Angular dependence of upper critical field for high-temperature superconductors

2002 ◽  
Vol 66 (1) ◽  
Author(s):  
Kenji Takanaka ◽  
Lui Sakai ◽  
Hiroaki Matueda
2014 ◽  
Vol 2014 ◽  
pp. 1-7 ◽  
Author(s):  
S. Orozco ◽  
R. M. Méndez-Moreno ◽  
M. A. Ortiz

The relation between thed-wave superconducting gapΔ0and the specific heat obtained with the Volovik effect is used to determine the upper critical fieldHc2as doping function, for high-temperature superconductors. A two-components model withd-wave symmetry, within the BCS framework, is introduced to describe the superconducting state. Generalized Fermi surface topologies are used in order to increase the density of states at the Fermi level, allowing the high-Tcvalues observed. The electron-phonon interaction is considered the most relevant mechanism for the high-Tccuprates, where the available phonon energy is provided by the half-breathing modes. The energy gap valuesΔ0calculated with this model are introduced to describe the variation of the upper critical fieldHc2as function of doping, forLa2-xSrxCuO4.


1990 ◽  
Vol 04 (07) ◽  
pp. 471-477 ◽  
Author(s):  
MARKO LEDVIJ ◽  
LJILJANA DOBROSAVLJEVIĆ-GRUJIĆ

The behavior of the perpendicular upper critical field in high T c superconductors is studied theoretically. It is shown, within proximity effect theory, that a substantial deviation from intrinsically linear behavior of [Formula: see text] near T c can occur when imperfections exist in single crystals. A positive curvature arises if there is a competition of superconductivity of two different superconducting phases — the bulk and the defect — in the specimen.


2011 ◽  
Vol 110 (12) ◽  
pp. 123906 ◽  
Author(s):  
F. Weickert ◽  
M. Nicklas ◽  
W. Schnelle ◽  
J. Wosnitza ◽  
A. Leithe-Jasper ◽  
...  

1988 ◽  
Vol 76-77 ◽  
pp. 547-551 ◽  
Author(s):  
G.W. Crabtree ◽  
W.K. Kwok ◽  
U. Welp ◽  
R. Burriel ◽  
H. Claus ◽  
...  

2003 ◽  
Vol 17 (18n20) ◽  
pp. 3415-3422
Author(s):  
Shi-Ping Zhou ◽  
Hao-Chen Du ◽  
Hong-Yin Liao

We study vortex lattice structure of high temperature superconductors by using the Ginzburg–Landau model. The structure of the vortex lattice is oblique at the temperatures well below the transition temperature Tc, where the mixed s–d state is expected to have the lowest energy. Whereas, very close to Tc, the dx2-y2 wave is slightly lower in energy, and a triangular vortex lattice recovers. The coexistence and the coupling between the s- and d-waves account for the upward curvature of the upper critical field curve HC2(T).


1966 ◽  
Vol 20 (2) ◽  
pp. 122-123 ◽  
Author(s):  
K. Yamafuji ◽  
T. Kawashima ◽  
F. Irie

Sign in / Sign up

Export Citation Format

Share Document