超薄单晶基底本征约瑟夫逊结的制备

为了加强本征约瑟夫逊结(简称本征结)与高频电磁波信号的耦合,我们通过平面工艺手段获得了厚度小于伦敦穿透深度的超薄单晶基底,其厚度小于150nm.并在此基底上利用传统的mesa结构制备工艺制备了本征结.所制备的本征结超导性能没有发生明显的退化,与常规本征结的特性基本一致.     

Large mode area OmniGuide fiber with superconductor-dielectric periodic multilayers cladding

An OmniGuide fiber consisting of superconductor–dielectric cladding periodic multilayers is investigated. The theoretical results of the OmniGuide fiber are presented and compared with that of multicore photonic crystal fiber and step-index fiber. The large mode area and low loss with small bending radius are observed by the OmniGuide fiber.     

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分别采用机械打磨去镍加热镀锡工艺和反电镀去镍加电刷镀银工艺制作一对接头,然后对接头进行低温直流测试,测得前者的直流电阻为1.98n-,后者的直流电阻为1.53n-。对比分析可知,反电镀去镍和电镀银工艺更有效、更简单。这些工艺研究对ITER校正场线圈超导接头的制作具有重要指导意义。     

高温超导YBCO带材的交流传输电流损耗测量

文中对不同频率不同幅值的交变电流下高温超导体YBCO带材的交流传输损耗进行了实验研究。实验在77K下,对Superpower公司生产的SCS4050型号带材采用电测法通过锁相放大器进行了交流损耗值的测量,并将其工作电流为50Hz时的测量结果与Norris矩形模型估算值进行了对比,同时也给出了15Hz到300Hz不同频率下交流损耗测量结果的比较分析。     

超导太赫兹天线耦合微测辐射热检测器

超导太赫兹天线耦合微测辐射热检测器具备探测频段宽、响应速度快、灵敏度高、易于阵列化等特点因而具备广阔的应用前景.本文的主要工作是设计并微纳加工出基于氮化铌薄膜的超导器件,针对所制备器件的关键参数进行了表征.测试结果显示,当浴冷温度为4 K时,器件响应时间为4μs,噪声等效功率达到30 fW/Hz^0.5.基于所制备的器件进行了陶瓷刀被动扫描成像实验并取得了良好的成像效果.     

Chemical and Physical Analysis of Acetate-Oxide Sol-Gel Processing Routes for the Y-Ba-Cu-O System

The formation of three sols by fluorine-free aqueous and non-aqueous processes were analyzed and modified to vary the chemical properties of the sols (inks) to suit a variety of deposition processes such as dip-coating and ink-jet coating/printing. Ink-jet printing requires high wetting angles; choosing the right complexing agents to modify the ink allows the formation of droplets with high wetting angles on the surface. Dip-coating and ink-jet coating require low wetting angles; additives added to the sols reduce wetting angles to 10^∘ and allow complete coverage of the substrate surface. The deposition theories and requirements are briefly discussed, as are some initial tests with the printing and converting of the developed superconducting inks.     

Influence of partial substitution of zinc for copper on electronic structures of YBa2Cu3O y

Summary By use of an approximate band-structure treatment based on the EHMO approach, the energy band structures for the Zn-doped superconductor YBa₂Cu_3–x Zn _x O _y were calculated in the present paper and the influence of partial substitution of zinc for copper on the electronic structures for orthorhombic YBa₂Cu₃O_y was studied. From analysis of the band structures and the densities of states for YBa₂Cu_3–x Zn _x O _y , it was demonstrated that the 2D Cu-O planes in the Y-Ba-Cu-O superconducting system have a direct and dominant influence on superconductivity, whereas the role of the 1D Cu-O ribbons and the O(4) atoms is also of some importance.     

高价离子掺杂对Bi系成相和结构的影响(Ⅱ)

Sunshine等在BiSrCaCuO体系掺入Pb~(2+)取代部分Bi,经较长时间灼烧后.获得T_(c(0))?110 K以2223相为主的样品,Hongbao等又报导了用Sb部分取代Bi(Pb)SrCaCuO体系中的Bi的研究结果.我们曾用Sb~(5+)、Sn~(4+)、W~(6+)、Mo~(6+)等高价离子部分取代Bi,研究这些离子对BiSrCaCuO体系成相的影响,发现掺高价离子后2223相易于生成并易于得到T_(c(0))?111K的超导体.本文则进一步探讨高价离子掺入的影响及其加速2223相生成的原因。     

Critical Comment on “Numerical solution of Bloch–Gruneisen function to determine the contribution of electron–phonon interaction in polycrystalline MgB2 superconductor” by Intikhab A. Ansari [Physica C: Superconductors, 470 (2010) 508–510]

We present critical comments on the recent paper [Intikhab A. Ansari, Physica C: Superconductors, 470 (2010) 508] concerning numerical methods for solving Bloch–Gruneisen function and its applications to MgB₂ superconductor. It is demonstrated that the presented in this work the formulas and examples are not original and they are quite identical the formulas already established in our article [B.A. Mamedov, I.M. Askerov, Physics Letters A, 362 (2007) 324].     

Magnetization modification by superconductivity in Nb/Ni80Fe20/Nb trilayers

We present experimental evidences for magnetization modification by superconductivity in a series of Nb/Ni₈₀Fe₂₀/Nb trilayers. By monitoring the magnetization in a zero field as a function of temperature, we observed an irreversibility in magnetization between the cooling and warming branches just above the superconducting transition temperature T_c. These results suggest that the magnetization of the ferromagnetic Ni₈₀Fe₂₀ layer is reduced by the mutual interactions between the ferromagnet and superconductor. Moreover, this effect diminishes with increasing thickness of the Ni₈₀Fe₂₀ layer, which indicates that the interaction between the superconducting and magnetic layers occurs mainly at the vicinity of the interfaces.