Penetration depth and pinning effects in high-Tc superconductors La-Sr-Cu-O and (Er, Ho)-Ba-Cu-O studies by μSR

1990 ◽  
Vol 61 (1-4) ◽  
pp. 1093-1096 ◽  
Author(s):  
V. G. Grebinnik ◽  
V. N. Duginov ◽  
V. A. Zhukov ◽  
S. Kapusta ◽  
A. B. Lazarev ◽  
...  
Keyword(s):  
Penetration Depth ◽  
High Tc Superconductors ◽  
High Tc

Anisotropic penetration depth measurements of High-Tc superconductors

1997 ◽  
Vol 282-287 ◽  
pp. 145-148 ◽  
Author(s):  
C. Panagopoulos ◽  
J.R. Cooper ◽  
T. Xiang ◽  
G.B. Peacock ◽  
I. Gameson ◽  
...  
Keyword(s):  
Penetration Depth ◽  
High Tc Superconductors ◽  
High Tc

Evidence of weak pair coupling in the penetration depth of Bi-baseb high-Tc superconductors

1990 ◽  
Vol 165-166 ◽  
pp. 1453-1454 ◽  
Author(s):  
J.R. Thompson ◽  
D.K. Christen ◽  
Yang Ren Sun ◽  
B.C. Chakoumakos ◽  
B.C. Sales ◽  
...  
Keyword(s):  
Penetration Depth ◽  
High Tc Superconductors ◽  
High Tc ◽  
Pair Coupling

scholarly journals Measurements of the absolute value of the penetration depth in high-Tc superconductors using a low-Tc superconductive coating

2000 ◽  
Vol 77 (25) ◽  
pp. 4202-4204 ◽  
Author(s):  
R. Prozorov ◽  
R. W. Giannetta ◽  
A. Carrington ◽  
P. Fournier ◽  
R. L. Greene ◽  
...  
Keyword(s):  
Penetration Depth ◽  
High Tc Superconductors ◽  
High Tc ◽  
Absolute Value ◽  
The Absolute

High Tc superconductors susceptibility: A measurement of their penetration depth

1988 ◽  
Vol 153-155 ◽  
pp. 1493-1494 ◽  
Author(s):  
P. Peyral ◽  
J. Rosenblatt ◽  
A. Raboutou ◽  
C. Lebeau ◽  
C. Perrin ◽  
...  
Keyword(s):  
Penetration Depth ◽  
High Tc Superconductors ◽  
High Tc

The many faces of STEM in materials science

1991 ◽  
Vol 49 ◽  
pp. 440-441
Author(s):  
John Silcox
Keyword(s):  
Materials Science ◽  
Auger Spectroscopy ◽  
Dark Field ◽  
High Tc Superconductors ◽  
High Tc ◽  
Acoustic Environment ◽  
Electromagnetic Vibration ◽  
The Many ◽  
Serial Mode

Determination of the microstructure and microchemistry of small features often provides the insight needed for the understanding of processes in real materials. In many cases, it is not adequate to use microscopy alone. Microdiffraction and microspectroscopic information such as EELS, X-ray microprobe analysis and Auger spectroscopy can all contribute vital parts of the picture. For a number of reasons, dedicated STEM offers considerable promise as a quantitative instrument. In this paper, we review progress towards effective quantitative use of STEM with illustrations drawn from studies of high Tc superconductors, compound semiconductors and metallization of H-terminated silicon.Intrinsically, STEM is a quantitative instrument. Images are acquired directly by detectors in serial mode which is particularly convenient for digital image acquisition, control and display. The VG HB501A at Cornell has been installed in a particularly stable electromagnetic, vibration and acoustic environment. Care has been paid to achieving UHV conditions (i.e., 10-10 Torr). Finally, it has been interfaced with a VAX 3200 work station by Kirkland. This permits, for example, the acquisition of bright field (or energy loss) images and dark field images simultaneously as quantitative arrays in perfect registration.

Crystal chemistry of high-Tc superconductors

1990 ◽  
Vol 48 (4) ◽  
pp. 1118-1119
Author(s):  
Maryvonne Hervieu
Keyword(s):  
Oxygen Deficiency ◽  
Large Family ◽  
Copper Oxides ◽  
High Tc Superconductors ◽  
High Tc ◽  
Single Mechanism ◽  
Square Planar ◽  
History Of ◽  
Bismuth Cuprates ◽  
New Compounds

Four years after the discovery of superconductivity at high temperature in the Ba-La-Cu-O system, more than thirty new compounds have been synthesized, which can be classified in six series of copper oxides: La2CuO4 - type oxides, bismuth cuprates, YBa2Cu3O7 family, thallium cuprates, lead cuprates and Nd2CuO4 - type oxides. Despite their quite different specific natures, close relationships allow their structures to be simply described through a single mechanism. The fifth first families can indeed be described as intergrowths of multiple oxygen deficient perovskite slabs with multiple rock salt-type slabs, according to the representation [ACuO3-x]m [AO]n.The n and m values are integer in the parent structures, n varying from 0 to 3 and m from 1 to 4; every member of this large family can thus be symbolized by [m,n]. The oxygen deficient character of the perovskite slabs involves the existence or the co-existence of several types of copper environment: octahedral, pyramidal and square planar.Both mechanisms, oxygen deficiency and intergrowth, are well known to give rise easily to nonstoichiometry phenomena. Numerous and various phenomena have actually been characterized in these cuprates, strongly depending on the thermal history of the samples.

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