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Incommensurate Spin Dynamics in Underdoped Cuprate Perovskites

机译:掺杂不足的铜酸盐钙钛矿中不相称的自旋动力学

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The incommensurate magnetic response observed in normal-state cuprate perovskites is interpreted based on Mori's projection operator formalism and the t-J model of Cu-O planes. In agreement with experiment, the calculated dispersion of maxima in the susceptibility has the shape of two parabolas with upward- and downward-directed branches which converge at the antiferromagnetic wave vector. The upper parabola reflects the dispersion of magnetic excitations of the localized Cu spins, while the lower parabola arises due to the weakness of the interaction between the spin excitations and holes near the hot spots. Also, in conformity with experiment, the low-frequency incommensurability parameter δ grows with the hole concentration x for x≤0.12 and then saturates. It is conjectured that the dissimilarity of the susceptibility frequency dependencies in yttrium and lanthanum cuprates may be connected with different values of the hole bandwidth and damping in these crystals.
机译:基于Mori的投影算符形式主义和Cu-O平面的t-J模型,解释了在正常状态的铜酸盐钙钛矿中观察到的不相称的磁响应。与实验一致,在磁化率中计算出的最大值弥散具有两个抛物线的形状,两个抛物线具有向上和向下指向的分支,它们会聚在反铁磁波矢量处。上方的抛物线反映了局部Cu自旋的磁激发的分散,而下方的抛物线则是由于自旋激发与热点附近的空穴之间的相互作用弱而产生的。而且,根据实验,低频不可通量参数δ随着x≤0.12的空穴浓度x而增大,然后饱和。据推测,钇和镧铜酸盐中的磁化率频率依赖性的不同可能与这些晶体中空穴带宽和阻尼的不同值有关。

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