cited:7

Characterizations of the electrothermal parameters of a transition edge sensor microcalorimeter and its energy resolution

Article Number:Article 100051 Corresponding Author: Bo Gao Author:Yue Zhao, Hubing Wang, Bo Gao, Zhen Wang Article preview
Abstract
We developed a transition-edge sensor microcalorimeter (μ-calorimeter) using Mo/Au/Au thin films. We report the detector fabrication, the measurements of the electrothermal parameters and the noise characterizations of the transition-edge sensor μ-calorimeters. We estimated the energy resolution of the μ-calorimeter using the measured noise spectrum and the calculated power-to-current responsivity. Using a 55Fe radioactive X-ray source, we characterized the detector responses to incident photons at various working points. The best instrumental energy resolution achieved was 4.13 eV @ 5.9 keV, which agrees qualitatively with the resolution of 4.01 eV estimated from the noise spectrum.
Review
cited:6

Field and current driven versions of Brandt method for calculating transport ac loss of superconducting cylinder and strip

Article Number:Article 100052 Corresponding Author: Xiao-Fen Li Author:Xiao-Fen Li, Shuo Li, Du-Xing Chen Article preview
Abstract
As an elegant and fast numerical tool for solving time-dependent electromagnetic field problems in hard superconductors, Brandt’s method has played an important role in understading the magnetic behavior of superconducting strips, discs, bars and cylinders in various aspect ratios. However, the application of this convenient method was mainly in magnetization processes. Traditionally, the solution of current transport problem needs to introduce a driving electric field Ea, which requires a low efficiency iterative process and Ea itself was not clearly explained. In this work, three integral algorithms based on the Brandt’s method are developed to deal with current transport problems, which directly adopt the applied current as a boundary condition. Namely the current (I)-driven version and two current-field-driven versions A and B. Moreover, the arbitrary applied magnetic field can also be included in the I-driven version. The derivation with all necessary formulas for the methods are given in this work. As an example, the new methods, as well as the traditional method are used for calculating transport ac loss Q of a superconducting cylinder or strip obeying a power-law relation of EJn as a function of a given I(t). Derived from the Ampère law and the differential rather than the integral expression of the Faraday law, the current-driven version can be used for more accurate and much quicker computation. Being an intermediate quantity, Ea(t) in the two current-field-driven versions is accurately calculated under the given I(t), but version B is much quicker than A. Problems relating to Ea(t) and Q stabilization process are discussed.
Review
cited:17

Electrical, magnetic and thermal circuit modelling of a superconducting half-wave transformer rectifier flux pump using Simulink

Article Number:Article 100053 Corresponding Author: A.C. Francis Author:A.C. Francis, S. Venuturumilli, D.A. Moseley, S. Claridge, B. Leuw, R.A. Badcock, C.W. Bumby Article preview
Abstract
Superconducting flux pumps (FP) are capable of supplying superconducting circuits with high currents by additively supplying current over a number of cycles without introducing large amounts of heat into the cryogenic environment. Superconducting FPs can be broadly classified into two types: dynamo and transformer rectifier. Modelling the behaviour of these systems is an emerging field. In this work a model of a half wave magnetically switched transformer rectifier FP created in MATLAB/Simulink/Simscape is presented. Unlike existing models, the characteristics of all circuit elements are fully integrated allowing all superconducting elements to be accurately incorporated. The presented method uses pre-calculated look-up tables, populated with experimentally derived material qualities to simulate these superconducting elements. The thermal evolution of the switches, calculated simultaneously to the magnetic field switching interaction has also been included. This model is compared to the performance of a real world FP during the pumping of a load coil and is found to be accurate. Furthermore, the presented model illustrates how small amounts of heating at a magnetic switch can profoundly affect a FPs performance over many cycles.
Review
cited:32

