在一个磁通量子内dc Josephson电流阶梯或振荡效应的物理本质

本文分析了放置于高Q谐振腔中的Josephson结、双结SQUID和单结超导环,当其Josephson频率ω=2eV₀/h和腔的本征频率相等时,Josephson电流在一个磁通量子内可以产生多次阶梯或振荡的物理本质。指出对于Josephson结或双结SQUID,当ω=ω_r时,被激发起的腔的本征振荡将反馈辐照结或SQUID,反馈场的频率作用使Josephson电流产生一般地感应台阶;而反馈场的振幅是受到外磁场调制的,当这种调制作用使反馈场振幅的空间部分与辐射场的空间部分匹配时,则引起电流在一个磁通量子内产生一系列的新的阶跃。对单结超导环,当nω=ω_r时,被激发起的腔的振荡反馈辐照作用将迫使其超流电流产生周期小于φ₀的振荡。 关键词：     

对Ⅱ类超导体混合态磁阻起因的重新认识

本指出常规和基于Ａｂｒｉｋｏｓｏｖ涡旋理论所提出的关于Ⅱ类超导体混合态磁阻起因的解释存在着某些不足之外，特别对新发现的高温氧化物超导体，该解释同实验有明显地冲突。为描述Ⅱ类超导体混合态磁阻，我们认为最好的理论基础是约瑟夫逊相滑移理论。本就此进行讨论并试图说明在此基础上可以导出常规的关于Ⅱ类超导体混合态磁阻的表达式。     

脉冲磁体中的热效应

本文第一次建立了在一个正弦型脉冲通过磁体期间考虑热效应时的瞬态电流方程.计算出热效应引起电流峰值的减小,指出在脉冲时间大于10ms、磁场强度小于1MG的脉冲磁体中,热效应不是影响获得高强脉冲磁场的主要因素,只要解决磁体受力问题,目前的场值还可以大幅度提高;并指出磁体的起始电阻是影响场值的敏感因素. 理论计算第一次给出了在一个脉冲期间,通过磁体的电流与时间关系,及磁体材料的电阻和温度随时间的变化.     

First-Principles Based Model of Spin-state Phase Transition

The nature of spin-state phase transition is investigated with [Fe（C4H4N2）（Pt（CN）4}] that is＂ a novel 3D Hofmann-like compound. The bistability of this system is obtained by the first-principles calculation. It is demonstrated that thermal expansion is the intrinsic force involved in spin-state transition. Based on these results, we suggest a thermal exciting bistable model of spin-state transition with a temperature dependent crystal-field splitting （CFS）. Experimental evidence of spin-state phase transition coincides with our theoretical model. This model approaches something fundamental in the mechanism leading to the transition, and it is important in developing new and practical controllable quantum devices.     

A位离子替代对(LaCa)MnO3材料磁转变温度的影响 *

测量了(La_1-xR_x) _{2 /3} MnO₃ (其中R代表Ce ,Pr,Nd等稀土离子)和La_{2 /3}(Ca_1-yCd_y) _1/3 MnO₃ 两组铁磁性巨磁阻材料的磁转变温度 .结果发现 ,尽管在(La_1-xR_x) _{2 /3} MnO₃ 材料中其A位平均离子半径恒定 ,但居里温度T_C 存在明显的差别 ;而在La_{2 /3}(Ca_1-yCd_y) _1/3 MnO₃ 系列中虽然随Cd的替代量的增加 ,A位平均离子半径略有下降 ,T_C 却增加 .A位离子的局域磁矩对磁转变温度可能有较大的影响 .     

EFFECT OF THERMAL TREATMENTS ON THE SUPERCONDUCTIVITY OF UNDOPED AND WO3 DOPED Y-Ba-Cu-O SYSTEM

Undoped and WO₃-doped Y-Ba-Cu-O ceramics have been slowly cooled in flowing oxygen or quenched in air from 900℃ to room temperature, after sintering at 900℃ for 3Oh in flowing oxygen. The ac susceptibility measurements show that the T_c of the quenched WO₃-doped Y-Ba-Gu-O superconductor can reach 88K, while the undoped Y-Ba-Cu-O ceramic quenched in air is a non-superconductor. X-ray diffraction data show that WO₃ does not enter into the YBa₂Cu₃O_7-x lattice but forms all impurity phase. The WO₃-doped YBCO specimens quenched in air consist of orthorhombic YBa₂Cu₃O_7-x phase and an impurity phase which increases with increasing WO₃ content. Raman spectra chow that oxygen contents are different for undoped and WO₃-doped samples. It la suggested that suitable doping with WO₃ can change the oxygen content and reduce the effect of thermal treatments on the superconductivity of Y-Ba-Cu-O system.     

SmFeAsO0.78F0.22中Mn掺杂对超导电性的抑制效应

本文报道了Mn替代Fe对最佳掺杂的Sm-1111体系超导电性的影响.通过电输运及磁性质的测量发现Mn对Fe的替代迅速抑制了超导电性.随着Mn含量的增加,体系的电阻率ρ和磁化率M逐渐增大.对于低掺杂x＜0.25%和未掺杂样品,M接近零,对于≤1%,M从室温到超导转变几乎不变,实验指出Fe2+失去其磁性.我们提出这是由于F...