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1.
A study of the environmental contamination of amorphous YBa2Cu3O7- fibers has been undertaken in order to determine the best method to handle these materials during the fabrication of superconducting wire. The fibers often need to be handled in organic solvents as part of the cleaning and manipulating process. In organics that are free of water, the fibers retain their mechanical strength with little carbon contamination or other ill effects. Water, however, causes premature crystallization and destroys the mechanical strength of the fibers.  相似文献   

2.
    
Single-crystal YBa2Cu3O (YBCO) has been made with some of the copper atoms in the copper-oxygen chains replaced by gold. The samples were made by a flux method. The gold concentration was determined by EDX (energy-dispersive X-ray spectroscopy) as a function of the nominal (i.e., flux) composition. Up to about 4.8% of all the copper atoms can be replaced by gold. The effect of the gold doping on the superconducting transition temperature (T c ) and the transition width (T c ) were determined.  相似文献   

3.
    
The effects of neutron irradiation on the critical temperature and critical current density at 77 K and zero magnetic field of high-temperature superconductors was studied in Li-doped YBa2Cu3O7–x . Damage and thermal neutron reactions with Li produce an insignificant increase of the critical temperature for Li inserted as flame-melted Li2CuO2 while for the others it remains nearly unaffected. The critical transport current density of the sintered YBa2Cu3O7–x remains unaffected for samples with Li2CuO2 and shows a decrease for LiFdoped samples.  相似文献   

4.
    
High-resolution electron microscopy (HREM) studies of grain boundaries and fractured surfaces in both the tetragonal and orthorhombic phases of dense (>90%) YBa2Cu3O7– and tetragonal LaBaCaCu3O7– have been conducted. Grain boundaries in polycrystalline YBa2Cu3O7– are found to be frequently parallel to a (001) plane of one of the adjacent grains, with a structure similar to that of the (001) surface of fractured YBa2Cu3O7-gd. Matching of experimental and calculated images shows that the outermost surface layer in this compound is a deformed BaO layer. Both grain boundaries and fractured surfaces in LaBaCaCu3O7– show no such tendency for preferential orientation of the interface plane. Results indicate that the low critical currents observed in sintered materials are caused by textured grain growth in combination with the atomic structure of the grain boundary plane, and the intercalation of off-stoichiometric species near the grain boundary.  相似文献   

5.
The disordered vortex phases induced by line and point pinning in YBa2Cu3O7– are explored. At high defect densities, only a single disordered solid separated from the liquid phase by a melting line is observed. At low defect densities the topology of the phase diagram changes dramatically, with a vortex lattice phase adjoining disordered phases at high or low field. Critical points at the termination of the first-order melting line separate the lattice and the disordered phases. The line defect disordered phases follow the expected Bose glass behavior, while the point defect disordered phases do not exhibit the expected vortex glass behavior.  相似文献   

6.
    
The specific heat of twinned and detwinned single crystal samples of YBa2Cu3O7– have been measured with magnetic fields up to 8 tesla applied parallel to the c-axes of the crystals. The samples measured had transition temperatures around 90K and transition widths from 0.3 K to 2 K. The data exhibits scaling behaviour characteristic of the 3-dimensional-X-Y model with critical exponents consistent with those observed in superfluid4He. We then compare the scaling properties of the specific heat in the different samples and look for the universal nature of the scaling function.  相似文献   

7.
Four-probe resistivity () and thermoelectric power (TEP) measurements were carried out on samples of YBa2Cu3O7– up to 950°C, in air and in flowing oxygen at 1 bar. Below 700 K the TEP is small and increases rapidly above it, reaching, at 1200 K, +140V/K in air and +120V/K in oxygen. At the changeover temperature (700 K) the slope of log vs.T changes abruptly. These results are interpreted in terms of a model of transport of carriers in a narrow band, which is full for = 1 and half-filled for = 0. Possible origins for such a narrow band are discussed in detail.  相似文献   

8.
    
