Pb-Sb合金脱溶过程对超导临界特性的影响

1961年Kunzler等人发现:Nb_3Sn,Nb-Zr等超导体在强磁场中临界电流密度jc仍然很大,可供制备获得强场的超导体磁体使用。 Mendelssohn曾将硬超导体临界磁场的增大,归源于样品内部存在尺寸很小的超导“系”。Kunzler将超导“系”和位错线联系起来,并且认为,他所观察到的高jc值是由于样品内部位错线密度很大。另一方面,却又把硬超导体当作均匀介质处理,他从理论出发,用负界面能效应来解释超导合金的反常磁行为。     

楔形薄膜逾渗系统的临界特性

报道一种楔形金属薄膜逾渗系统的制备方法和测量结果,这种新型逾渗系统具有独特的非线性I-V特性和临界规律,从实验中发现:在这一各向异性系统中,普适标度关系仍然成立,分析表明:这些特性是由于该系统中随空间坐标而变化的跳跃电导效应而引起的. 关键词：     

超导磁体物理研究的新实验技术

一、引 言 在文献[1]中评述了超导磁体稳定性的各种理论,作为续篇,这里我们讨论有关磁体物理研究的实验新技术. 稳定化是建造超导磁体的关键所在.在讨论稳定化时,我们首先应该明确,我们是针对哪一种不稳定因素或扰动来进行稳定的.电磁不稳定性以磁通跳跃为表征,经过多年的研究已趋于解决;而机械不稳定性可以看成是在应力连续作用下的不连续反应:剪切式相变(孪生和马氏体相变)引起的锯齿形屈服;浸渍剂的破碎;超导线的滑移或微滑移……。这些机械扰动的物理抽象是在磁体某一局域产生热脉冲,超导电性的猝灭是其次级效应. 当今磁体物理的前沿课…     

SrMn0.5Fe0.5O3的自旋玻璃态和过渡金属离子价态的研究

采用固相反应法制备了SrMn_0.5Fe_0.5O₃陶瓷样品,并对样品的晶体结构,磁性和离子价态进行了系统的表征与分析. X射线衍射谱的Rietveld拟合表明样品属于理想的立方钙钛矿型结构,Mn离子和Fe离子随机占据B位的O八面体中心. X射线光电子能谱表明Mn离子为+3和+4的混合原子价态,Fe离子为+3价. 样品在大于230K的高温区域呈现Curie顺磁特性,在小于230 K的低温区域样品表现出自旋玻璃态行为,这种特性源于Mn离子和Fe离子之间的交换作用及自身价态和分布的不均匀性. 由于Fe³⁺离子占据O八面体的中心,对顺磁区的Mssbauer谱测量表现为四级分裂.     

铁基铁磁超导体

超导电性与铁磁长程序是两个"敌对"的物质状态。长期以来,探索超导与铁磁共存是十分耐人寻味的课题。文章在回顾半个多世纪以来该课题主要进展的基础上,重点介绍了作者近年来对新型铁基铁磁超导体的发现和发展,最后对这类新材料的进一步研究进行了展望。     

Interplay of superconductivity and d-f correlation in CeFeAs_(1-x)P_xO_(1-y)F_y

The recent discovery of high-temperature superconductivity in iron-based pnictides (chalcogenides) not only triggers tremendous enthusiasm in searching for new superconducting materials, but also opens a new avenue to the study of the Kondo physics. CeFeAsO is a parent compound of the 1111-type iron-based superconductors. It shows 3d-antiferromagnetic (AFM) ordering below ～ 139 K and 4f-AFM ordering below ～ 4 K. On the other hand, the phosphide CeFePO is a ferromagnetically correlated heavy-fermion (HF) metal with Kondo scale T K ～ 10 K. These properties set up a new platform for research of the interplay among magnetism, Kondo effect, and superconductivity (SC). In this review, we present the recent progress in the study of chemical pressure effect in CeFeAsO 1-y F y (y = 0 and 0.05). This P/As-doping in CeFeAsO serves as an effective controlling parameter which leads to two magnetic critical points, x c1 0.4 and x c2 0.92, associated with suppression of 3d and 4f magnetism, respectively. We also observe a turning point of AFM-FM ordering of Ce 3+ moment at x c3 0.37. The SC is absent in the phase diagram, which is attributed to the destruction to Cooper pair by Ce-FM fluctuations in the vicinity of x c1 . We continue to investigate CeFeAs 1-x P x O 0.95 F 0.05 . With the separation of x c1 and x c3 , this chemical pressure results in a broad SC region 0≤ x ≤ 0.53, while the original HF behavior is driven away by 5% F doping. Different roles of P and F dopings are addressed, and the interplay between SC and Ce-4f magnetism is also discussed.     

Upper Critical Fields and Anisotropy of BaFe1.9Ni0.1As2 Single Crystals

Temperature dependence of the upper critical magnetic field （Hc2） near Tc of 20 K in a BaFe1.9 Ni0.1 As2 single crystal is determined via magneto-resistance measurements, for the out-plane （H ⊥ab） and in-plane （H ｜｜ ab） directions in magnetic fields of up to 8 T. The upper critical fields at zero temperature estimated by the Werthamer-Helfand- Hohenberg （WHH） formula are μ0H^｜｜ c2（0） = 137 T and μ0H⊥c2（0） = 51 T, both exceeding the weak-coupling Pauli paramagnetic limit （μ0Hp = 1.84Tc）. However, the WHH formula could overestimate the μ0H^｜｜12（0） value. The anisotropy of upper critical fields is around 3 in the temperature range close to Tc. The result is very similar to the Co-doped 122 superconductor BaFe2-x Cox As2, indicating that electron-doped 122 superconductors exhibit similar superconducting properties.     

无规分形衬底上银膜逾渗系统的交流特性

通过对沉积在具有无规自相似结构的α-Al₂O₃断裂面上的银薄膜逾渗系统交流特性的测量,证明了在逾渗阈值p_c附近这一系统的交流电导率和介电常数满足指数临界规律和普适标度关系。还给出了这种逾渗系统的电容与直流电阻的关系,并对其意义作了讨论。 关键词：     

氧缺位对单相YBa2Cu3O7-x热电势率的影响

研究了氧缺位对单相YBa₂Cu₃O_7-x体系超导电性及热电势率的影响。结果表明,超导转变温度随氧缺位的增加而下降,热电势率随氧缺位的增加而增大。由实验结果推断,单相YBa₂Cu₃O_7-x的多数载流子为空穴。存在较大的声子曳引热电势表明。在YBa₂Cu₃O_7-x超导体中存在较强的电-声子相互作用。 关键词：     

Co,Zn元素对YBa2Cu3O7-δ的不同的掺杂效应

对单相掺杂样品YBa₂Cu_3-xCo_xO_y (x=0.00,0.025,0.05,0.075,0.10,0.125,0.15,0.20,0.25,O.275,0.30,0.325,0.35,0.375,0.40)和YBa₂Cu_3-xZn_xO_y(x=O.025,0.05,0.075,0.10,0.15,0.20,0.30)作了室温下的 关键词：