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Spin susceptibility of cuprates in the model of a 2D frustrated antiferromagnet: Role of renormalization of spin fluctuations in describing neutron experiments

机译:二维挫折反铁磁体模型中铜酸盐的自旋磁化率:自旋波动的重新归一化在描述中子实验中的作用

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摘要

Experimental data on the spin susceptibility of HTSC cuprates are reproduced on the basis of a spherically symmetric approach in the frustrated Heisenberg model. The inclusion of real and imaginary renormalizations in spin Green's functions makes it possible to explain the evolution of spin excitation spectrum omega(q) and susceptibility spectrum chi(q, omega) in the range from insulator to optimal doping. In the low-frustration limit corresponding to the weakly doped mode, the saddle singularity of omega(q) and scaling of chi(2D)(omega) = integral dq Im chi(q, omega) are reproduced and an analytic expression is derived for the scaling function. In the strong frustration (optimal doping) mode, the stripe scenario is demonstrated; this leads to a peak of chi(2D) (omega) in the region of omega similar to 60 meV.
机译:在沮丧的海森堡模型中,基于球对称方法,复制了HTSC铜酸盐自旋敏感性的实验数据。自旋格林函数中包含实数和虚数归一化,可以解释从绝缘体到最佳掺杂的自旋激发谱omega(q)和磁化谱chi(q,omega)的演变。在与弱掺杂模式相对应的低挫折极限中,再现了omega(q)的鞍奇异性和chi(2D)(omega)=积分dq的缩放比例Im chi(q,omega),并导出了解析表达式缩放功能。在强挫折(最佳掺杂)模式下,将演示条带场景;这会在类似于60 meV的欧米茄区域中导致chi(2D)(欧米茄)的峰值。

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