首页> 外文期刊>Solid State Communications >An X-ray absorption study of the dependence of the density of holes on T-c and/or the diamagnetic fraction in the oxycarbonate superconducting system Hg1-xMxSr4Cu2(CO3)O6+delta (M = Mo, Cr)
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An X-ray absorption study of the dependence of the density of holes on T-c and/or the diamagnetic fraction in the oxycarbonate superconducting system Hg1-xMxSr4Cu2(CO3)O6+delta (M = Mo, Cr)

机译:X射线吸收研究碳酸盐超导系统Hg1-xMxSr4Cu2(CO3)O6 +δ(M = Mo,Cr)中空穴密度与T-c和/或反磁性分数的相关性

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摘要

X-ray absorption near edge structure (XANES) measurements have been made on Cu L-3 and O 1s edges for two transition metal substituted Hg based superconducting oxycarbonates Hg0.5Mo0.5Sr4Cu2(CO3)O6+delta and Hg0.4Cr0.6Sr4Cu2(CO3)O6+delta. The diamagnetic (DM) fraction for the Cr substituted system is nearly double (similar to 60%) that for the Mo substituted system (similar to 35%). On the other hand, the superconducting transition temperature (T-c) for the Cr sample (37 K) is only about half that for the Mo sample (similar to 74 K). Thus it was very interesting to look at the density of holes in these two cases. Cu L-3 and O 1s edge XANES spectra clearly indicate the presence of an adequate number of doping holes in both the samples, characteristic of their superconducting properties. But surprisingly, the densities of the holes (doh) are almost the same (similar to 0.15) for the two samples. If it was solely correlated with the T-c, one would expect the doh of the Mo sample to be nearly double the Cr one. But the present finding presents evidence indicating that the doh must have a dependence upon the diamagnetic fraction over and above its dependence upon the transition temperature in the cuprate perovskites. This important basic question/fact needs to be explored for some other systems too, to put the conclusion on a firm footing. The results of resistivity and susceptibility measurements have also been presented briefly. (c) 2006 Elsevier Ltd. All rights reserved.
机译:对两个过渡金属取代的Hg基超导碳酸盐Hg0.5Mo0.5Sr4Cu2(CO3)O6 + delta和Hg0.4Cr0.6Sr4Cu2( CO3)O6 +δ。 Cr取代系统的抗磁性(DM)分数几乎是Mo取代系统(近似35%)的两倍(约60%)。另一方面,Cr样品(37 K)的超导转变温度(T-c)仅为Mo样品的超导转变温度的一半(类似于74 K)。因此,在这两种情况下查看孔的密度非常有趣。 Cu L-3和O 1s的边缘XANES光谱清楚地表明两个样品中都存在足够数量的掺杂孔,这是它们的超导特性的特征。但是令人惊讶的是,两个样品的孔密度(doh)几乎相同(近似0.15)。如果仅与T-c相关,则可以预期Mo样品的doh几乎是Cr的两倍。但是,本发现提供了证据,表明doh不仅必须依赖于反磁性组分,还必须依赖于其对铜酸盐钙钛矿中转变温度的依赖。对于其他一些系统,也需要探索这个重要的基本问题/事实,以使结论牢固立足。还简要介绍了电阻率和磁化率测量的结果。 (c)2006 Elsevier Ltd.保留所有权利。

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