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Transport and microwave properties of yttrium barium(2) copper(3) oxygen(7-x) superconducting films.

机译:钇钡(2)铜(3)氧(7-x)超导薄膜的传输和微波特性。

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High quality YBCO c-axis oriented films were made by a laser ablation technique. Josephson weak links were fabricated on a modified microbridge by using bicrystal YBCO films. Shapiro steps were observed on modified microbridge weak links.; Vortex ring nucleation by thermal activation and quantum tunneling processes in high {dollar}Tsb{lcub}c{rcub}{dollar} superconductors is discussed. The nonlinear resistance scales as {dollar}esp{lcub}-(Jsbnu/J)spnu{rcub}{dollar}. Thermal activation yields a critical index of {dollar}nu{dollar} = 1, while quantum tunneling (without normal current dissipation) yields {dollar}nu{dollar} = 2. I-V characteristics were measured on both disordered (low {dollar}Jsb{lcub}c{rcub}{dollar}), ordered (high {dollar}Jsb{lcub}c{rcub}{dollar}) YBCO films and microbridges below {dollar}Tsb{lcub}c{rcub}{dollar}. The data were examined in terms of both thermal activation and quantum tunneling models. For a disordered film, the {dollar}nu{dollar} = 1 scaling law is in reasonable agreement with the data, while {dollar}nu{dollar} = 2 scaling is required to explain the results of an ordered film at low temperatures. For the microbridge, the {dollar}nu{dollar} = 2 scaling extended even to high temperatures.; Intrinsic critical current densities in high {dollar}Tsb{lcub}c{rcub}{dollar} superconducting films are discussed. The enhancement of the quantum electrodynamic tunneling process due to normal current dissipation is proposed to explain the measured {dollar}Jsb{lcub}c{rcub}{dollar} results for YBCO films. The depairing current density calculated from vortex ring model is in the order of 10{dollar}sp9{dollar} {dollar}A/cmsp2{dollar} and an upper limit of {dollar}Jsb{lcub}c{rcub}{dollar} is in the order of 10{dollar}sp7{dollar} {dollar}A/cmsp2{dollar}. Supercurrent was observed to flow across a bridge constriction with a {dollar}Jsb{lcub}c{rcub}{dollar} up to 1.3 {dollar}times{dollar} 10{dollar}sp9{dollar} {dollar}A/cmsp2{dollar}, the highest critical current density yet reported. The limitation of {dollar}Jsb{lcub}c{rcub}{dollar} appears to be due to vortex ring creation. We found that studying {dollar}Jsb{lcub}c{rcub}{dollar} of bridge constrictions was a way to approach the depairing current limit.; A novel microwave self-resonant (MSR) technique was developed to measure surface resistance, {dollar}Rsb{lcub}s{rcub}{dollar}, of YBCO superconducting films directly and surface reactance, {dollar}Xsb{lcub}s{rcub}{dollar}, indirectly. {dollar}Rsb{lcub}s{rcub}{dollar} at 21 GHz decreased by about three orders of magnitude as the temperature decreased from 90K to 80K. The smallest surface resistance was 2.7 {dollar}times{dollar} 10{dollar}sp{lcub}-4{rcub}Omega{dollar} at 