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1.
用脉冲激光沉积法在先在MgO衬底上制备一层Sr2(AlTa)O6薄膜作为过渡层,再制备(Y0.6Ho0.4)Ba2Cu3O7-δ超导薄膜,新超导薄膜的零电阻温度Tc0为89K,临界电流密度Jc为2.3*10^6A/cm^2(77K),用X射线衍射仪及扫描电子显微镜分析了薄膜特性。  相似文献   

2.
用反射式高能电子衍射(RHEED) 和原子力显微镜(AFM) 研究激光分子束制备的铁电BaTiO3 和高Tc 超导c 取向Y1Ba2Cu3O7 薄膜的生长模式,BTO 铁电薄膜是原子级平整的层状生长模式;c 取向YBCO 超导薄膜是SK生长模式 当薄膜厚度小于5 个原胞时,层状生长,然后是台阶岛状生长.处理SrTiO3 基片表面可以改变c 取向YBCO薄膜的生长模式  相似文献   

3.
激光沉积法制备(Y1—xHox)Ba2Cu3O7—δ薄膜   总被引:1,自引:1,他引:0  
本文报道了用激光沉积法在(100)LaAlO3衬底上制备(Y1-xHox)Ba2Cu3O7-δ(x=0,0.2,0.4)超导薄膜.结果表明,新超导薄膜表面光滑,具有很强的c轴织构,零电阻温度Tc0约91K,最佳临界电流密度Jc为4.7×106A/cm2(77K).  相似文献   

4.
苏杰  李元 《低温物理学报》1998,20(3):161-164
本文利用脉冲激光沉积的定向性和掩模的阴影效应,原位沉积N-YBCO作为势垒层制备了高TcYBa2Cu3O7Josephson边缘结,在60K,微波辐照观察到明显的Shapiro台阶,在Tc附近,Ic∽(1-T/Tc),n=1.88。  相似文献   

5.
本研究了利用YSZ(Y稳定的ZrO2)缓冲层在Si衬底上单靶偏轴溅射Bi-Sr-Ca-Cu-O高温超导薄膜的工艺条件,给出了YSZ和BSCCO薄膜的性能测试结果,并根据电镜分析结果,提出了BSCCO薄膜的螺旋柱状生长机理。  相似文献   

6.
MOCVD法在金属基体上制备YBCO超导带   总被引:2,自引:0,他引:2  
本报道了用MOCVD静态和动态沉积两种工艺制备YBCO超导带的实验结果。以Y(TMHD)3、Ba(TMHD)2和Cu(TMHD)2为挥发源,O2气为反应剂,高纯Ar气为载流气体,在静止和以10-15cm/h带速移动的金属银基体上,制出了有强烈c-轴取向的YBCO超导带。静态沉积样品的Jc达到1.04×10^4A/cm^2,动态沉积样品的Jc达到1.4×10^4A/cm^2(78K,0T)。对改…  相似文献   

7.
采用磁控溅射方法在(100)YSZ基底上沉积了YBa2Cu3O7/SrTiO3/YBa2Cu3O7异质外延三层膜。利用交流磁化率和四引线电阻测量的方法确定了三层膜的超导性能,利用X射线衍射和透射电子显微镜研究了三层膜的结构特征。研究结果表明,膜层的结晶质量较好,临界转变温度Tc在83.5K和86.7K之间。YBCO膜层中的绝大多数甚至全部)晶粒为c取向,在有些膜中只存在少量的a或b取向的YBCO晶  相似文献   

8.
采用磁控溅射方法在(100)YSZ基底上沉积了YBa2Cu3O7/SrTiO3/YBa2Cu3O7异质外延三层膜,利用交流磁化率和四引线电阻测量的方法确定了三层膜的超导性能,利用X射线衍射和透射电子显微镜研究了三层膜的结构特征.研究结果表明,膜层的结晶质量较好,临界转变温度Tc在83.K和86.7K之间.YBCO膜层中的绝大多数甚至全部)晶粒为C取向,在有些膜中只存在少量的a或b取向的YBCO晶粒.三层膜中层界面比较清晰但不十分平整.在膜/基界面处有8-10nm厚的过渡层,它由多晶的BaZrO3组成.膜层和(10)YSZ基底之间具有如下的外延生长关系YSZ[001]//YBCO[110]//SrTjO3[110];YSZ(100)//YBCO(001)//SrTiO3(001).  相似文献   

