共查询到20条相似文献,搜索用时 140 毫秒
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报道了YBa_(2-x)Pr_xCu_3O_(7-δ)(0≤x≤0.15)体系的超导电性和正常态输运性质的测量。实验结果表明随着Pr在Ba晶位替代量的增加,超导转变临界温度T_c和由Hall系数推算的荷电载流子浓度P_H均单调下降。通过与Y_(2-x)Pr_xBa_2Cu_3O_(7-δ)和Nd_(1+x)Ba_(2-x)Cu_3O_(7-δ)体系的比较研究,作者发现上述三个体系的T_c变化均与载流子浓度的变化相关联。作者进而提出,在YBa_(2-x)Pr_xCu_3O_(7-δ)体系中Pr的空穴填充效应
关键词: 相似文献
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利用正电子湮没实验,结合x射线衍射(XRD)结构分析,研究了具有混合稀土特征的(Y1 -xGdx)Ba2Cu3O7-δ系列样品. XRD 实验结果表明,半径较大的Gd离子Y位替代使得样品晶胞参数和晶胞体积增大,但所有样品 仍保持与YBa2Cu3O7-δ(YBCO)样品相同的单相正交结 构. 正电子湮没实验表明,正电子各寿命参数表现出很强的Gd替代依赖关系. 从正电子实验 结果出发,计算了Cu-O链区局域电子密度ne的变化. 结果表明,局域电子密度n e随Gd含量x的增加而减小,而超导转变温度Tc随局域电子密度ne的减小而增加,这种局域电子密度ne与超导电性的关联是与铜位替代 完全不同的,且可能是近年来人们关于混合稀土铜氧化物体系具有较高临界电流密度的原因 之一. 该研究结果为铜氧化物超导体的应用和机理研究提供了相应的正电子实验资料.
关键词:
超导电性
正电子湮没
相结构
局域电子密度 相似文献
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采用固相反应法制备La5/8(PrxCa1-x)3/8MnO3(x=0.25,0.5,0.75)多晶样品,研究其磁性质和电磁输运特性.X射线衍射表明,La5/8(PrxCa1-x)3/8MnO3(x=0.25,0.5,0.75)多晶样品室温的晶体结构呈Pnma空间群的正交结构.磁化强度-电阻(M~T)关系显示,La5/8(PrxCa1-x)3/8MnO3(x=0.25,0.5,0.75)的居里温度TC随Pr掺杂量增加而逐渐降低,三种样品分别为160K、150K、100K.此外,随着Pr3+掺杂量增加,样品晶格畸变程度增大,铁磁相互作用减弱,并且三种成分均形成自旋玻璃态,其自旋冻结温度分别为150K、75K、70K.电阻-温度(ρ~T)关系表明,样品在x=0.25时出现电阻的双峰现象,这是由于样品中铁磁相与反铁磁相相互竞争造成的.结果表明,通过对钙钛矿锰氧化物的A位稀土掺杂,可对其CMR效应进行有效调控. 相似文献
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Powder samples of YBa2Cu3O6 were magnetically aligned and the anisotropies in the systems were studied by means of Cu(1) nuclear quadrupole resonance (NQR) in the absence of external magnetic fields. Our room temperature measurements of the NQR lineshapes and the spin–lattice and spin–spin relaxation times as a function of the aligning magnetic field indicate that full microscopic alignment can be achieved by using a magnetic field of about 4.7 T, for which doublet line patterns arising from a hyperfine splitting were observed. 相似文献
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W. Prettl H. Lengfellner J. P. Kaminski Gi. Schneider P. G. Huggard T. O'Brien W. Blau 《International Journal of Infrared and Millimeter Waves》1992,13(10):1659-1666
The far infrared response of granular thin-film Bi2Sr2CaCu2O8 superconductor has been investigated using long (5 s) but sharply truncated free electron laser pulses in the frequency range between 50 cm–1 and 125 cm–1. Under constant current bias, a fast response and a slow bolometric signal component could be identified in this energy range, which is below the BCS energy gap ( 200 cm–1). Measurements of the power dependences of the signal voltages showed that both the fast and the thermal responses are consistent with the predictions of the resistively shunted Josephson junction model. 相似文献
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M. Hagiwara T. Shima R. Kitada H. Deguchi K. Koyama 《Physica C: Superconductivity and its Applications》2010,470(20):1052-1055
Intergrain ordering phenomena of frustrated ceramic YBa2Cu4O8 (Y124) and dual phase mixed ceramic containing CuO are studied by both magnetic and resistivity observations. Magnetically estimated intergrain ordering temperature Tc2 and zero-resistivity attainment temperature Tz are both decreased with CuO content. However, it is also revealed that mutual location of Tc2 and Tz is changed. For the mixed ceramic with torn intergrain network structure, Tz stays above Tc2, indicating local dissolution of frustration by cluster structure. On the other side, remaining resistivity tails blow Tc2, indicating intrinsic fluctuation effect on the resistivity caused by frustration in the ordered state. It is known then that, superconductive ceramic samples which is free from structural phase inhomogeneity is essential in order to clarify the frustration effect. 相似文献
