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1.
YBa_2 Cu_3 O_(7-δ)/BaZrO_3(YBCO/BZO) composite film with enhanced flux-pinning performance was prepared on LaAlO_3(LAO) substrate via a fluorine-free sol-gel method in combination with a novel photosensitive sol-gel lithography technique.Owing to the difference of lattice mismatch between the interfaces of YBCO/LAO and YBCO/BZO,high-density stacking faults were successfully introduced into YBCO matrix,which has been confirmed by XRD and HRTEM analysis.Magnetization measurement results indicate that YBCO/BZO composite film has a stronger current-carrying capacity than the pure YBCO film especially under applied magnetic fields.However,the critical current density of YBCO/CeO_2 composite film is much lower than that of the pure YBCO film at all the applied magnetic fields due to the chemical reaction between YBCO and CeO_2.Therefore,it can be concluded that the flux-pinning performance of YBCO film can be improved by the lattice distortions within YBCO matrix as long as the metal oxide microarrays cannot react with YBCO films.  相似文献   

2.
高温超导材料YBa2Cu4O8(YBCO)和铁磁材料La2/3Ca1/3MnO3(LCMO)形成的三层薄膜LCMO/YBCO/LCMO由对靶溅射技术制得.与YBCO单层薄膜相比,由于超导/铁磁系统中的磁性邻近效应,三层薄膜表现出较低的超导转变温度(Tc,ON).与LCMO单层膜相比,三层薄膜的金属半导体转变温度(TMS)被提高并且强烈依赖于YBCO层的厚度.随中间层厚度的变化,磁电阻显示出非单调行为,长振荡周期被发现.结果表明,当YBCO处于正常态时两层LCMO膜之间存左着磁性自旋相互作用.  相似文献   

3.
应用磁控溅射法在SrTiO3(STO)单晶基片上原位制备了Pb(Zr,Ti)O3/YBaCu3O7(PZT/YB-CO)异质结,X射线衍射、透射电镜和选区电子衍射结果表明PZT/YBCO为外延生长,磁化率的测量结果表明YBCO的超导转变温度接近90 K,外延铁电体/超导体异质结的制备为进一步研究铁电性、超导性以及铁电体/超导体复合器件奠定了基础.  相似文献   

4.
运用HP4284A通过对不同质量样品的实验研究比较,对PZT/YBCO异质结电容值在超导临界温区的跳变行为进行了系统的研究,以一个物理参数等效电路模型,揭示了PZT/YBCO异质结电容值在超导临界温区跳变行为的起因,给出薄膜的漏电阻,氧化物电极的自电阻及测试所用信号频率与超导临界转变温度区电容跳变幅度间的定量关系。  相似文献   

5.
A frequency mixing system including microwave coupling and intermediate frequency (IF) measurement arrangements is designed. In lieu of liquid nitrogen, a pulse tube cryocooler is used to cool the whole system. With YBa2Cu3O7/Yttrium stabilized zirconia (YBCO/YSZ) bicrystal Josephson junction as the mixing element, 36th harmonic frequency mixing at the 8 mm waveband is obtained.  相似文献   

6.
YBCO掺杂效应研究   总被引:3,自引:0,他引:3  
介绍了YBCO掺杂的基础知识,总结了YBCO各个位置采用典型元素掺杂而导致的超导电性和结构的变化,阐述了掺杂对YBCO的重要影响,并简介了当前YBCO掺杂效应研究中的几个热点问题.  相似文献   

7.
研究了MTG法制备的YBCO超导体中的211相含量与名义配比的关系,用SEM观察了样品中211相的分布,用磁滞回线测量法估算了YBCO超导体的临界电流密度与样品中211相含量的关系,总结出YBCO超导体中起钉扎中心作用的211相含量的最佳值。  相似文献   

8.
第二代高温超导带材YBa2Cu3O7-δ(YBCO)具有高载流能力、高不可逆场、低交流损耗和高转变温度,成为当前的热点研究对象.采用低成本的电泳沉积技术在Hastelloy合金上成功制备了YBCO超导层.添加剂对电泳液的稳定性及涂层性能有着重要影响.实验研究了添加剂(种类选择及添加量)与YBCO超导层的关系.结果表明,添加005gPVB时所制备的样品具有较好的超导电性,其临界电流密度可达100A/cm2(0T,77K).  相似文献   

9.
建立一个含有圆形夹杂和纵向贯穿共线裂纹的YBCO超导平板模型,在外加磁场产生洛伦兹力的作用下,研究含有夹杂的YBCO超导体中两个共线裂纹的相互作用,采用Bean模型描述超导体的电磁行为.通过确定裂纹尖端的应力强度因子(SIFs)并进行相关的磁弹性应力分析.结果表明外磁场大小、粘性磁通量流速v0夹杂物的大小、裂纹长度、夹杂半径以及夹杂与基体杨氏模量之比对应力强度因子都有影响.  相似文献   