9.
用MOCVD法在YSZ衬底上制备YBCO膜   总被引:1,自引:0,他引:1  
用低压MOCVD多源法在单晶YSZ和具有双轴取向IBADYSZ的金属基带上沉积了YBCO膜,它们的Jc(77.3K,0T)分别为~2×106A/cm2和~7×104A/cm2.分析了本试验中的Jc差别原因.在单晶YSZ上YBCO高Jc数值显示了用MOCVD制备涂层膜导体的潜力  相似文献   

10.
应用脉冲激光沉积法和光刻技术我们成功地制作Ag/Pb(Zr0.53Ti0.47)O3/YBa2Cu3O7-x(PZT/YBCO)三端器件.为了降低矫顽场,应用变形相界(x≈0.53)的550纳米厚的PZT作为门电极,通过优化沉积条件和门电极面积小型化(6×10-6cm2),在64K下三端器件门电极显示了极好的电性能,低的矫顽场(~37kV/cm)、大的饱和极化强度(60μC/cm2)、剩余极化强度(41μC/cm2)以及击穿电压~3×105V/cm.对于我们的场效应器件,在±9V的情况下沟道电阻被调制~3%.  相似文献   

11.
We have investigated defects and in-plate orientations of YBa2Cu3Ox thin films prepared by pulsed laser deposition (PLD) with YSZ as a buffer layer. The films showed c-axis oriented growth with the transition temperature Tco up to 87 K. Several types of defects including thermally induced cracks, grain boundaries and outgrowths were observed by scanning electron microscopy (SEM) and high resolution transmission electron microscopy (HRTEM). The grain boundary provided a favorable path for crack propagation. The outgrowths nucleated on the YSZ surface grew with stoichiometric composition. According to X-ray diffraction (XRD) and HRTEM studies the YSZ buffer layer grew with the orientation relationship, YSZ110//Si110 and YSZ(001)//Si(001) up to the YBCO/YSZ interface. The superconducting YBCO films on top grew mainly with YBCO100//Si110 and YBCO(001)//Si(001), with some minor portions of YBCO110//Si110 and YBCO(001)//Si(001).  相似文献   

12.
Epitaxial thin films of YBa2Cu3O7 (YBCO) have been deposited on Y–ZrO2 (YSZ) substrates by means of the pulse laser deposition technique. It has been found that the initial epitaxy of YBCO thin films grown on YSZ can be significantly improved by using La1.85Sr0.15CuO4 (LSCO) as a buffer layer. X-ray diffraction measurements show that the epitaxial YBCO films have single in-plane orientation with YBCO [100]LSCO [100] and LSCO [100]YSZ [110]. The real-time resistance measurements reveal that with LSCO buffer layers the initial formation of the YBCO ultra-thin films changes from the island growth to the layer-by-layer growth.  相似文献   

13.
CeO2/YSZ/CeO2 buffer layers were deposited on biaxially textured Ni substrates by pulsed laser deposition. The influence of the processing parameters on the texture development of the seed layer CeO2 was investigated. Epitaxial films of YBCO were then grown in situ on the CeO2/YSZ (yttria-stabilized ZrO2)/CeO2-buffered Ni substrates. The resulting YBCO conductors exhibited self-fleld critical current density Jc of more than 1 MA/cm^2 at 77K and superconducting transition temperature Tc of about 91K.  相似文献   

14.
YBa2Cu3O7−δ (YBCO) films with high critical current density (Jc) were successfully fabricated on nickel tapes buffered with epitaxial NiO. NiO was prepared on the textured nickel tape by the surface-oxidation epitaxy (SOE) method. We have reported so far a critical temperature (Tc) of 87 K and Jc=4–6×104 A/cm2 (77 K, 0 T) for the YBCO films on NiO/Ni tapes. To enhance the superconducting properties of the YBCO films on the SOE-grown NiO, depositions of thin oxide cap layers such as YSZ, CeO2, and MgO on NiO were investigated. These oxide cap layers were epitaxially grown on NiO and provided the template for the epitaxial growth of YBCO films. Substantially improved data of Tc=88 K and Jc=3×105 A/cm2 (77 K, 0 T) and 1×104 A/cm2 (77 K, Hc, 4 T) were obtained for YBCO film on NiO, by using a MgO cap layer with a thickness of 50 nm. The method described in this paper is a simple way to produce long YBCO tape conductors with high-Jc values.  相似文献   

