...
首页> 外文期刊>Physica, A. Statistical mechanics and its applications >On superconductivity of hole-doped C-60 and comparison with electron-doped X3C60 (X = alkali atom) - Quantitative analysis on the basis of indirect-exchange pairing
【24h】

On superconductivity of hole-doped C-60 and comparison with electron-doped X3C60 (X = alkali atom) - Quantitative analysis on the basis of indirect-exchange pairing

机译:掺杂空穴的C-60的超导性及其与电子掺杂的X3C60(X =碱原子)的比较-基于间接交换对的定量分析

获取原文
获取原文并翻译 | 示例
   

获取外文期刊封面封底 >>

       

摘要

We undertake a quantitative analysis of critical temperatures in electron-doped X3C60 (with X an alkali atom or a combination of alkalis) and hole-doped C-60, the latter realized recently (Nature 408 (2000) 549) by using strong electrostatic fields on thin films. The formalism employed involves indirect-exchange pairing between conduction electrons (quasi-particles) via diamagnetic Cooper-pair mediators, in the present case carbon-carbon double bonds of the C60 molecules. The same principle was previously applied in analyses of high-Tc cuprates with oxygen anions O-2-mediating Cooper-pair formation. The primary goals of the analysis are the interpretation of the established surprisingly high (52 K) T-C in hole-doped C-60 with 3.2 holes per molecule C-60, and the projected (same authors) T-C beyond 100 K which might be reached upon modest expansion of the lattice. It is found, on the basis of the indirect-exchange formalism, that the high TC values for hole-doped C-60 are due to an intrinsic correlation between the two principal parameters (kappa, beta) of the formalism, which is lacking in electron-doped compounds. It is further conjectured that the projected Tc beyond 100 K upon expansion of the lattice is not realistic instead of T-C > 100 K at a (cubic) lattice parameter a = 14.60 Angstrom we find T-C = 68.0 K for that value of a, and a maximum T-C(a) of 72.4 K at a = 15.02 Angstrom. The calculated T-C(a) for electron-doped C-60, evaluated along the same lines, are very similar to those obtained earlier (Chem. Phys. 176 (1993) 1), and are in quantitative agreement with experiment. (C) 2001 Elsevier Science B.V. All rights reserved. [References: 22]
机译:我们对掺杂电子的X3C60(其中X为碱原子或碱的组合)和掺杂空穴的C-60(最近通过自然电场(自然408(2000)549)实现)的临界温度进行了定量分析。在薄膜上。所采用的形式主义涉及经由抗磁性库珀对介体(在当前情况下为C60分子的碳-碳双键)在导电电子(准粒子)之间进行间接交换配对。以前,相同的原理还用于分析具有氧阴离子O-2-介导的库珀对的高Tc铜酸盐。分析的主要目的是解释在空穴掺杂的C-60中每分子C-60具有3.2个孔的已确立的令人惊讶的高(52 K)TC,以及可能达到的超过100 K的预计(相同作者)TC适度扩展晶格。在间接交换形式主义的基础上,发现掺杂空穴的C-60的高TC值是由于形式主义的两个主要参数(kappa,β)之间的内在联系所致,而在这方面缺乏这种联系。电子掺杂的化合物。进一步推测,在晶格扩展时超过100 K的投影Tc是不现实的,而不是在(立方)晶格参数a = 14.60埃时TC> 100 K,我们发现a的TC = 68.0 K,a在a = 15.02埃时的最大TC(a)为72.4 K.沿着相同的线评估的电子掺杂的C-60的T-C(a)计算值与早期获得的值非常相似(Chem。Phys。176(1993)1),并且与实验定量一致。 (C)2001 Elsevier Science B.V.保留所有权利。 [参考:22]

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号