An overview is given of three techniques for preparing thin specimens of YBa2Cu3O7- for high-resolution electron microscopy: grinding, cleaving, and ion milling. Advantages and disadvantages are described, with particular attention to the artefacts that may be introduced by the different techniques. It is concluded that the most serious problem encountered during high-resolution electron microscopy studies is a surface-initiated decomposition leading to the ultimate degradation of the structure. This problem was found to be most pronounced in ion-milled specimens.  相似文献   

9.
An analytical method is presented for investigating the resonant behavior of a c-axis oriented YBa2Cu2O7–(0) thin film on a resonator composed of LaAlO3 (001). The concept of the negative dielectric medium for a superconductor is introduced within the framework of the two-fluid model, which permits us to treat a superconductor as any other penetrable materials so that only its electromagnetics are concerned. A conformai transformation is further suggested to map the original open boundary-value problem to a closed one. This not only makes the original problem readily solvable by using the variational technique, but is also a powerful tool for analyzing some kinds of problems such as the propagation characteristics of the superconducting microstripe and coplanar waveguide structures.  相似文献   

10.
    
We have measured the in-plane longitudinal resistivities a and b as functions of temperature and magnetic field. The measurements were all made on the same detwinned single crystal of YBa2Cu3O7 – (YBCO). DefiningT c to be at the onset of resistance, it is the same for a and b in a magnetic field ranging from 0 to 3.5 T. In zero field,T c = 93.4 K, so the oxygen doping of the crystal was approximately optimal. In the mixed state, the anisotropy ratio of the resistivities ( a/b) decreases with decreasingT orH, and the chain conductivity ( b-a) is smaller than the plane conductivity ( a). Both a and b increase with decreasing temperature, and so does ( b-a).  相似文献   

11.
The melt-texture growth (MTG) method has been shown to be effective in fabricating high-T csuperconducting bulk samples with highly oriented layers of single crystals. The critical current densityJ cof the typical samples are enhanced significantly. Furthermore, making use of the nonzero spatial temperature gradient at certain locations of a common tube furnace, we fabricated Y-123 bulk samples with various dopants allowingJ cup to 3.0×104 A cm–2 in our recent investigations. We followed up our project by analyzing the relations among the crucial parameters involved in the modified version of the MTG process. These parameters include the temperature gradient, the time rate of change of temperature, the growth front of the crystal, etc. Our study indicates that some of the empty space regions that appear between layers are only shallow gap lines. True layers of single crystals do exist, and we present an explanation for the growth of crystal layers along special directions as observed.  相似文献   

12.
We present measurements of the uniaxial pressure dependence ofT c of untwinned YBa2Cu3O7– crystals with various oxygen stoichiometries. For all samples investigated,T c decreases for pressure alonga, increases for pressure alongb, and, in oxygen deficient samples, increases strongly for pressure alongc. These results are compared to the behavior found in the La2–x Sr x CuO4 and YBa2Cu4O8 systems. Neither the model of pressure-induced charge transfer nor coupling to orthorhombic distortions can explain all the data. However, the presence of singularities in the electronic density of states close to the Fermi energy is a possible origin of the observed behavior. Our preliminary data on the pressure dependence of thec-axis and in-plane resistivities in twinned crystals are consistent with this view.  相似文献   

13.
The effects of Ce-based additions (CeO2 and BaCeO3) in combination with MgO additions on the magnetic properties of melt-textured YBa2Cu3O7 – and ErBa2Cu3O7 – have been investigated. The additions lead to improvements in the magnetic properties of both RE-123 compounds compared to samples with either addition alone or with no additions. The Ce–Mg addition combination produces a peak effect in the magnetic hysteresis loop without significant T c degradation. This is postulated to be due to the formation of a new type of pinning center. Both Ce and Mg ions are thought to substitute in the RE-Ba2Cu3O7 – lattice, creating defects that produce a peak effect in the magnetic hysteresis loop. Mg additions alone lead to a reduced T c, while Ce additions restore the T c and enhance the magnitude of the peak.  相似文献   

14.
Picosecond nonequilibrium and slow bolometric responses to infrared radiation from a patterned high-T c superconducting (HTS) film in resistive and normal states deposited onto LaAlO3, NdGaO3, and MgO substrates were investigated using both pulse and modulation techniques. The response time of 35 ps to a laser pulse of 17 ps FWHM has been observed. The intrinsic response time of the fast process is expected to be about a few picoseconds. The modulation technique, being free from the disadvantages of pulse methods (poor sensitivity, limited dynamic range), makes the detailed study of a number of relaxation processes possible. Besides the nonequilibrium response, two kinds of bolometric processes, namely phonon transport through the film-substrate interface and phonon thermal diffusion in a substrate, manifest themselves in certain frequency dependences.  相似文献   