15.
我们研究了T1-2212超导薄膜在带有YSZ/CeO2缓冲层和带有Ce02/YSZ/CeO2缓冲层的Ni金属RABiTS基带上的生长情况.基带上的缓冲层是采用PLD方法制备的,T1-2212薄膜的制备采用了磁控溅射和后热处理两步方法.XRD实验结果表明。T1-2212薄膜都具有很好的C轴垂直于膜面的织构,并具有双向外延生长特性.在CeO2/YSZ/CeO2/Ni基带上制作的T1-2212薄膜的Tc达到102.8K,J,(77K,0T)达到2.6MA/cm^2;在YSZ/CeO2/Ni基带上薄膜Tc可达97.7K,Jc(77K,0T)也可以达到0.45MA/cm^2.  相似文献   

16.
我们研究了Tl-2212超导薄膜在带有YSZ/CeO2缓冲层和带有CeO2/YSZ/CeO2缓冲层的Ni金属RABiTS基带上的生长情况.基带上的缓冲层是采用PLD方法制备的,Tl-2212薄膜的制备采用了磁控溅射和后热处理两步方法.XRD 实验结果表明,Tl-2212薄膜都具有很好的C轴垂直于膜面的织构,并具有双向外延生长特性.在CeO2/YSZ/CeO2/Ni基带上制作的Tl-2212薄膜的Tc达到102.8 K,Jc(77 K,0 T)达到2.6 MA/cm2;在YSZ/CeO2/Ni基带上薄膜Tc可达97.7 K,Jc(77 K,0 T)也可以达到0.45 MA/cm2.  相似文献   

17.
在钇钡铜氧(YBCO)高温超导涂层导体制备路线中,离子束辅助沉积技术(IBAD)是两大主流技术路线之一,取得了最为突出的研究成果.本文简要介绍了IBAD技术制备YBCO涂层导体的最新研究进展;并采用离子束辅助沉积技术在哈氏合金(Hastelloy)基底上成功制备了1米长具有钇稳定氧化锆(YSZ)缓冲层的金属基带.采用X射线衍射仪(XRD)分析YSZ缓冲层的取向;利用原子力显微镜(AFM)和扫描电镜(FESEM)观察其表面形貌.获得了可以实际应用的IBAD-YSZ/Hastelloy缓冲层长基带,可以在该基带上研制其他缓冲层以制备YBCO高温超导涂层导体带材.  相似文献   

18.
The a-axis oriented YBa2Cu3Ox(YBCO) thin films could be grown on (100) SrTiO3(STO) substrates with STO buffer layers by dc and rf magnetron sputtering either by low-ering the deposition temperature, or by using a self-template technique. For the latter, the resistivity of the thin film at 290K along the substrate [001] direction is about four times larger than that in the [010] direction. The zero resistance temperatures Tc0 are 89 K in both directions. So high quality a-axis oriented YBCO thin films can be prepared by the self-template technique. Also the Tc0 increase monotonously with the reduction of the thickness of the YBCO seed layer.  相似文献   

19.
YBa2Cu3O7-x(YBCO)膜存在“厚度效应”: 随着厚度增加, YBCO薄膜的临界电流密度下降, 尤其是YBCO薄膜的厚度超过1 μm时, 它的临界电流密度急剧下降. 本文在YBCO薄膜之间引入极薄的二氧化铈(CeO2)薄膜, 成功制备出结构为YBCO/YBCO/CeO2/YBCO的超导厚膜. 所制备的厚度为2 μm的YBCO膜临界电流密度为1.36 MA/cm2 (77 K, 自场), 其性能比相同厚度的纯YBCO膜有了较大幅度的提升. 研究表明CeO2薄膜起到了传递织构、松弛应力的作用.  相似文献   

20.
Superconducting thick films were grown on single crystals MgO and YSZ by electrophoretic deposition with Y_2BaCuO_5(Y211) addition. YBCO thick films were then accomplished by sintering the precursor films above the peritectic temperature. Single crystals of MgO (3×3×0.5 mm^3) were used as top-seed to control crystal structure of the thick films. As shown by scanning electron microscopy, the morphologies of YBCO/YSZ and YBCO/MgO thick films are spherulitic texture and platelet type. The critical temperature is ~89 K for the YBCO/YSZ thick film; the onset transition temperature is 86.4 K and the transition width is ~3 K for YBCO/MgO thick film. The critical current densities (as determined by Bean model) are, in A/cm^2, 3870 (77 K) for YBCO/YSZ thick films and 2399 (77 K) for YBCO/MgO thick films, which are comparable to the best J_c reported of the thick films prepared by the same method.  相似文献   

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