Form factor, standard deviation, and skewness of the field distribution in a hard type-II heavy-fermion superconductor from the Ginzburg-Landau model

2011 ◽  
Vol 84 (1) ◽  
Author(s):  
P. Dalmas de Réotier ◽  
A. Yaouanc
1985 ◽  
Vol 57 (8) ◽  
pp. 3087-3089 ◽  
Author(s):  
C. Stassis ◽  
J. D. Axe ◽  
C. F. Majkrzak ◽  
B. Batlogg ◽  
J. Remeika

2003 ◽  
Vol 14 (1) ◽  
pp. 111-127 ◽  
Author(s):  
E. COSKUN ◽  
Z. CAKIR ◽  
P. TAKAC

The standard scales that are used to non-dimensionalize the temperature- and time-dependent Ginzburg–Landau (TTDGL) model developed by Schmid [27], eliminate temperature- dependent parameters, and thus do not allow for superconducting phenomena due to variations in temperature. In this study, a set of new scales is presented to non-dimensionalize the TTDGL model so that the resulting dimensionless system depends upon a temperature parameter as well. Moreover, some properties of solutions to TTDGL system as a function of temperature are explored. Numerical experiments illustrating the temperature-dependency of vortex nucleation in type-II superconductors as well as the transition to the Meissner state in type-I superconductors are presented.


2002 ◽  
Vol 106-107 ◽  
pp. 959-961 ◽  
Author(s):  
K. Kajantie ◽  
M. Laine ◽  
T. Neuhaus ◽  
A. Rajantie ◽  
K. Rummukainen

2021 ◽  
Vol 2021 (8) ◽  
Author(s):  
Alexander A. Penin ◽  
Quinten Weller

Abstract We elaborate a theory of giant vortices [1] based on an asymptotic expansion in inverse powers of their winding number n. The theory is applied to the analysis of vortex solutions in the abelian Higgs (Ginzburg-Landau) model. Specific properties of the giant vortices for charged and neutral scalar fields as well as different integrable limits of the scalar self-coupling are discussed. Asymptotic results and the finite-n corrections to the vortex solutions are derived in analytic form and the convergence region of the expansion is determined.


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