首页> 外文OA文献 >Electronic and Magnetic Properties of Electron-doped Superconductor, Sm_{1.85}Ce_{0.15}CuO_{4-delta}
【2h】

Electronic and Magnetic Properties of Electron-doped Superconductor, Sm_{1.85}Ce_{0.15}CuO_{4-delta}

机译:电子掺杂超导体的电子和磁性,   sm_ {1.85} CE_ {0.15} CuO_ {4-Δ}

代理获取
本网站仅为用户提供外文OA文献查询和代理获取服务,本网站没有原文。下单后我们将采用程序或人工为您竭诚获取高质量的原文,但由于OA文献来源多样且变更频繁,仍可能出现获取不到、文献不完整或与标题不符等情况,如果获取不到我们将提供退款服务。请知悉。

摘要

Temperature-dependent magnetization (M(T)) and specific heat (C_p(T))measurements were carried out on single crystal Sm_{1.85}Ce_{0.15}CuO_{4-delta}(T_c = 16.5 K). The magnetic anisotropy in the static susceptibility, chi{equiv} M/H, is apparent not only in its magnitude but also in its temperaturedependence, with chi_{perp} for H{perp}c larger than chi_{parallel} forH{parallel}c. For both field orientations, chi does not follow the Curie-Weissbehavior due to the small energy gap of the J = 7/2 multiplet above the J = 5/2ground-state multiplet. However, with increasing temperature, chi_{parallel}(T)exhibits a broad minimum near 100 K and then a slow increase whilechi_{perp}(T) shows a monotonic decrease. A sharp peak in C_p(T) at 4.7 Kmanifests an antiferromagnetic ordering. The electronic contribution, gamma, toC_p(T) is estimated to be gamma = 103.2 (7) mJ/moleSmK^2. The entropyassociated with the magnetic ordering is much smaller than Rln2, where R is thegas constant, which is usually expected for the doublet ground state ofSm^{+3}. The unusual magnetic and electronic properties evident in M(T) andC_p(T) are probably due to a strong anisotropic interaction between conductionelectrons and localized electrons at Sm^{+3} sites.
机译:对单晶Sm_ {1.85} Ce_ {0.15} CuO_ {4-δ}(T_c = 16.5 K)进行了随温度变化的磁化强度(M(T))和比热(C_p(T))测量。静态磁化率chi {equiv} M / H的磁各向异性不仅在幅度上而且在温度依赖性上都很明显,H {perp} c的chi_ {perp}大于H {parallel}的chi_ {parallel} C。对于两个场方向,由于J = 7/2多重峰的能隙比J = 5/2基态多重峰小,所以chi不遵循居里-魏斯行为。但是,随着温度的升高,chi_ {parallel}(T)在100 K附近表现出很宽的最小值,然后缓慢升高,而chi_ {perp}(T)显示出单调降低。 C_p(T)的峰值在4.7 Kmanifest处表明反铁磁有序。对C_p(T)的电子贡献γ估计为γ= 103.2(7)mJ / molSmK ^ 2。与磁序相关的熵比Rln2小得多,其中R是气体常数,通常对于Sm ^ {+ 3}的二重态基态是期望的。 M(T)和C_p(T)中明显的异常磁和电子性质可能是由于传导电子与Sm ^ {+ 3}位处的局域电子之间的强各向异性相互作用所致。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
代理获取

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