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Shojiro Kimura Hitoshi Ohta Mitsuhiro Motokawa Seitaro Mitsudo Wen-Jye Jang Masahi Hasegawa Humihiko Takei 《International Journal of Infrared and Millimeter Waves》1996,17(5):833-841
Submillimeter wave ESR system in Kobe University is presented. It covers the frequency region from 60 to 383GHz and can apply the pulsed magnetic field up to 30T. The measurement of Y2Cu2O5 single crystals using our system is presented. 相似文献
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通过在碱液中共沉淀Mn2+、Ni2+和Fe2+后制备了棒状的前躯体,前躯体于不同温度煅烧后制得了MnxNi0:5-xZn0:5Fe2O4棒状体. 利用X射线衍射仪和透射电镜对棒状体的物相、形貌及粒径进行了表征,并利用振动样品磁强计对磁性能进行研究. 结果表明长径比大于15的棒状,随着x值的增加,MnxNi0:5-xZn0:5Fe2O4样品的直径增加,长度下降,长径比变小,当x=0.5时其直径在50 nm左右而长径比减小到7~8. 随着x值的增加,样品的矫顽力先增加后减少,x值达到0.4时样品的矫顽力再次增加,当煅烧温度为600 oC,x=0.5时样品的矫顽力最大为134.3 Oe. 饱和磁化强度随着x值的增加先增加后减少,当煅烧温度为800 oC和x=0.2时达到最大为68.5 Oe. 相似文献
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使用牛津震动样品磁强计(VSM)研究了Bi2Sr2CaCu2O8单晶的磁滞回线.在20到40K温度之间发现了反常的尖锋效应,随样品O含量的增加,发生尖锋效应的外场也相应提高.可以认为在尖峰效应处发生了由涡漩物质的有序固态到无序固态的相变,在有少量点缺陷存在的BSCCO单晶相图上,Bsp线终止于20K温度处,在20K以下温区没有发生准格子到涡漩玻璃的相变,涡漩固相始终以准格子形式存在;可以认为尖峰效
关键词:
2Sr2CaCu2O8单晶')" href="#">Bi2Sr2CaCu2O8单晶
磁滞回线
尖锋效应
相变 相似文献
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G.N. Darriba L.A. Errico E.L Muoz D. Richard P.D. Eversheim M. Rentería 《Physica B: Condensed Matter》2009,404(18):2739-2741
We report perturbed-angular-correlation (PAC) experiments on 181Hf(→181Ta)-implanted corundum Cr2O3 powder samples in order to determine the magnitude and symmetry of the electric-field gradient (EFG) tensor at Ta donor impurity sites of this semiconductor. These results are analyzed in the framework of ab initio full-potential augmented-plane wave plus local orbitals (FP−APW+lo) calculations. The results are also compared with EFG results coming from PAC experiments in isomorphous α-Al2O3 and α-Fe2O3 doped with 111In→111Cd and 181Hf→181Ta tracers. This combined analysis enables us to quantify the magnitude of the lattice relaxations induced by the presence of the impurity and to determine the charge state of the impurity donor level introduced by Ta in the band gap of the semiconductor. 相似文献
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M. N. Kotov V. F. Masterov V. V. Potapov A. V. Prichodko O. V. Smertin N. M. Shybanova 《International Journal of Infrared and Millimeter Waves》1993,14(8):1679-1687
Experimental investigations of superconductivity effects in single-phase and multiphase Bi2Sr2CaCu2O8 single-crystals have been carried out at 142 GHz frequency by means of the standing wave profile method [1]. Josephson harmonic generation has been observed to be responsible for the appearence of additional peaks on the standing wave profile of the open dielectric resonator loaded with a properly orientated multiphase high-Tc superconductor specimen. This leads to the conclusion that most of the Josephson junctions in multiphase crystals are located in certain crystallographic planes. The investigations of temperature dependencies showed that sharp resonant peaks of conductivity observed earlier [2] at 60 GHz could also be observed at 142 GHz. 相似文献