, the ground state goes through a sequence of level crossings as its momentum changes away from k = π/2. An even length chain, on the other hand, is gapped for any J_2 > 0.24 J_1 and has the ground-state momentum k = 0. This gradual change in the ground-state wave function for chains with an odd number of sites is reflected in a dramatic manner directly in the ground-state on-site magnetization as well as in the bipartite von Neumann entanglement entropy. Our results are based on DMRG calculations and variational calculations performed in a restricted Hilbert space defined in the valence bond picture. In the vicinity of the point J_2 = J_1/2, we expect the variational results to be very precise.
机译:对于具有偶数个位点的反铁磁J_1-J_2量子自旋链,点J_2〜d = J_1 / 2是无序点。它标志着J_2> J_2〜d出现不相称的真实空间相关性的开始。在明显更大的J_2 = 0.520 36(6)J_1值Lifshitz点处,静态结构因子的峰值开始偏离k =π。在这里,我们重点关注具有奇数个站点的链。在这种情况下,无序点也位于J_2〜d = J_1 / 2,但行为接近Lifshitz点,即J_2〜L≈0.5387J_1,是完全不同的:从J_2〜L开始,基态经历一个序列当其动量从k =π/ 2改变时,平交路口的角度。另一方面,对于任何J_2> 0.24 J_1,均等长度的链是有间隙的,并且基态动量k =0。对于具有奇数个位点的链,基态波动函数的这种逐渐变化反映在直接在基态现场磁化以及二分体冯·诺依曼纠缠熵中以惊人的方式出现。我们的结果基于在价键图中定义的受限希尔伯特空间中进行的DMRG计算和变分计算。在点J_2 = J_1 / 2附近,我们期望变化结果非常精确。

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