Critical Current Densities JC(H,T) and Current-Voltage Characteristics in Melt Processed Bi-2212 with and without Preferential Orientation

1992 ◽  
Vol 275 ◽  
Author(s):  
W. Paul ◽  
B. Heeb ◽  
Th. Baumann ◽  
M. Guidolin ◽  
L. J. Gauckler

ABSTRACTIn contrast to sintered Bi2Sr2Ca1Cu2Oy (Bi-2212), melt processed material exhibits nonzero intergrain supercurrents at T < 77 K. By means of partial melting and long term annealing we achieved nonoriertted material with Jc(77) - 3500 A/cm2 (1μV/cm criterion) and Tc = 96 K. Zone melting leads to well textured bulk material with the c-axis of the crystallites oriented perpendicular to the pulling direction R, and thus to an anisotropie critical current density. The anisotropy factor is between 2 and 5. At low temperatures the melt textured ceramic exhibits higher critical currents than the nonoriented material. This is not true at high temperatures, since the latter has a higher critical temperature.At 77 K and small fields both oriented and nonoriented ceramics exhibit no transition in their current-voltage characteristics, but obey the power law E = Eo(j/jo(H)) α(H) over a large range in E (10”−3-10”−3 V/cm). Measurements on the textured ceramic with magnetic fields parallel and perpendicular to the pulling direction demonstrate that the superconducting properties of these materials are only affected by the field components parallel to the c-axes of the crystallites. For fields parallel to the pulling direction the measured values of α(H), Jo(H) and of the reversible magnetization Mrev can be attributed to the misorientation of the Bi-2212 platelets which is in average about 14°.

1999 ◽  
Vol 13 (29n31) ◽  
pp. 3718-3720 ◽  
Author(s):  
GIN-ICHIRO OYA ◽  
SHINNOSUKE NOZAWA ◽  
AKINOBU IRIE

We have studied the current-voltage characteristics of intrinsic Josephson junctions in mesa-shaped Bi 2 Sr 2 CaCu 2 O y and ( Bi 1-x Pb x)2 Sr 2 CaCu 2 O y single crystals as a function of x. Pronounced Josephson tunneling characteristics, which are characterized by high critical current densities and multiple quasiparticle branches with clear subgap structures, have been observed for ( Bi ~0.8 Pb ~0.2)2 Sr 2 CaCu 2 O y. A strong correlation between the characteristics and structural modulation in this system has been found.


1988 ◽  
Vol 31 (6) ◽  
pp. 1101-1104 ◽  
Author(s):  
L.A. Delimova ◽  
Yu.V. Zhilyaev ◽  
V.Yu. Kachorovsky ◽  
M.E. Levinshtein ◽  
V.V. Rossin

2014 ◽  
Vol 95 ◽  
pp. 181-185 ◽  
Author(s):  
Kenta Nakazato ◽  
Miryala Muralidhar ◽  
Kazuo Inoue ◽  
Michael R. Koblischka ◽  
Masato Murakami

Bulk YBa2Cu3Oy “Y-123” superconductors with high critical current density (Jc) have been grown by infiltrating a Ba3Cu5Oy “Y-035” liquid source into a Y2BaCuO5 “Y-211” precursor block. Magnetization measurements showed that similar Tc (onset) values and large variation in self-field critical currents were observed when the samples were isothermally grown at different temperatures. We then adapted slow cooling process for the samples 27 mm in diameter and 5 mm in thickness using the growth profile which was optimized on the basis of isothermal growth conditions. The specimens cut from various locations of a large bulk material showed the uniform and sharp superconducting transition with Tc (onset) around 93.2 K. Jc values at 77 K and 0T was in the range of 150 - 175 kA/cm2. Such high Jc values could be obtained without refining the particle size of Y-211 secondary phase. Atomic force microscopy measurements revealed that uniform nanosized secondary Y-211 particles are embedded in the Y-123 matrix, which led to a dramatic improvement of the critical current performance at 77 K.


1999 ◽  
Vol 10 (07) ◽  
pp. 1335-1345
Author(s):  
I. MORGENSTERN ◽  
W. FETTES ◽  
T. HUSSLEIN

The high-Tc glass model can be combined with the repulsive tt'–Hubbard model as microscopic description of the striped domains found in the high-Tc materials. In this picture, the finite Hubbard clusters are the origin of the d-wave pairing. In this paper we show that the glass model can also explain the critical currents usually observed in the high-Tc materials. We use two different approaches to calculate the critical current densities of the high-Tc glass model. Both lead to a strongly anisotropic critical current. Finally we give an explanation of why we nonetheless expect a nearly perfect isotropic critical current in high-Tc superconductors.


2000 ◽  
Vol 338-342 ◽  
pp. 1319-1322
Author(s):  
N.V. Dyakonova ◽  
Pavel A. Ivanov ◽  
V.A. Kozlov ◽  
Michael E. Levinshtein ◽  
John W. Palmour ◽  
...  

2013 ◽  
Vol 740-742 ◽  
pp. 1010-1013 ◽  
Author(s):  
Alexey V. Afanasyev ◽  
Boris V. Ivanov ◽  
Vladimir A. Ilyin ◽  
Alexey F. Kardo-Sysoev ◽  
Maria A. Kuznetsova ◽  
...  

This paper presents the results of research and development of two types diode structures based on wide bandgap 4H-SiC: drift step recovery diodes (DSRDs) and field emission diodes (FED). Diodes’ structure and manufacturing methods are reviewed. Diode’s characteristics were obtained (static current-voltage characteristics and capacitor-voltage characteristic, switching properties’ characteristics for DSRDs). Field emission 4H-SiC structures illustrated high (≥102 А/сm2) current densities at electric field intensity of approximately 10V/um. 4H-SiC DSRDs in the generator structure with a single oscillating contour allowed to form sub nanosecond impulses at a load 50 Ohm and 1,5-2kV amplitude for a single diode (current density at V=2kV J= 4•103 А/сm2),what is significantly higher than similar DSRD’s parameters obtained for silicon.


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