激光淀积YBa2Cu3O7外延超导薄膜

利用准分子脉冲激光成功地在(100)SrTiO_3与(100)Y-ZrO_2衬底上淀积了 YBa_2Cu_3O_7超导薄膜,T_c(R=0)>90K,J_c(T<82K)>1×10~6A/cm~2.研究了衬底温度对外延YBa_2Cu_3O_7薄膜超导性能及结构的影响.     

用二维欧拉方法模拟滑移爆轰作用下金属圆筒的收敛运动

本文用二维流体-弹塑性欧拉编码对金属圆筒在滑移爆轰作用下的收敛运动作了数值模拟。文中考虑了起爆端对金属圆筒运动的影响,给出了圆筒自由面不同时刻的运动姿态和自由面速度随时间变化规律。计算结果与实验结果符合较好。     

液氮下工作的薄膜biPbSrCaCuO dc SQUID

利用电阻加热、单源混合分层蒸镀方法制备的 Bi PbSrCaCuO 超导薄膜,研制成功带双桥结的单圆孔的直流超导量子干涉器(dc SQUID).这些 dc SQUID 在78K 呈现出完全的周期性磁通响应的电压特性.在无屏蔽条件下,0—1Hz 频率范围内,78K 的磁通噪声的典型值为1.7×10~(-3)φ_0/(Hz)~(1/2),相应的能量分辨率为3.6×10~(-26)J/Hz.同时,我们发现了无偏置电流下的可以锁定的磁通响应的电压二次谐波现象,此现象尚未理解清楚,但它与 dc SQUID的 I—V 特性形状有密切关系,并对其进行了探讨.     

Alternating-current losses in two-layer superconducting cables consisting of second-generation superconductors coated by U-shaped ferromagnetic materials

Alternating-current losses in a two-layer superconducting cable, each layer being composed of 15 closely-spaced rectangular wires made up of second-generation superconductors when the ends of wires are coated by either a non-magnetic or strong ferromagnetic material having a U profile is numerically investigated. Computations are carried out through the finite-element method. The alternating-current losses do not increase significantly if the relative permeability of the coating is increased three orders of magnitude, provided that the current amplitude is less than half of the critical current in a superconducting wire. However, the losses are much higher for ferromagnetic coating if the amplitude of the applied current oscillating at 50 Hz is close to the critical current. The ferromagnetic coating is seen to accumulate the magnetic field lines normally on its surfaces, while the field lines are parallel to the long axes of the wires, leading to more significant flux penetration in the coated regions. This facilitates a uniform low-loss current flow in the uncoated regions of the wires. In contrast, coating with a non-magnetic material gives rise to a considerably smaller current flow in the uncoated regions, whereas the low-loss flow is maintained in the coated regions. Moreover, the current flows in opposite directions in the coated and uncoated regions, where the direction in each region is converse for the two materials.     

波纹管对超导电缆出口液氮温度的影响

建立了30米长高温超导电缆的二维模型,利用Fluent软件对该模型进行仿真分析。在该模型中,采用波纹管恒温器,分析了波纹管的波距、波高等因素对出口液氮温度的影响。结果表明:在相同的热负荷及流量下,波纹管的波距越小,波高越大,出口液氮温度越高。超导电缆波纹管内液氮温度模拟,为低温冷却系统的优化设计提供理论依据。     

Fabrication of rhenium Josephson junctions

Rhenium is a superconductor with a relatively weak tendency to oxidize, which is advantageous in superconducting quantum circuit and qubit applications. In this work, Re/A1-A1Ox/Re Josephson tunnel junctions were fabricated using a selective film-etching process similar to that developed in Nb trilayer technology. The Re films had a superconducting transition temperature of 4.8 K and a transition width of 0.2 K. The junctions were found to be highly reproducible using the fabrication process and their characteristics had good quality with a low leakage current and showed a superconducting gap of 0.55 meV.     

Progress in superconducting qubits from the perspective of coherence and readout

Superconducting qubits are Josephson junction-based circuits that exhibit macroscopic quantum behavior and can be manipulated as artificial atoms.Benefiting from the well-developed technology of microfabrication and microwave engineering,superconducting qubits have great advantages in design flexibility,controllability,and scalability.Over the past decade,there has been rapid progress in the field,which greatly improved our understanding of qubit decoherence and circuit optimization.The single-qubit coherence time has been steadily raised to the order of 10 to 100μs,allowing for the demonstration of high-fidelity gate operations and measurement-based feedback control.Here we review recent progress in the coherence and readout of superconducting qubits.     

FeTe合金结构分析及其薄膜制备

利用固态反应法制备了名义成分为FeTe的合金, 采用X射线粉末衍射技术和Rietveld全谱拟合分析方法测定了其相组成和晶体结构. 研究表明,主相为Fe_1.08Te,空间群为P4/nmm,点阵参数 a = 3.8214(3) Å, c = 6.2875(3) Å, Z = 2, Fe原子占据2a和2c晶位, Te原子占据2c晶位. 利用脉冲激光沉积技术制备的FeTe薄膜超导转变起始温度为13.2 K,零电阻温度为9.8 K. 关键词： FeTe Rietveld结构精修 超导薄膜