共查询到19条相似文献,搜索用时 109 毫秒
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利用倾斜衬底沉积法在无织构的金属衬底上生长了MgO双轴织构的模板层,在这一模板层上实现了YBa2Cu3O7-x薄膜的外延生长.在外延YBa2Cu3O7-x薄膜前,依次沉积了钇稳定的立方氧化锆和CeO2作为缓冲层.利用X射线衍射2θ扫描、φ扫描、Ω扫描和极图分析测定了这些膜的结构和双轴织构取向,利用Raman光谱表征了其超导相的品质和取向特性,利用扫描电镜和原子力显微镜观测了薄膜的表面形貌和粗糙度.考察了不同厚度的CeO2层对YBa2Cu3O7-x生长和性质的影响.发现了YBa2Cu3O7-x薄膜的外延生长和性能对CeO2的不同厚度具有显著而独特依赖性.讨论了其可能的机理. 相似文献
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YBa2Cu3O7-δ/LaAlO3 (YBCO/LAO) 超导薄膜是通过热蒸发沉积方法制备的,实验中使用的Tl2Ba2CaCu2O8/LaAlO3 (TBCCO/LAO) 超导薄膜是通过直流磁控溅射方法制备的.通过分析两片超导薄膜的XRD谱计算出了两片超导薄膜内的应变,ΔCY=4.8483×10-3;ΔCT=8.5272×10-5,结果显示YBCO超导薄膜内的应变要大于TBCCO超导薄膜内的应变.另外,采用共面谐振技术研究这两片超导薄膜内的微波表面电阻随温度的变化,结果表明YBCO超导薄膜具有更大的微波表面电阻.分析和讨论了应变对超导薄膜微波表面电阻的影响. 相似文献
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超导体/半导体结(Superconductor/semiconductor p-n junction)在制备场效应管,晶体管方面具有巨大的潜力.本文通过脉冲激光沉积的方法,使用Nb掺杂的(100)方向SrTiO3作为薄膜衬底,沉积了厚度约为350nm c轴取向的YBa2Cu3O7-δ薄膜,从而得到YBa2Cu3O7-δ/Nb:SrTiO3双层结.R~T曲线,以及XRD曲线显示YBa2Cu3O7-δ薄膜具有良好的超导电性和晶体结构,在零磁场不同温度下测量得电流-电压曲线显示YBa2Cu3O7-δ/Nb:SrTiO3构成的超导体/半导体双层结在小于YBa2Cu3O7-δ临界转变温度Tc时具有p-n结整流特性,当大于YBa2Cu3O7-δ超导转变温度时,呈现出非典型肖特基结的特性. 相似文献
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研究了高温氧化物超导体Y0.5Gd0.5Ba2Cu3O7-δ体系中通氧时间对超导转变温度及超导转变温区的影响。Y0.5Gd0.5Ba2Cu3O7-δ样品是按相等摩尔数的Gd与Y元素配比,采用传统的固相反应法烧结而成的多晶块材。实验结果显示:Y0.5Gd0.5Ba2Cu3O7-δ烧结样品与YBa2Cu3O7-δ烧结样品均具有很好的单相性,在一定的通氧条件下其超导临界转变温度TC与超导初始转变温度TCO值相对YBa2Cu3O7-δ烧结样品有提高。文中对此结果进行了讨论。 相似文献
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利用脉冲激光沉积(PLD)方法制备了c轴取向的高质量YBa2(Cu1-xZn)3O7-δ(x=0, 0.01, 0.02)外延薄膜.超导临界温度随Zn掺杂量增加而较快地下降,与单晶样品的结果相符.在强磁场下的输运测量发现YBa2(Cu1-xZn)3O7-δ系列样品在Tc附近均出现反常的Hall电阻率符号反向,但其Hall电导率σxy随磁场的变化关系与氧欠掺杂的YBa2Cu3O6.66存在很大差异,说明Zn掺杂和氧掺杂对混合态中的磁通涡旋性质的影响有显著不同. 相似文献
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This paper systematically investigates the intermediate phases of YBa2Cu3O7-x (YBCO) film prepared by metalorganic deposition method using trifluoroacetates (TFA-MOD). According to x-ray diffraction and Raman analyses, the precursor film decomposed in a mixture of BaF2, Y2O3 and CuO after the pyrolysis process. Then these intermediate phases converted into tetragonal YBa2Cu3O6.5 at about 725°C. The influence of water vapour pressure on the YBa2Cu3O7-x film growth on LaAlO3 single-crystal substrates was also studied. The films prepared at low water vapour pressures (40-140 hPa) showed poor electrical performance due to the a-axis grain structure and impurity phases. However, the films prepared at 190 hPa exhibited the highest critical temperature of 90 K and the highest Jc of 3.8 MA/cm2, which was attributed to the formation of a purer YBCO phase and stronger biaxial texture. 相似文献
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本文首先综述了大规模应用的超导磁体,依赖并推动铌三锡Nb3Sn导线技术进步,向更强磁场发展的趋势.着重分析了超高场14 T全身MRI磁体的挑战性技术.选择青铜Nb3Sn导线,采用Nb3Sn线圈和NbTi线圈相结合的混合结构,对14 T全身MRI磁体进行了电磁概念设计和热稳定性及失超保护仿真分析,并简要阐述了14 T全身MRI磁体在应力、接头和匀场方面的关键问题.根据分析结果认为:1)Nb3Sn导线是14 T全身MRI磁体需要面临的首要挑战性问题—作为最佳选择的青铜Nb3Sn导线,其现有产品的性能指标离14 T全身MRI磁体的要求尚存在有一定的差距;2)14 T全身MRI磁体的失超保护涉及线圈的铜超比设计、运行电流同线圈电感的协调配置、被动保护的分段策略和主动保护的失超触发控制以及主动屏蔽结构磁体在失超过程中的逸散磁场限制等多个十分复杂的环节,是最具挑战性的综合性技术. 相似文献
