Inhomogeneous charging problem in XPS measurement of surface contaminated high-TC superconducting material

1990 ◽  
Vol 52 ◽  
pp. 395-404 ◽  
Author(s):  
Liang Zhong Zhao
1989 ◽  
Vol 20 (8) ◽  
pp. 1353-1356 ◽  
Author(s):  
Wolf Wilczek ◽  
Elisabeth Drosselmeyer ◽  
Ines Lind ◽  
Elisabeth Mainka ◽  
Arnulf Seidel

1989 ◽  
Vol 42 (4) ◽  
pp. 431 ◽  
Author(s):  
CB Smith ◽  
JM BelI ◽  
N Savvides ◽  
S Filipczuk ◽  
C Andrikidis

Experimental resistance versus temperature plots measured in various magnetic fields up to 7 T in strength are presented for highly oriented YBaCu oxide thin films deposited onto crystalline zirconia. Possible broadening mechanisms are summarised and a detailed analysis made for three models which involve processes intrinsic to the ideal superconducting material. It is shown that two distinct potentials may be needed to understand flux pinning in different temperature ranges below Te. These two potentials have quite different temperature and field dependence.


1989 ◽  
Vol 32-33 ◽  
pp. 1125-1132 ◽  
Author(s):  
H LIU ◽  
D COCKE ◽  
D NAUGLE ◽  
R PANDEY

1994 ◽  
Vol 30 (1) ◽  
pp. 92-93 ◽  
Author(s):  
L.P. Ivrissimtzis ◽  
T.S.M. Maclean ◽  
N. McN. Alford ◽  
M.J. Lancaster

1989 ◽  
Vol 160 (3-4) ◽  
pp. 369-374 ◽  
Author(s):  
J. Hagberg ◽  
A. Uusimäki ◽  
J. Levoska ◽  
S. Leppävuori

Author(s):  
C. Barry Carter ◽  
Lisa A. Tietz

Interfaces in high-Tc superconducting oxides are influential during both the processing of bulk materials and the growth of thin epitactically aligned layers. In the first case, the formation of the superconducting phase involves the movement of phase boundaries during the solid-state reaction, while in the second, the phase boundary is formed as the superconducting material grows on the single-crystal substrate. Having formed the superconducting material, the superconducting phase will, in general, contain a large number of grain boundaries varying from the simple twin boundaries which can be produced during the cubic-to-tetragonal transformation, to low-angle grain boundaries, special high-angle grain boundaries, other high-angle grain boundaries and phase boundaries due to incomplete or on-going solid-state reactions. During the course of this presentation, recent results on these topics will be reviewed, paying particular attention to the more widely studied material, YBa2Cu3O6+x.The importance of grain boundaries in high-Tc superconducting oxides has been firmly established by the systematic analysis of Dimos et al who have shown that the misorientation of the grains in layers of YBa2Cu3O6+x which had been grown on polycrystalline SrTiO3 substrate varies with the relative misorientation between the grains.


Author(s):  
H.-J. Ou ◽  
J. M. Cowley

Using the dedicate VG-HB5 STEM microscope, the crystal structure of high Tc superconductor of YBa2Cu3O7-x has been studied via high resolution STEM (HRSTEM) imaging and nanobeam (∽3A) diffraction patterns. Figure 1(a) and 2(a) illustrate the HRSTEM image taken at 10' times magnification along [001] direction and [100] direction, respectively. In figure 1(a), a grain boundary with strong field contrast is seen between two crystal regions A and B. The grain boundary appears to be parallel to a (110) plane, although it is not possible to determine [100] and [001] axes as it is in other regions which contain twin planes [3]. Following the horizontal lattice lines, from left to right across the grain boundary, a lattice bending of ∽4° is noticed. Three extra lattice planes, indicated by arrows, were found to terminate at the grain boundary and form dislocations. It is believed that due to different chemical composition, such structure defects occur during crystal growth. No bending is observed along the vertical lattice lines.


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