Pressure Dependence of the Energy Gap Anisotropy in Aluminum

1972 ◽  
Vol 50 (21) ◽  
pp. 2568-2573
Author(s):  
C. R. Leavens ◽  
J. P. Carbotte

We have calculated the superconducting energy gap for a large number of points on the irreducible (1/48)th of the Fermi surface of pure single-crystal aluminum both at zero and finite pressure. It is found that the energy gap anisotropy in aluminum increases with increasing pressure.

1967 ◽  
Vol 163 (2) ◽  
pp. 364-372 ◽  
Author(s):  
J. E. Gueths ◽  
N. N. Clark ◽  
D. Markowitz ◽  
F. V. Burckbuchler ◽  
C. A. Reynolds

2007 ◽  
Vol 21 (18n19) ◽  
pp. 3290-3293 ◽  
Author(s):  
G. L. ZHAO ◽  
D. BAGAYOKO

The superconducting energy gap of YBa 2 Cu 3 O 7 (YBCO) varies strongly with [Formula: see text] and from a sheet of the Fermi surface to another. The strong anisotropic superconducting gap in high Tc materials such as YBCO has led to conflicting d-wave and s-wave interpretations. We have utilized electronic wave functions from the ab-initio density functional calculation and the related electron-phonon interaction matrix elements for the calculation of the superconducting gap values of YBCO. We have found that the superconducting gap on one sheet of the Fermi surface around S-point only shows a minor variation from about 18 meV to 25 meV. Especially, there is no node on this sheet of the Fermi surface around the S-point. We propose a new test measurement of the superconducting gap of YBCO on this sheet of the Fermi surface around the S-point in the Brillouin zone. This measurement is expected to shed light on the gap symmetry properties of high Tc superconductors.


1971 ◽  
Vol 4 (9) ◽  
pp. 2988-2996 ◽  
Author(s):  
S. I. Ochiai ◽  
M. L. A. MacVicar ◽  
R. M. Rose

1994 ◽  
Vol 7 (2) ◽  
pp. 355-360 ◽  
Author(s):  
E. L. Wolf ◽  
A. Chang ◽  
Z. Y. Rong ◽  
Yu. M. Ivanchenko ◽  
Farun Lu

The surface resistance of specimens of superconducting tin and of tin-indium alloys has been measured at a frequency of 140 kmc/s and at temperatures near to the superconducting transition. In both single crystal and polycrystalline alloy specimens, the onset of quantum absorption was well defined and corresponded to an isotropic energy gap with a value at absolute zero of about 3·6 kT c . With pure tin, however, the absorption edge was not well defined in specimens oriented away from the tetrad axis; but near to the tetrad axis, there seems to be a considerable region in which the gap varies com paratively slowly, taking a value of about 3·6 kT c . Assuming that the absence of a clearly defined absorption edge for other orientations is the result of gap anisotropy, it is shown that regions in which the gap takes values very different from 3·6 kT c must lie well away from the tetrad axis. The analysis also shows that such regions are comparatively unimportant, and that the 3·6 kT c gap predominates strongly.


1968 ◽  
Vol 175 (2) ◽  
pp. 556-559 ◽  
Author(s):  
F. V. Burckbuchler ◽  
D. Markowitz ◽  
C. A. Reynolds

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