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测量了 YBa_2Cu_3O_(7-x),Tl_2Ba_2Ca_2Cu_3O_(10)和 Bi_(1.5) Pb_(0.5),Ca_2Sr-2Cu_3Oy 等氧化物超导体的热电势率与温度的关系,发现在超导转变前,都有一明显的峰.在温度较高时,热电势率与温度的关系可用 S=AT+B/T 表示,因而,在这些高温超导体中声子曳引热电势不能忽略,存在电-声子相互作用,我们还由热电势数据估计了上述三种氧化物超导体的费米能,它们分别为1.05eV、2.98eV 和3.24eV. 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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测量了零电阻温度为114K 的 TlBaCaCuO 超导体的热电势率,结果表明,在150K 以上热电势率与温度的关系可用 S=AT+B/T 表示,说明在这类高温超导体中声子曳引热电势即使在高温区也不能忽略,存在电-声子相互作用. 相似文献
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对高品质单相多晶Bi2Sr2CaCu2O8+δ样品作真空或H2气氛中不同温度下的热处理。由X射线结构分析,其正常态和超导态性质(特别是载流子浓度)的系统测量结果表明:Bi2Sr2CaCu208+δ样品在H2气氛中热处理,其氧的释放可分为两个阶段:一是Bi-O层之间的过量氧原子的逸出,降低系统的载流子浓度,从而调节Tc;二是CuO2面内氧原子的迁移,产生氧空位,使CuO2面内Cu2+的短程二维反铁磁(2D-AFM)有序背景遭到破坏。可以认为:以往文献中报道的Bi2Sr2CaCu2O8+δ超导体的吸氢效应导致Tc的变化,很可能主要的并不是氢原子的电子掺杂行为,而是与吸氢过程中氧含量的变化相联系。
关键词: 相似文献
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测量了MgB2的热电势和电阻率与温度的依赖关系.在100K—300K区间,热电势呈近似线性温度依赖关系,其斜率为正,表明载流子为空穴型且与能带贡献的图像相一致.与此对应,在此温区电阻率呈T2依赖关系.在100K以下,热电势和电阻率各自转变了其高温区的温度依赖关系.热电势在超导转变温度Tc(零电阻366K)到100K间有一宽峰,具有声子曳引峰的特征,表明电子-声子相互作用很强.估算了一些重要的参数,如带米能EF、能带宽度
关键词:
新型超导体
热电势
电阻率 相似文献
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本文研究了Bi-Sr-Ca-Cu-O体系中理想成份为Bi2Sr2CaCu2O8化合物的超导性能和晶体结构。名义成份为BiSrCaCu2O5.5零电阻超导转变温度Tc(0)=81.5K。用X射线粉末衍射方法测定了Bi2Sr2CaCu2O8的晶体结构,其基本结构属体心四方晶系,空间群为D4h17-l4/mmm,点阵常数a=3.825?,c=30.82?。每单胞化合式单位为2.2Ca占据2(a)等效点系,4Sr,4Bi和4Cu占据三组4(e)位置,其原子参数z分别为0.110,0.302和0.445,16O分别占据8(g),z=0.445和二组4(e),z=0.210和0.380。Bi2Sr2CaCu2O8晶体结构可认为是阳离子沿z轴的(00z)和((1/2)(1/2)z)交错排列,由Aurivillius相导生出来的。讨论了在Bi-Sr-Ca-Cu-O体系中可能存在的其它沿z轴不同堆垛层数的超导相。
关键词: 相似文献
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实验研究了Bi2Sr2CaCu2-xSnxO8+δ 的X射线衍射(XRD)和光电子能谱(XPS).实验发现随着掺杂(Sn)量的增加,晶格参数a 和c都有所变化,O1s和Cu2p芯能级谱也发生了变化.实验结果表明: 在低掺杂量时,Sn主要 呈二价态;而在高掺杂浓度时呈四价态;掺Sn对超导电性的影响与其他元素的掺杂不同.这 些实验结果支持化学环境在高温超导样品的电子结构中起着重要作用的结论.
关键词:
Bi系超导体
掺杂
X射线衍射
光电子能谱 相似文献
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X.F. Hu 《Surface science》2006,600(11):2252-2257
Temperature dependent infrared study of water adsorption on the bc-plane of a Bi2Sr2CaCu2O8 (Bi2212) single crystal reveals that water is molecularly physisorbed, and forms hydrogen-bonded clusters in the temperature range of 85-150 K. Although dissociative adsorption is expected on surfaces terminated with Ca-O and Cu-O groups, no dissociated species is detected. The main absorption bands occur between 3200 and 3500 cm−1 and are assigned to the O-H stretching and the overtone of O-H bending. For exposures higher than 1.0 L, the sticking coefficients are similar for different temperatures. The features in the O-H stretch region for water clusters red-shift as a function of temperature between 85 and 140 K. Water clusters have an amorphous structure between 85 and 140 K, and form a crystalline structure at 150 K. 相似文献
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A. Balzarotti M. Fanfoni F. Patella R. Sperduti F. Licci 《Physica C: Superconductivity and its Applications》1995,250(3-4):382-388
We have applied the phenomenological model of diffused interfaces, developed originally to describe the Fe growth on Bi2Sr2CaCu2O8, to interpret quantitatively the core photoemission spectra of two reactive interfaces, namely Cr and Ge on Bi2Sr2CaCu2O8. At room temperature the interfaces with Fe and Cr have the same kinetics of growth suggesting similar adatom condensation, while the semiconductor-superconductor interface grows layer-by-layer according to the Franck-van der Merwe kinetics. Differences in the parameters of the model resulting from the simultaneous fit of the core-level decays are related to differences in the microscopic processes occurring during the growth. 相似文献
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August Yurgens Dag Winkler Nicolay Zavaritsky Tord Claeson 《Czechoslovak Journal of Physics》1996,46(Z3):1293-1294
We report on thec-axis superconducting energy gap parameter Δ
c
(T) of intrinsic Josephson tunnel junctions inBi
2
Sr
2
CaCu
2
O
8+δ (Bi2212) single crystals. Δ
c
(4.2K)≈10−13 meV, which is approximately a factor of two smaller than reported in the majority of tunneling experiments. Δ
c
(T) deviates strongly from the BCS temperature dependence. These observations may be explained by a multilayer model of Bi2212
which assumes that theBi−O layers are superconducting due to the proximity effects. The Josephson tunneling then takes place between adjacentBi−O layers while there is a strong proximity coupling betweenBi−O andCu−O layers.
The work is supported by Swedish Supercon-ductivity Consortium and NUTEK, and, in part, by Russian Foundation for Basic Research,
grant #95-02-04307 相似文献