共查询到19条相似文献,搜索用时 296 毫秒
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研究了掺Ba对Bi2Sr2-xBaxCaCu2Oy(0≤x≤0.15,0.3)单晶和多晶样品超导电性的影响,结果表明,有少量Ba2+离子进入了超导相,且有固溶度极限.对于2212相单晶,c轴参数和Tc均随Ba含量增加而增加;对于慢冷多晶样品,掺Ba可明显提高Tc;然而对于淬大多晶样品,Tc没有明显变化,用掺Ba
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用第一原理的LDF-LMTO-ASA超元胞法,模拟由X射线吸收谱精细结构测定的BaBiO3中,Bi有两种价态Bi3+和Bi5+及与之相应的两种不同键长的Bi—O八面体,以及K掺杂对晶体结构的影响.计算了Ba4Bi4O12,(Ba3K)Bi4O12,(BaK)Bi2O6,(BaK3)Bi4O12,K2Bi2O6(简记为(404),(314),(112),(134),(022))五种“样本”的电子结构.结果表明,(404)和(314)分别为Eg=1.6eV及Eg=1.5eV的半导体,其它“样本”为金属.总能的分析表明(134)是不稳定的,故溶解极限为x=0.5.以“取样”方式按伯努利分布确定任意组分各“样本”的概率,进而计算了(Ba1-xKx)BiO3电子结构随组分的变化.最后用逾渗模型说明了超导转变温度Tc在x=0.25附近的突变
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本文中我们用X射线旋进照相观察了Bi2+xSr2-xCuOy的晶体调制结构.实验结果表明x=0.2的单晶样品具有单斜对称性,其空间群为B2/b(或Bb).随着x的增加,单斜畸变减小.我们测量了调制波矢随名义组成的变化规律,讨论了调制波矢在第一布里渊区的对称性质.对调制结构提出了几种可能的有公度模型.最后讨论了调制结构对超导电性的影响. 相似文献
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研究了Gd1-xCaxBa2Cu3O7-y(0.0≤X≤0.20)高温超导体在常压和高压下的超导电性在1-300K温度范围内,利用Bridgman对顶砧获得压力达9.0GPa,测量了(X=0.10,0.15,0.20)样品的dTc/dp分别为7.68,7.8和4.46K/GPa。发现Tc的压力导数随着ca2+含量的增加而下降,分析了氧含量对Tc和dTc/dP的影响.利用常压下晶格参数精修值和阳离子与氧离子间距随压力的改变,说明CuO2面在超导电性上的作用,用CuO2面之间耦合解释Tc(P)曲线的非线性关系。
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本通过X射线衍射、差热分析和超导电性测量等手段对Bi1.6Pb0.4Sr2Ca2-x(Nd0.75Ce0.25)xCu3Oy体系的相结构和超导电性进行了研究。该体系中,在810-840℃空气中烧结40小时样品的Tc随着x增加而降低。研究了在750-820℃空气中烧结40小时样品的超导转变温度为19-21K。这种超导电性可能是由于部分被稳定的Bi-2222相所致。 相似文献
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作者报道了用X射线衍射法对Bi2Sr2-yMyCuO6+δ(M=La,Pr,0.0≤y≤1.0)系列单晶样品进行结构研究的结果.根据晶体结构的不同性质,我们将掺杂区分为三个区域.第一个区域的掺闭量在0.0≤y≤0.10之间,在此区域中晶体的平均结构为单斜结构,其调制波矢具有两个非公度分量q1=β1b+γ1c.第二个掺杂区的掺镧量在0.10<y≤0.60之间,晶体的平均结构由单斜转变为正交结构,调制波矢具有单个非公度分量q1=β1b+c.第三掺杂区的掺镧量在0.60<y≤1.0之间,晶体的平均结构转变为另一单斜结构,在这一区域有两类调制结构共存.第一类调制结构与第一、第二掺杂区的调制结构类似;第二类调制结构的调制调幅沿α轴方向极化,调制波矢β分量约为第一类调制结构的二分之一.对于Bi2(Sr1.2La0.8)CuO6+δ单晶,其第二类调制波矢为q2=0.122b+0.43c. 相似文献
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《Journal of magnetism and magnetic materials》2003,262(3):508-513
In this paper, we report the observation of X-ray photoelectron spectra (XPS), which were obtained from high-Tc superconducting compounds Bi-2212 with some percentage of 3d elements (Fe, Co, and Ni) substituted for copper. The changes in characteristics of XPS spectra Sr 3d and Cu 2p3/2 with the doping content were explained in the relation to the hole concentration on CuO2 planes, which resulted in high-Tc superconductivity. 相似文献
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通过测量YBa2Cu3-xMxO7-y(M=Zn,Ni,x=0,0.025,0.05,0.075,0.1,0.15,0.2,0.3)系列样品的晶体结构、正常态电子输运性质、超导电性以及O含量,给出了Zn择优取代Cu(2)的更直接证据;同时,观察到掺Zn系统中的由正交相Ⅰ到正交相Ⅱ的结构相变以及Ni取代Cu带来的电子局域化效应。研究结果表明,具有正二价态的Zn对Cu(2)具有择优取代性,而具有正二价和正三价的Ni并不具有明显的择优取代。对Cu(2)的取代引起超导临界温度的显著变化,但对正常态电子输运性质的影响不明显;对Cu(1)的取代更显著地影响了晶体结构和正常态电子输运性质,同时对Tc产生抑制,我们认为,YBa2Cu307中的高温超导电性以及正常态输运性质是由CU-O平面和Cu-0链共同承担,而Cu-O平面和Cu-0链之间的耦合强度决定着该系统的超导电性的强弱。
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《Solid State Communications》1987,63(7):645-648
In relation to the high Tc recently observed in YBaCuO systems, the possibility of formation of Cooper pairs by virtual exciton exchange in a single phase is analysed. Electron-Exciton coupling matrix elements and possible optimum condition of superconducting Tc and its upper limit are evaluated. It shows that this kind of superconductivity may display some different features compared with usual BCS superconducting phase. 相似文献
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K. Kumagai Y. Nakamichi Y. Nakamura I. Watanabe H. Nakajima T. Fujita 《Hyperfine Interactions》1989,50(1-4):583-591
Nuclear quadrupole resonances (NQR) of139La in La2−xMxCuO4 (M=Ba, Sr) and63Cu in YBa2CU3O7 have been investigated with substitution of Cu by magnetic impurities. For La-system, the strong enhancement of the nuclear
