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1.
将高温固相法制得的YBCO研磨,于无水乙醇中进行超声分散获得纳米YBCO/乙醇溶胶,随后掺入纳米金溶胶,浓缩、干燥得金掺杂的YBCO材料.结果发现,纳米金掺杂的YBCO/乙醇溶胶中粒子形成纳米链;掺杂适量金提高了YBCO的晶化程度;掺金量为0.025wt%~0.500wt%时,金/YBCO材料的超导转变温度丁Tc为93.84~92.01 K,但掺杂1%的金时,样品超导性能消失.若能进一步控制好掺金量,金掺杂YBCO的Tc也会相应得到提高.  相似文献   

2.
将高温固相法制得的YBCO研磨,于无水乙醇中进行超声分散获得纳米YBCO/乙醇溶胶,随后掺入纳米金溶胶,浓缩、干燥得金掺杂的YBCO材料.结果发现,纳米金掺杂的YBCO/乙醇溶胶中粒子形成纳米链;掺杂适量金提高了YBCO的晶化程度;掺金量为0.025wt%~0.500wt%时,金/YBCO材料的超导转变温度丁Tc为93...  相似文献   

3.
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   

4.
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   

5.
采用顶部籽晶熔融织构法,结合Y_2O_3和Y-211掺杂制备了高质量的准单畴YBCO块材.Jc测量结果表明,对于Y_2O_3掺杂的YBCO块材,其临界电流密度Jc在10K温度和0.6T磁场下达到1.60×10~6A/cm~2,用合作钉扎理论可推得,其在70K温度和2T磁场下为1.24×10~4/cm~2。扫描电镜观察结果表明,掺杂Y_2O_3所形成的Y-211粒子是柱状的,而掺杂Y-211在母体材料中是球形的,其尺寸接近纳米粒子。掺杂Y_20_3比Y-211更能增强磁通钉扎效应并有效地改善样品的生长状况。Y-211粒子与超导母体材料之间的界面对磁通钉扎起主要作用,Y-211粒子作为强钉扎中心属于界面钉扎。  相似文献   

6.
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   

7.
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   

8.
利用微带谐振技术研究了YBa2Cu3O7/LaAlO3 (YBCO/LAO)和YBa2Cu3O7/MgO (YBCO/MgO)超导薄膜的微波响应.通过测量微带谐振器的共振频率、有载品质因数、插入损耗与温度之间的依赖关系,分析了超导薄膜的微波特性,获得了超导薄膜在绝对零度时的穿透深度λ0.对于YBCO/LAO,λ0=265nm;对于YBCO/MgO,λ0=280nm.本文还利用微带谐振器研究了YBCO/LAO和YBCO/MgO超导薄膜的微波表面电阻.  相似文献   

9.
为了提高氧化钇钡铜(YBCO)超导体的捕获磁场,成功制备了单畴YBCO超导块材,研究了不同强度脉冲磁场和充磁次数对YBCO超导体捕获磁场的影响。结果表明:对直径20mm的YBCO超导体,存在一个最佳的脉冲磁场强度,使得捕获磁场最强;当采用最佳脉冲磁场充磁时,增加充磁次数可以显著增加YBCO超导体的捕获磁场。进一步采用Bean模型解释了该磁化规律。本文的研究结果有助于提高YBCO超导体的磁化效果和理解YBCO超导体的磁化机制。  相似文献   

10.
刘岗 《科技资讯》2011,(34):85-85
简单介绍了高温超导体YBCO体系的基本特征,系统介绍了YBCO体系不同位置、不同元素替代对其超导电性的影响。  相似文献   

11.
高温超导体YBaCuO光掺杂效应的正电子寿命谱研究   总被引:6,自引:3,他引:3  
报道了YBaCuO高温超导体进行光掺杂的基本情况,提供了正电子寿命与光掺杂量之间的变化关系,讨论了光掺杂机理,并将实验结果与理论模型进行了对比.  相似文献   

12.
Large-scale applications of high-transition-temperature (high-T(c)) superconductors, such as their use in superconducting cables, are impeded by the fact that polycrystalline materials (the only practical option) support significantly lower current densities than single crystals. The superconducting critical current density (J(c)) across a grain boundary drops exponentially if the misorientation angle exceeds 2 degrees -7 degrees. Grain texturing reduces the average misorientation angle, but problems persist. Adding impurities (such as Ca in YBa2Cu3O7-delta; YBCO) leads to increased J(c) (refs 9, 10), which is generally attributed to excess holes introduced by Ca2+ substituting for Y3+ (ref. 11). However, a comprehensive physical model for the role of grain boundaries and Ca doping has remained elusive. Here we report calculations, imaging and spectroscopy at the atomic scale that demonstrate that in poly-crystalline YBCO, highly strained grain-boundary regions contain excess O vacancies, which reduce the local hole concentration. The Ca impurities indeed substitute for Y, but in grain-boundary regions under compression and tension they also replace Ba and Cu, relieving strain and suppressing O-vacancy formation. Our results demonstrate that the ionic radii are more important than their electronic valences for enhancing J(c).  相似文献   

13.
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   

14.
用固相反应法制备123相YBa2-xSrxCu3O7-δ(YBCO)和掺Sr的YBa2-xSrxCu3O7-δ系列超导样品.利用四端引线电阻法测量样品的电阻温度曲线,得到Sr元素替代Ba位时超导转变温度Tc降低且Tc随掺杂量单调变化,从实验上验证了CuO2面的耦合可能是维持高温超导电性的一个重要条件.  相似文献   

15.
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   

16.
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   

17.
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   

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