PrBa2Cu3O7不是一个内禀超导体

通过协同控制固相反应气氛和温度制备了接近化学计量的PrBa2Cu3O7多晶体。样品的X-射线衍射（XRD）未能检测出杂相。对XRD数据作Rietveld拟合，分析其结果，表明Pr占据Ba位非常少（≤1%）。磁测量显示Pr的反铁磁序温度为19.0K，比前人报导值高出2K，进一步证实样品中仅含有很少的Pr占据Ba位的缺陷。电、磁测量未能检测到任何超导迹象，说明PrBa2Cu3O7本身不是一个超导体。     

钒掺杂对Pb_2Sr_2Nd_（1．5）Ce_（0．5）Cu_3O_（10＋δ）

本文着重研究了钒对Ｐｂ－３２２２相成相的影响．当Ｎｄ３＋／Ｃｅ４＋为３：１时，通过钒掺杂简单方便地制备了单相性较好的Ｐｂ－３２２２相样品．本文还讨论了钒在Ｐｂ２Ｓｒ２—Ｎｄ１．５Ｃｅ０．５Ｃｕ３Ｏ１０＋δ中的可能位置．     

水合钴氧化物超导体的合成和表征

最近发现的水合钴氧化物超导体引起了超导领域的强烈兴趣．由于该超导体非常不稳定，因此有关该超导体的合成和表征是个重要的基本课题．本文报道几种典型的合成方法，并对所得到的超导体进行表征．我们将着重介绍利用歧化反应来制备含有很低的钠离子浓度和很高的水合氢离子浓度的钴氧化物超导体的新方法．     

Neutron Powder Diffraction Study on the Non-Superconducting Phases of ThFeAsN_(1-x)O_x(x=0.15,0.6)Iron Pnictide

We use neutron powder diffraction to study the non-superconducting phases of ThFeAsN_(1-x)O_x with x = 0.15,0.6.In our previous results of the superconducting phase ThFeAsN with T_c = 30 K,no magnetic transition is observed by cooling down to 6 K,and possible oxygen occupancy at the nitrogen site is shown in the refinement[Europhys.Lett.117(2017)57005].Here in the oxygen doped system ThFeAsN_(1-x)O_x,two superconducting regions(0≤x≤0.1 and 0.25≤x≤0.55)are identified by transport experiments[J.Phys.:Condens.Matter30(2018)255602].However,within the resolution of our neutron powder diffraction experiment,neither the intermediate doping x= 0.15 nor the heavily overdoped compound x = 0.6 shows any magnetic order from 300 K to 4 K.Therefore,while it shares the common phenomenon of two superconducting domes as most 1111-type iron-based superconductors,the magneticall.y ordered parent compound may not exist in this nitride family.     

Interplay of superconductivity and d-f correlation in CeFeAslPOl_yFy

The recent discovery of high-temperature superconductivity in iron-based pnictides （chalcogenides） not only trig- gers 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 corelated heavy-fermion （HF） metal with Kondo scale TK 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 CeFeAsOl_yFy （y = 0 and 0.05）. This P/As-doping in CeFeAsO serves as an effective controlling parameter which leads to two magnetic critical points, Xcl -- 0.4 and Xc2 - 0.92, associated with suppression of 3d and 4f magnetism, respectively. We also observe a turning point of AFM-FM ordering of Ce3＋ moment at Xc3 - 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 Xcl. We continue to investigate CeFeAsl-xPxO0.95Fo.os. With the separation of xcl and xc3, 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.     

CaCu3Ti4O12块材和薄膜的巨介电常数

用固相反应法和脉冲激光沉积(PLD)制备了CaCu₃Ti₄O₁₂块材和薄膜，获得了相对介电常数ε′（1kHz,300K)高于14000的介电特性，是目前该体系最好的结果.报道了(00l)取向高质量CaCu₃Ti₄O₁₂外延薄膜及其介电性质.C aCu₃Ti₄O₁₂相对介电常数ε′在100—300K温度范围 内 关键词： 3Ti₄O₁₂')" href="#">CaCu₃Ti₄O₁₂ 巨介电常数 PLD     

新型交生结构自掺杂铁基超导体

铁基高温超导体的基本结构单元是反萤石型Fe₂X₂层（X为磷族或硫族元素）,因此,设计具有Fe₂X₂层的新化合物成为探索铁基超导材料的有效途径.本文在回顾铁基超导体结构特征和基本结构类型的基础上,归纳总结了铁基超导体块层结构设计的基本原则;着重介绍迄今发现的几类具有层状交生（intergrowth）结构的新型自掺杂铁基超导材料.     

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。     

CaCu3Ti4O12块材和薄膜的巨介电常数

用固相反应法和脉冲激光沉积 (PLD)制备了CaCu3Ti4O1 2 块材和薄膜 ,获得了相对介电常数ε′( 1kHz ,3 0 0K)高于140 0 0的介电特性 ,是目前该体系最好的结果 .报道了 ( 0 0l)取向高质量CaCu3Ti4O1 2 外延薄膜及其介电性质 .CaCu3Ti4O1 2 相对介电常数ε′在 10 0— 3 0 0K温度范围内基本保持恒定 ,稳定性好 .基于跳跃电导模型 ,对CaCu3Ti4O1 2薄膜介电电导的频率依赖关系作了合理解释     

SYNTHESIS AT AMBIENT PRESSURE AND SUPERCONDUCTIVITY OF Hg-DOPED TI-BASED DOUBLE [(T1, Hg)-O]-LAYERED CDPHATES

The Hg-doped T1-based 2201 and 2212 phase layered cuprates have been successfully syn-thesized at ambient pressure and identified by X-ray powder diffraction and electron diffraction analysis. Compared with pure T1-based 2212 phase compound, there are indications that the corresponding Hg-doped T1-based compound (T1_1.8Hg_0.2)Ba₂CaCu₂O_z exhibits much higher T_c (> 132K).