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Y. Endoh R. J. Birgeneau M. A. Kastner G. Shirane K. Yamada 《Physica B: Condensed Matter》2000,280(1-4):201-204
The discovery of the spin density wave (SDW) state defined as stripe in the doped Cu oxides becomes a central issue in the elucidation of the high-temperature superconducting mechanism. We present the coexistence of the stripe order and superconductivity, and the change of the stripe structure associated with the insultor–metal transition. Both static and dynamical SDW are robust of the high-temperature superconducting Cu oxides. 相似文献
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采用传统方法生产的NbTi/Cu多芯超导线在生产芯数较多的超导线时存在填充系数较大的问题,这直接影响了芯丝的整齐排布,所以组装完成后加入热等静压过程.研究了经过热等静压和未经过热等静压的NbTi/Cu多芯超导线的加工性能.经过试验证明,经过100~150MP,2小时热等静压处理的NbTi/Cu多芯超导线坯锭在加工过程中具有良好的加工性能,提高了超导线复合坯锭的成品率;而未经过热等静压处理的NbTi/Cu多芯超导线坯锭加工性能较差,坯锭内部缺陷较多. 相似文献
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《Physics letters. A》1987,123(1):34-36
The superconducting transition temperatures of a family of YBaCu oxides have been explored by dc resistivity measurements. Substitutions of magnetic and non-magnetic ions on Y, Ba and Cu sites are reported. For some compositions, achieving high superconducting transition temperatures is strongly dependent on growth conditions for the material. 相似文献
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Sasaki S Kriener M Segawa K Yada K Tanaka Y Sato M Ando Y 《Physical review letters》2011,107(21):217001
A topological superconductor (TSC) is characterized by the topologically protected gapless surface state that is essentially an Andreev bound state consisting of Majorana fermions. While a TSC has not yet been discovered, the doped topological insulator Cu(x)Bi(2)Se(3), which superconducts below ~3 K, has been predicted to possess a topological superconducting state. We report that the point-contact spectra on the cleaved surface of superconducting Cu(x)Bi(2)Se(3) present a zero-bias conductance peak (ZBCP) which signifies unconventional superconductivity. Theoretical considerations of all possible superconducting states help us conclude that this ZBCP is due to Majorana fermions and gives evidence for a topological superconductivity in Cu(x)Bi(2)Se(3). In addition, we found an unusual pseudogap that develops below ~20 K and coexists with the topological superconducting state. 相似文献
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V. P. Korzhov M. I. Karpov V. I. Vnukov 《Bulletin of the Russian Academy of Sciences: Physics》2012,76(1):27-36
A multilayer layer from the superconducting compound Nb3Sn was obtained by the thermal treatment of composite (Cu/Nb)/Cu12Sn conductor consisting of Cu-12% Sn and Cu/Nb interlayers
consisting in turn of nanosized copper and niobium layers. The conductor was coated with copper from the outside, which served
as a stabilizer. The microstructure of the cross section of the composite band in dependence on the volume ratio of Cu/Nb
