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FREE AND SPIN-POLARON STATES IN HIGH T_C SUPERCONDUCTORS

机译:高T_C超导体中的自由态和自旋极化态

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摘要

Hole states in the antiferromagnetically ordered CuO_2 planes of cupra-te perovskites are calculated within the three-band Hubbard model and with a self-consistent calculation of the Cu spin polarization. It is found that in the low doping limit the spin-polaron and the free-hole states are separated by a barrier of energy ~ 0.05eV. At finite dopings the spin-polaron states become less favorable and at high doping they turn out to be metastable. In case of high mobility of donors a phase separation of the charge carriers into domains with a local hole concentration c ~ 0.5 takes place. This explains experimentally observed formation of stripe domains with local hole concentrations c = 0.5.
机译:在三波段Hubbard模型中计算了铜钛矿型钙钛矿的反铁磁有序CuO_2平面中的空穴状态,并通过自洽计算了Cu自旋极化。发现在低掺杂极限下,自旋极化子和自由空穴态之间的能垒为〜0.05eV。在有限的掺杂下,自旋极化子态变得不利,而在高掺杂下,它们变成亚稳态。在给体高迁移率的情况下,电荷载流子发生相分离为局部空穴浓度为c〜0.5的畴。这解释了实验观察到的局部孔浓度为c = 0.5的条纹区域的形成。

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