10.
本文用半经验CNDO/2量子化学计算方法,对YBCO的结构单元及晶胞作了计算,结果指出:1.采用簇模型不能较好地反映YBCO晶体性质。2.YBCO中Cu(2)的氧化态为( 2),Cu(1)的氧化态为( 1.5),Cu(1)也可能是在( 2)与( 1)两个氧化态之间共振。3.铜的电子组态分别为Cu(2)(d_(xy)~2d_(x2)~2d_(yz)~2d_(x~2-y~2)~1d_z~(2_2)),Cu(1)(d_(xy)~2d_(xz)~2]d_(yz)~2d_(x~2-y~2)~2d_(z~2)~1)。这种组态是YBCO形成层状氧缺位结构的主要原因。4.超交换作用在YBCO中普遍存在,但铜-氧面间这种作用最大,超导电流在其间进行最为有利。5.Y,Ba在YBCO中的主要作用是促成Cu(d_(xy))与O(P)形成最高占领杂化带。  相似文献   

11.
夏红伟  胡学飞 《科技信息》2011,(1):33-34,413
固体氧化物燃料电池(SOFC)具有稳定性高、寿命长、污染低等优点,是二十一世纪的绿色能源之一。当前SOFC阴极通常采用掺杂的ABO3钙钛矿型材料。这类材料在高温下具有较高的导电率和催化活性,但中温化是SOFC的趋势,高温下常用的La(Sr)MnO3阴极材料在中温下性能下降,不能满足中温下电导率的要求。本论文尝试采用柠檬酸燃烧法来制备YBa2Cu3O7-δ,并在YBCO中加入一定量的Sm2O3掺杂的Ce2O3(SDC)作为SOFC的阴极材料,通过对阻抗分析,研究了SDC掺杂量、烧结温度等对该阴极材料性能的影响。实验结果表明:随着SDC的掺杂量x(0≤x≤50%)和烧结温度的升高,阴极材料的界面阻抗减小。在SDC的掺杂量为50%时,且在800℃下烧结得到的烧结体界面阻抗最小,其界面比电阻仅为0.1353ohm/cm2(800℃),这标志着掺杂SDC的YBCO作为中温固体氧化物燃料电池的阴极材料时非常具有发展前景的。  相似文献   

12.
本文采用顶部籽晶熔融织构法(TSMTG)成功地将Bi2O3掺杂到YBCO超导块材中,研究了Bi2O3掺杂含量对单畴YBCO超导块材生长形貌和磁悬浮力的影响.结果表明,在YBa2Cu3O7-δ(Y123):Y2BaCuO5(Y211)=1:0.4不变的情况下,掺杂的Bi2O3粉体在样品内部均生成了Y2Ba4CuBiOx纳米粒子.当Bi2O3添加量x≤1.5wt%时,样品均可长成完整的单畴YBCO超导块材,且样品的磁悬浮力随着Bi2O3掺杂量的增加而增大;当x1.5wt%时,YBCO超导块材的单畴区域随着Bi2O3掺杂量的增加而逐渐减小,且随机成核现象严重,磁悬浮力降低;当x=1.5wt%时,样品的磁悬浮力最大.该结果对缩短样品制备的周期及进一步提高超导块材性能具有十分重要的意义.  相似文献   

13.
Recent development of a high-performance narrowband high-temperature superconducting (HTS) filter is presented. A 10-pole quasi-elliptic function response filter with two pairs of transmission zeros (for high selectivity), which has a center frequency of 2.185 GHz and a 3 dB bandwidth of 10 MHz (a fractional bandwidth of 0.45%), is introduced. The filter was fabricated on a 40 mm×16 mm×0.5 mm MgO wafer with double-sided YBCO films. The measured results show that the filter has 0.15 dB insertion loss at the ...  相似文献   

14.
采用顶部籽晶熔渗工艺(TSIG)制备出了配比为Bi2O3:Y2BaCu05=x:(1吨)的系列单畴YBCO超导块材(其中x=0.1,0.3,0.5,0.7,0.9,2,单位为wt%),并且研究了不同比例的氧化物Bi2O3掺杂对样品的生长形貌、磁悬浮力以及其微观结构的影响.实验结果表明了,Bi20,粒子的掺杂在样品中生成Y2Ba4CuBiOx(YBi2411)纳米粒子从而可以有效地提高样品的磁悬浮性能.当Bi203粒子掺杂量x从0.1wt%(质量分数,下同)增加到0.7wt%时,样品的磁悬浮力从7N增加到25N;当其掺杂量从0.7wt%增加到2wt%时,样品的磁悬浮力从25N降低到6N.该实验结果对于我们进一步研究氧化物掺杂对磁通钉扎作用的影响以及提高YBCO超导块材的性能有着重要的影响.  相似文献   

