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1.
Crystalline samples of La3Ni2B2N3 were synthesized using solid state metathesis reactions from combinations of La, LaCl3, NiCl2 together with Li3BN2. The structure was determined by single crystal X‐ray diffraction (I4/mmm (No. 139), a = 372.95(2) pm, c = 2056.3(2) pm, R1 = 0.027, wR2 = 0.062) and confirmed earlier results from neutron powder diffraction. La3Ni2B2N3 contains BN units capping square planar Ni layers. Isolated nitrogen atoms reside in La6 octahedra. Magnetic measurements on several bulk samples exhibit superconductivity at temperatures below 14.6 K. 相似文献
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We present the thermoelectric and superconducting properties of the bulk misfit-layered (SnSe)1.17(TaSe2) compound with the critical temperature (Tc ~ 3.8 K). From XRD and electrical resistivity, the anisotropic properties of the misfit-layered compound by the preferred orientation were observed. The zero-temperature-limit upper critical field Hc2(0) and coherence length ξ are obtained by Hc2(0) = 8.94 T and ξ = 6.1 nm. The electron-phonon coupling constant (λe-p = 0.735) and the specific heat jump (ΔCe/γTc ~ 1.4) imply that the (SnSe)1.17(TaSe2) compound is a weak coupled conventional s-wave superconductor. Density functional theory (DFT) calculation results show that some electronic charge transfers from the SnSe layers into the TaSe2 layers. In addition, the thermoelectric properties of the bulk misfit-layered (SnSe)1.17(TaSe2) compound show significant anisotropic properties. 相似文献
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In-plane single domain and vortex magnetization configurations of the magnetic dot in the hybrid superconductor–ferromagnet system are considered. Single domain configuration energy shift due to the presence of superconductor is calculated. The change of the phase curve of the ferromagnetic dot magnetization due to the repulsion of the magnetic field by the superconductor is obtained. Up to the two-fold decrease of the ferromagnetic dot critical radius due to the presence of the superconductor is predicted. 相似文献
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H. Kitaguchi K. Itoh T. Takeuchi H. Kumakura H. Miao H. Wada K. Togano T. Hasegawa T. Koizumi 《Physica C: Superconductivity and its Applications》1999,320(3-4):253-258
High-transport critical current density (Jc-oxide)>500 kA/cm2 at 4.2 K, 10 T can be obtained for Bi-2212/Ag tapes fabricated by using pre-annealing and intermediate rolling (PAIR) and melt-solidification process. In this paper, we report high-temperature properties of PAIR-processed Bi-2212/Ag multilayer tape in order to show their potential for practical applications operated at cryocooling temperatures. Magnetic field dependence and angular dependence of critical current (Ic) are investigated at temperatures ranging 10–50 K by using helium gas cooling and liquid neon. Field-temperature curves for Ic=0.2 and 2.0 A are also determined in order to show the approximation of the irreversible field. High-temperature performance of the tape is attractive to consider future applications. For example, the best sample carries Ic=267 A (engineering-Jc=303 A/mm2, Jc-oxide=151 kA/cm2) and 92 A (104 A/mm2, 52 kA/cm2) at 27.1 K (in liquid neon), in magnetic fields (parallel to the tape surface) of 2 and 10 T, respectively. Engineering-Jc of 100 A/mm2 is obtained even in the perpendicular field of 0.5 T at 27.1 K. 相似文献
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分光光度法测定铋系超导材料中钙 总被引:1,自引:0,他引:1
在pH=10.6的NH3-NH4Cl缓冲溶液中,钙离子和酸性铬蓝K显色,于498nm波长处以试剂空白作参比,测定该显色液的吸光度。建立了铋系超导前驱粉(Bi2Sr2Ca2Cu3Ox)中直接测定钙含量的方法。试样中大量存在的锶不干扰测定,用柠檬酸溶液作掩蔽剂,消除了铜的干扰。ε=9.0×103L·mol-1·cm-1,Ca在0—50μg·25mL-1范围内吸光度和浓度有良好的线性关系,回归系数r=0.9994。对合成样品进行6次测定,相对误差为-0.93%。对两种实际样品分别进行6次测定,RSD分别为1.63%和1.19%。 相似文献
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T. Tsuneta T. Toshima K. Inagaki T. Shibayama S. Tanda S. Uji M. Ahlskog P. Hakonen M. Paalanen 《Current Applied Physics》2003,3(6):473-476
We succeed in synthesizing NbSe2 nanotubes along with nanofibers by chemical vapor transportation. They are stable crystalline systems and can be synthesized reproducibly in a nearly equilibrium reacting process. We have investigated these nanosize structures of NbSe2 by transmission electron microscopy and electron diffraction. Both of the structures have a similar size of 100–200 nm in diameter. While nanotubes consist of rolled-up NbSe2 layers, nanofibers are a pile of thin flat layers. We propose a mechanism of the formation of NbSe2 nanotubes and nanofibers on the basis of deseleniditive transition from a NbSe3 fiber-shaped crystal. We also measured electrical resistance of the nanofibers with conductive atomic force microscopy and demonstrated that the material show metallic behavior at room temperature. 相似文献
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