relaxation rate, 1/T
1 atT
c
*≈10 K (suggesting the occurrence of magnetic instability with hole-doping), is suppressed by 3D-antiferromagnetism induced
by magnetic impurities. In the superconducting region, fluctuations of Cu moments at low temperatures remain extremely fast
as at high temperatures. For Y-system, Fe-ions are substituted for both Cu(1) and Cu(2) sites, But Co-ions are preferentially
substituted to Cu1 sites. The peaks in the relaxation rate of Cu indicate the appearance of magnetic ordering without destroying
superconductivity for the 0.5%-Fe doped sample. 相似文献
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V. F. Nesterenko 《高压研究》2013,33(5-6):767-772
Abstract The properties of high Tc-ceramics (Y-123, Bi-1112, Bi-4334, Bi-4457, (Bi-Pb)-4457) under shock loading and subsequent heat treatment were investigated. The peculiarities of their structure, tecture creation, changes of superconductivity parameters depending on loading conditions at P~ 10GPa Were revealed, and regimes of heat treatment were determined. The possibilities of obtaining crack-free cylindrical superconducting shields as well as strong metal high-Tcceramic joints were demonstrated. 相似文献
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We have substituted 1.5% of Fe for Cu in several “2212” and “2223” Bi-Sr-Ca-Cu superconductors. All of the samples show a reduction ofT c about 13 K due to the Fe impurities. Mössbauer measurements at room temperature reveal the structural characteristics such as stacking faults and intergrowth of different phases in these Bi-based compounds on the microscopic scale. The susceptibility ofT c to Fe-doping in the Bi-“2212” or “2223” system is comparable to that of the “123” system but much smaller than that of the “214” system. The interplanar correlation existing in the “123” and the Bi-“2212” and “2223” systems seems to play an important role in sustaining the high temperature superconductivity and weakening the detrimental effect of impurity elements on superconductivity in these two systems. 相似文献
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We have made superconducting samples of the Y?Ba?Cu?O system with Fe substituted for the Cu. The percentage of Fe substituted varied from 2 to 100. The samples have been verified by x-ray diffraction to be single-phase 1–2–3 compounds. The 6% Fe substitution reduces Tc from 94 K to 80 K. The room temperature Mössbauer spectrum shows two pairs of doublets, indicating there are two distinct Cu sites in the sample. The most surprising result is that magnetic ordering of the Fe coexists with superconductivity of the material at 4.2 K. 相似文献
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Unusual behavior of nuclear relaxation in CeCu2Si2 “possible evidence for triplet superconductivity”
Yoshio Kitaoka Koh-ichi Ueda Takao Kohara Kunisuke Asayama 《Solid State Communications》1984,51(7):461-466
Nuclear relaxation of 63Cu in the superconducting state of the Kondo-lattice system CeCu2Si2 has been studied with the use of the 63Cu nuclear quadrupole resonance technique under zero field and down to 65mK. The nuclear spin-lattice relaxation rate (1/T1) decreases drastically just below Tc=0.67 K down to 0.5Tc without the apparent enchanced behavior and then is found to be almost temperature independent below 0.3Tc. These results suggest that the superconductivity in CeCu2Si2 is not in the usual BCS regime. The analysis based upon the existing triplet pairing model with an anisotropic energy gap describes well the behavior from Tc down to 0.5Tc, while the temperature independence below 0.3Tc remains unexplained. 相似文献