15.
Development of miniature HTSC wide-band filter with open-loop resonators   总被引:1,自引:0,他引:1  
The strong electric and magnetic coupled novel HTSC (high temperature superconductor) open-loop microstrip resonators are studied in this report and the traditional structure of open-loop resonators is improved. A miniature wide-band HTSC bandpass filter is developed by the novel structure, which is fabricated on YBCO/LaAIO3/YBCO substrate with dimensions of 14.8×9.6 mm^2. This filter is tested at 77 K, and the specifications are that the center frequency is 2230 MHz, the bandwidth is 455 MHz, and the best insertion loss is 0.14 dB in passband.  相似文献   

16.
Following the discovery of type-II high-temperature superconductors in 1986 (refs 1, 2), work has proceeded to develop these materials for power applications. One of the problems, however, has been that magnetic flux is not completely expelled, but rather is contained within magnetic fluxons, whose motion prevents larger supercurrents. It is known that the critical current of these materials can be enhanced by incorporating a high density of extended defects to act as pinning centres for the fluxons. YBa2Cu3O7 (YBCO or 123) is the most promising material for such applications at higher temperatures (liquid nitrogen). Pinning is optimized when the size of the defects approaches the superconducting coherence length ( approximately 2-4 nm for YBCO at temperatures < or =77 K) and when the areal number density of defects is of the order of (H/2) x 10(11) cm(-2), where H is the applied magnetic field in tesla. Such a high density has been difficult to achieve by material-processing methods that maintain a nanosize defect, except through irradiation. Here we report a method for achieving a dispersion of approximately 8-nm-sized nanoparticles in YBCO with a high number density, which increases the critical current (at 77 K) by a factor of two to three for high magnetic fields.  相似文献   

17.
The perspectives of fast three-terminal (3T) super- conducting devices with considerable gain have triggered many research activities on suppression of superconductivity; especially on that in high-Tc superconductors[1—3] and many achievements have been obtained. Unfortunately, certain factors such as current superposition and heating are overlooked in some experiments, thus leaving much room for improvement. With YBCO micro-bridges, we have looked at quasiparticle injections in the forms o…  相似文献   

18.
本文采用顶部籽晶熔融织构法(TSMTG)成功地将纳米Y2Ba4CuBiOx(YBi2411)引入了YBCO超导块材,研究了YBi2411掺杂量对单畴YBCO超导块材晶体生长形貌和磁悬浮力的影响.结果表明,YBi2411在YBCO超导块材中呈现出直径约100 nm~200 nm的纳米点状粒子和直径约100 nm~200nm,长约2μm的纳米棒状粒子.当YBi2411添加量x≤8 wt%时,样品均可长成完整的单畴YBCO超导块材,样品的磁悬浮力随着YBi2411掺杂量的增加而增大;当x≥8 wt%时,样品均可长成一定的单畴区,但随着YBi2411掺杂量的增加,YBCO超导块材的单畴区域逐渐减小,且随机成核现象越来越严重,同时磁悬浮力逐渐减小;当x=8 wt%时,样品磁悬浮力最大.在此基础上,结合超导材料的微观形貌,分析了YBi2411掺杂量对单畴YBCO超导块材磁悬浮力的影响.  相似文献   

19.
We have fabricated M doped (M = Al, Co, Fe, Ga, Ni and Zn) PrBa2Cu3O7(PBCO), i.e. PrBa2(CU1-xMx)3O7. The doping levels x are 0.05, 0.10, 0.15, and 0.20. X-ray data indicated no significant second phase for substituting Cu by Al, Co, Fe and Ga up to 20%. However impurity phases were detected for Ni and Zn substituted samples with doping levels equal to and higher than 15%. At 77 K the electrical resistivity of these compounds is orders in magnitude higher than that of PBCO. We also found that although the lattice parameters in the doped samples differ from PBCO, all samples remain orthorhombic. The lattice parameters of the doped sample are very close to those of YBa2CU3O7-δ (YBCO) and PBCO. For this reason these compounds are better materials to be used as the I-layer for YBCO SIS junctions. Results of structural and transport studies on 2000 A thick PrBa2[Cu0.80G0.2]3O7 (PBCGO) and YBCO/PBCGO multilayers are presented in this paper.  相似文献   

20.
The behavior of YBCO/metal bilayers under transport currents was explored in the framework of fault current limitation (FCL). Properties of the superconducting-normal transition were first studied phenomenologically during sweep current experiments. For current rates higher than 500A/s, the transition into the normal state was based on non-thermal phenomena and was characterized by a flux creep regime ended by a jump into the normal state. At lower sweep rates, a total diversion of the current in the metallic shunt was observed for temperatures higher than 85 K. In this regime, a partial recovery of the superconducting state took place due to a finite thermal resistance between the superconducting and the metallic films. These two properties of partial diversion into the shunt and of fast switching for a quick rise of the current during a default were exploited for current limitation at 77 K. FCL experiments at 50 Hz show that YBCO/Au bilayers limit the current in about 1 ms at a value of 2.5/c by developing electrical fields as high as 3 kV/m. Moreover, a recovery of the zero resistance state could occur under rated mode. A straightforward application of this property would be the transformer connection. Finally, results on DC current limitation and recovery under nominal mode were presented for the first time.  相似文献   

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