首页> 外文OA文献 >Charge compensation and optimal stoichiometry in superconducting (Ca$_x$La$_{1-x}$)(Ba$_{1.75-x}$La$_{0.25+x}$)Cu$_3$O$_y$
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Charge compensation and optimal stoichiometry in superconducting (Ca$_x$La$_{1-x}$)(Ba$_{1.75-x}$La$_{0.25+x}$)Cu$_3$O$_y$

机译:超导中的电荷补偿和最佳化学计量   (钙$ $ _x拉$ _ {1-X} $)(巴$ _ {1.75-X} $拉$ _ {0.25 + X} $)的Cu $ $ _3ö$ $ _y

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摘要

The superconductive and magnetic properties of charge$-$compensated(Ca$_x$La$_{1-x}$)(Ba$_{1.75-x}$La$_{0.25+x}$)Cu$_3$O$_y$ (normally denoted asCLBLCO) are considered through quantitative examination of data for electricalresistivity, magnetic susceptibility, transition width, muon$-$spin rotation,x$-$ray absorption, and crystal structure. A derivative of LaBa$_2$Cu$_3$O$_y$,cation doping of this unique tetragonal cuprate is constrained by compensatingLa substitution for Ba with Ca substitution for La, where for 0 {\le} x {\le}0.5 local maxima in T$_C$ occur for y near 7.15. It is shown that optimumsuperconductivity occurs for 0.4 {\le} x {\le} 0.5, that the superconductivityand magnetism observed are nonsymbiotic phenomena, and thatcharge$-$compensated doping leaves the carrier density in the cuprate planesnearly invariant with x, implying that only a small fraction of superconductingcondensate resides therein. Applying a model of electronic interactions betweenphysically separated charges in adjacent layers, the mean in-plane spacingbetween interacting charges, {\ell} = 7.1206 {\AA}, and the distance betweeninteracting layers, {\zeta} = 2.1297 {\AA}, are determined for x = 0.45. Thetheoretical optimal T$_{C0}$ {\propto} {\ell}$^{-1}${\zeta}$^{-1}$ of 82.3 K isin excellent agreement with experiment ({\approx} 80.5 K), bringing the numberof compounds for which T$_{C0}$ is accurately predicted to 37 from sixdifferent superconductor families (overall accuracy of {\pm}1.35 K).
机译:电荷$-$的超导和磁性质(Ca $ _x $ La $ _ {1-x} $)(Ba $ _ {1.75-x} $ La $ _ {0.25 + x} $)Cu $ _3 $通过对电阻率,磁化率,过渡宽度,μ子-自旋旋转,x $-射线吸收和晶体结构的数据进行定量检查,可以考虑Oy_y $(通常表示为CLBLCO)。 LaBa $ _2 $ Cu $ _3 $ O $ _y $的导数,此独特的四方铜酸盐的阳离子掺杂受到La的Ba置换和La的Ca置换的补偿,其中0 {\ le} x {\ le} 0.5局部T $ _C $的最大值出现在7.15附近的y处。结果表明,最佳超导发生在0.4 {\ le} x {\ le} 0.5处,所观察到的超导和磁性是非共生现象,并且电荷$-$补偿的掺杂使铜酸盐平面中的载流子密度几乎与x不变,这意味着仅一小部分超导冷凝物留在其中。应用相邻层中物理分离的电荷之间的电子相互作用模型,相互作用电荷之间的平均面内间距{\ ell} = 7.1206 {\ AA},相互作用层之间的距离{\ zeta} = 2.1297 {\ AA},确定x = 0.45。理论上的最佳T $ _ {C0} $ {\ propto} {\ ell} $ ^ {-1} $ {\ zeta} $ ^ {-1} $的实验值与实验({\ approx} 80.5 K ),从而从六个不同的超导体族中准确预测出T $ _ {C0} $的化合物数量达到37(总精度{\ pm} 1.35 K)。

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