and bronze interlayers and the microstructure of the Cu/Nb interlayers themselves in dependence on the annealing temperature
were investigated. The optimum ratio of composite components was as follows: t
Nb
N
Nb ≈ 0.288t
CuSn
N
CuSn, where t and N are the thickness and number of the niobium and bronze layers, respectively. Trying to maintain the optimum design of the
conductor forced us to increase the bronze volume content relative to the content of Cu/Nb interlayers, which had a negative
impact on the composite microstructure. This resulted in disruptions of Cu/Nb interlayers. A technique has been developed
for producing the (Cu/Nb)/Cu12Sn composite as a precursor to the band from the Nb3Sn compound with allowance for the first experiment’s shortcomings. 相似文献
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M. Salluzzo F. Natali C. Aruta M.G. Maglione F. Ricci E. Koller Ø. Fischer N.L. Saini 《The European Physical Journal B - Condensed Matter and Complex Systems》2002,27(4):467-472
We report results of a time resolved X-ray Absorption Spectroscopy (XAS) experiment on the oxidation process of epitaxial
Y1(Nd0.05Ba1.95)Cu3Ox superconducting thin films. For the first time Cu K-edge XAS technique has been used to explore local structural changes
around the Cu ions during the oxidation process of a high critical temperature superconducting film. The results show that
during the oxygenation of a tetragonal Y1(Nd0.05Ba1.95)Cu3Ox additional local transitions appear in the orthorhombic I phase, which are not linked to long range order transformations
as shown by in situ X-ray diffraction experiment. New questions concerning the dynamic microscopic process leading to the oxygenation and eventually
to superconductivity of the complex R1+xBa2-xCu3Ox (R = Y or rare earth) compounds arose from these results.
Received 21 December 2001 Published online 25 June 2002 相似文献
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P. V. Leksin A. A. Kamashev N. N. Garif’yanov A. A. Validov Ya. V. Fominov J. Schumann V. E. Kataev B. Büchner I. A. Garifullin 《Physics of the Solid State》2016,58(11):2165-2176
An important role of the morphology of a superconducting layer in the superconducting spin-valve effect has been established. The triplet pairing induced by the superconductor/ferromagnet proximity effect has been experimentally investigated for samples CoOx/Py1/Cu/Py2/Cu/Pb (where Py = Ni0.81Fe0.19) with a smooth superconducting layer. The optimization of the parameters of this structure has demonstrated a complete switching between the normal and superconducting states with a change in the relative orientation of magnetizations of the ferromagnetic layers from the antiparallel to orthogonal orientation. A pure triplet contribution has been observed for the sample with a permalloy layer thickness at which the superconducting spin-valve effect vanishes. A direct comparison of the experimental data with the theoretical calculation of the temperature of the transition to the superconducting state has been performed for the first time. 相似文献