Bending performance analysis on YBCO cable with high flexibility

Article Number:Article 100054 Corresponding Author: Qiong Wu, Jinggang Qin Author:Huan Jin, Qiong Wu, Guanyu Xiao, Chao Zhou, Haihong Liu, Yunfei Tan, Fang Liu, Jinggang Qin Article preview
Abstract
In order to utilize high-temperature superconducting Yttrium Barium Copper Oxide (YBCO) tapes to develop superconducting cables for high magnet field applications, it is critical to ensure the stable operation of the YBCO cable under challenging mechanical and thermal conditions. A new type of cable featuring the winding of YBCO and copper tapes around a spiral stainless steel tube has been proposed to increase flexibility and cooling. Experiments are performed to confirm that its critical current varies with the bending diameter. The cables wound with nine YBCO tapes in three layers show a critical current degradation of less than 5% for a bending diameter of 30 mm. The performance of the cable degrades as the number of wound layers increases. The critical current degradation of cable specimens wound from 15 tapes in five layers reached approximately 12% for a bending diameter of 30 mm. In addition, when compared to traditional CORC cable specimens, the developed cable specimens show better-bending flexibility and achieve a lower critical bending diameter. The finite element models show that the higher elasticity coefficient and lower plasticity of the stainless steel spiral tube results in a lower strain on the YBCO tapes of the HFRC cable than that of the CORC cable, and the maximum strain on the YBCO tapes of the HFRC cable was only about 10% of that of the CORC cable. Therefore, it is less likely that the YBCO tape in this type of cable will reach the irreversible strain limit during bending, resulting in a degradation in current carrying performance. Furthermore, the cooling efficiency can be improved by flowing the cooling medium inside the central core, which can significantly improve its thermal stability. These advantages indicate the possibility of using it in future high-field magnets with high current carrying capacity at fields greater than 15 T.
Review
cited:16

Estimation of critical current density of bulk superconductor with artificial neural network

Article Number:Article 100055 Corresponding Author: Huadong Yong Author:Gangling Wu, Huadong Yong Article preview
Abstract
In the applications of superconducting materials, the critical current density Jc(B) is a crucial performance parameter. The conventional method of measuring Jc(B) of bulk superconductor is magnetization method. However, there are errors in the estimation of Jc(B) in the lower field, and the estimation is not applicable in the region where the magnetic field reverses. In this paper, Jc(B) of the bulk superconductor is determined by the hysteresis and magnetostriction loops with artificial neural network (ANN), respectively. Compared with double-output ANN, the critical current density obtained by single-output ANN is more accurate. Finally, the prediction results given by the hysteresis and magnetostriction loops are discussed.
Review
cited:16

32 × 32 NbN SNSPD array based on thermally coupled row-column multiplexing architecture

Article Number:Article 100056 Corresponding Author: Hao Li, Lixing You Author:TianZhu Zhang, You Xiao, HuiQin Yu, Jia Huang, ChaoLin Lv, LingDong Kong, XiaoYu Liu, Hao Li, LiXing You, Zhen Wang Article preview
Abstract
We report a superconducting nanowire single-photon detector (SNSPD) array aiming for a near-infrared 1550-nm wavelength that consists of 32 × 32 nanowire pixels and an area of 0.96 mm × 0.96 mm. Unlike most reported large-scale SNSPD arrays with amorphous films, NbN superconducting nanowires are employed in our array, which allows the detector operation at 2.3 K provided by a compact two-stage Gifford–McMahon cryocooler. Thermally coupled row–column multiplexing is employed in our arrays to avoid current redistribution and loss of electrical signal occurring in the electrically coupled row–column architecture. The fabricated detector array shows a pixel yield of 94% and maximal intrinsic efficiencies of 77% and 96% at 1550 nm and 405 nm, respectively. The timing jitter and the thermal coupling probability are also investigated.
Review
Current page19, Total Pages32, Total Record192 First Prev ...1718192021... Next Last Goto
Superconductivity One-Stop Service Platform
TOP