15.
We have doped the YBa2Cu3O7– superconducting ceramics with BaZrO3 up to 75wt.% and studied the changes of some physical properties. The most important finding is the enhancement of the critical current density, which has a maximum at around 5 wt.% doping level. Compared with the undoped samples, the critical current density is four times higher if the doping compound is introduced prior to the calcination treatment, or two times higher if BaZrO3 is introduced prior to the sintering treatment. The dependence of the critical current density on the doping level is consistent with the dependence of the Seebeck coefficient. We also observed a very small decrease of the critical temperature. The real density of the samples decreases with increasing doping level as expected from the ratio between the theoretical densities of YBa2Cu3O7– and BaZrO3, the effect being important for doping levels higher than 25 wt.%.  相似文献   

16.
The morphology of the silver films deposited and annealed on laser ablated YBa2Cu3O7– thin films and the corresponding contact resistivity have been systematically investigated. A minimum contact resistivity of 6 × 10–8 cm2 was reached at 77 K by annealing Ag/YBa2Cu3O7– contact at the optimum temperature. The effect of the annealing temperature on the contact resistivity was explained by considering the morphology of the silver films and the diffusion of silver into YBa2Cu3O7– film, etc. The difference of the contact resistivity for Ag contact to polycrystalline, single crystal and thin film of YBa2Cu3O7– were also explained.  相似文献   

17.
A 1201-phase superconductor (Pb0.5Cu0.5)SrLaCuO exhibiting a zero-resistance (R=0) state at 21 K has been synthesized. Neutron Rietveld refinement of the structure shows substantial oxygen disorder in the (Pb/Cu)-O(3) monolayer and excess occupancy of oxygen at the O(3) sites. The superconducting behavior of (Pb0.5Cd0.5)SrLaCuO , prepared under identical conditions, yields a value ofT c (R=0) equal to 24 K. The presence of extra oxygen appears to be responsible for trapping of holes within the rock-salt (Pb/Cu)-O(3).  相似文献   

18.
Previously, we have observed that parallel lattice fringes show up regularly in MTG samples, indicative of good alignment of unit cells in strips of size 100 nm × a few times 100 nm. We have prepared films ( 80 nm) for TEM observation using YBCO material fabricated by the conventional solid-state reaction method in order to study the crystal texture in a length scale from a few 100 nm down to 3 Å. Parallel lattice fringes are observed to stretch across a cross-section 0.3×0.5 m2. Cross lattice fringes intersecting at 90° and 45° are observed as rare events. This result suggests that the degree of alignment in the crystal texture is higher than expected inside a grain of size a few m.  相似文献   

19.
    
Experimental results of research on the influence of deposition temperature (T s) on crystal structure and superconductivity of Y1–x HoxBa2Cu3O7 – (YHBCO) films deposited by dcmagnetron sputtering are reported. X-ray diffraction analysis showed that the films grew with preferential orientation of thec-axis normal to the substrate surface in the range of temperature 750–820°C. The single-crystal structure of the YHBCO films grown epitaxially at the optimal substrate temperatures of 820, 800, 760, and 750°C, respectively, have been established by rocking curves, -scan, and electron channeling pattern (ECP). Typical values of the critical current density (A · cm–2) at 77 K and 0.1 T field are 2.1×105, 4×105, 6.2×105, and 3.1×105 for thex=0, 0.2, 0.4, 0.7 films respectively, measured by a Quantum Design magnetrometer (Hc).  相似文献   

20.
We have fabricated a series of glass-ceramic (Bi2 – Zn) Sr2Ca2Cu3O10 + y , where = 0.0, 0.2, 0.4, 0.6, 0.8, and 1.0, and investigated the effect of Zn ions on the glass formation, crystallization, thermal, electrical, and on the magnetic properties of the BSCCO-2223 superconductor system. The structural symmetry was found to be tetragonal in all the substitution levels. The best electrical performance was obtained from the = 0 sample, the T c and T zero was obtained at 110 K and 107 K, respectively. The J c values of the samples were determined using the magnetization hysteresis and Bean's model. The crystallization kinetics were investigated using nonisothermal models of Augis–Bennett. The calculated activation energy, E a, of the system was found to be in the range of 258–336 kJ/mol.  相似文献   

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