21 GHz and at 15K, and the surface reactance was 0.031{dollar}Omega{dollar}. Using the MSR technique, we measured the London penetration depth and coherence length, and found that both {dollar}lambda{dollar} and {dollar}xi{dollar} were anisotropic, their values depended on the direction of the microwave electric field relative to the c-axis. We found that {dollar}lambdasbVert{dollar}(0) (penetration depth in a-b plane at zero temperature) was about 1840A and {dollar}lambdasbperp{dollar}(0) about 3640A, while {dollar}xisbVert{dollar}(0) {dollar}sim{dollar} 25A and {dollar}xisbperp{dollar}(0) {dollar}sim{dollar} 11A. The Ginzburg-Landau parameters were {dollar}kappasbVert{dollar} in the range of 110-165 and {dollar}kappasbperp{dollar} in the range of 62-74, yield an anisotropic factor {dollar}gamma{dollar} about 2.
机译:通过激光烧蚀技术制成高质量的YBCO c轴取向薄膜。约瑟夫森的薄弱环节是通过使用双晶YBCO薄膜在改性微桥上制造的。在改良的微桥薄弱环节上观察到了夏皮罗台阶。讨论了高Tsb {lcub} c {rcub} {dollar}超导体中热活化和量子隧穿过程的涡环形核。非线性电阻的缩放比例为{doles} esp {lcub}-(Jsbnu / J)spnu {rcub} {dollar}。热活化产生的临界指数为{dol} nu {dollar} = 1,而量子隧穿(无正常电流耗散)的结果为{dollar} nu {dollar} =2。在两种无序(低{dollar} Jsb {lcub} c {rcub} {dollar}),订购(高{dollar} Jsb {lcub} c {rcub} {dollar})低于{dollar} Tsb {lcub} c {rcub} {dollar}的YBCO薄膜和微桥。根据热活化和量子隧穿模型对数据进行了检查。对于无序胶片,{dol} nu {dollar} = 1缩放定律与数据合理吻合,而{dollar} nu {dollar} = 2缩放则需要用来解释有序胶片在低温下的结果。对于微桥,{dol} nu {dollar} = 2的缩放比例甚至扩展到了高温。讨论了高Tsb {lcub} c {rcub} {dollar}超导薄膜的本征临界电流密度。提出了由于正常电流耗散而引起的量子电动力学隧穿过程的增强,以解释YBCO膜的测量结果。根据涡环模型计算出的去对电流密度为10 {dol}} 9 {dol}} a / cmsp2 {dol},上限为{s} Jsb {lcub} c {rcub} {dol}的顺序为10 {dollar} sp7 {dollar} {dollar} A / cmsp2 {dollar}。观察到过电流以{dols} Jsb {lcub} c {rcub} {dollar}穿过桥颈缩流,直至1.3 {dollar} times {dollar} 10 {dollar} sp9 {dollar} {dollar} A / cmsp2 {美元},这是迄今报道的最高临界电流密度。 {dollar} Jsb {lcub} c {rcub} {dollar}的限制似乎是由于涡流环的产生。我们发现,研究桥梁收缩的{dollar} Jsb {lcub} c {rcub} {dollar}是一种接近限制电流极限的方法。已开发出一种新颖的微波自谐振(MSR)技术来直接测量YBCO超导薄膜的表面电阻{dols} Rsb {lcub} s {rcub} {dollar}和表面电抗{dollar} Xsb {lcub} s { rcub} {dollar},间接。随着温度从90K降低到80K,21 GHz的{rsb {lcub} s {rcub} s {rcub} {dollar}降低了大约三个数量级。在21 GHz和15K时,最小表面电阻为2.7 {dollars} {dollar} 10 {dollar} sp {lcub} -4 {rcub} Omega {dollar},表面电抗为0.031 {dollar} Omega {dollar} 。使用MSR技术,我们测量了伦敦的穿透深度和相干长度,发现{dollar} lambda {dollar}和{dollar} xi {dollar}都是各向异性的,它们的值取决于微波电场相对于c轴。我们发现{dollar} lambdasbVert {dollar}(0)(零温度下ab平面中的穿透深度)约为1840A,{dolmb} lambdasbperp {dollar}(0)约为3640A,而{dollar} xisbVert {dollar}(0 ){dollar} sim {dollar} 25A和{dollar} xisbperp {dollar}(0){dollar} sim {dollar} 11A。 Ginzburg-Landau参数的{dollar} kappasbVert {dollar}在110-165的范围内,并且{dollar} kappasbperp {dollar}在62-74的范围内,产生约2的各向异性因子{dollar} gamma {dollar}。

著录项

  • 作者

    Jiang, Hua.;

  • 作者单位

    Northeastern University.;

  • 授予单位 Northeastern University.;
  • 学科 Physics Condensed Matter.
  • 学位 Ph.D.
  • 年度 1992
  • 页码 200 p.
  • 总页数 200
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 O49;
  • 关键词

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