Journal of Superconductivity and Novel Magnetism
https://doi.org/10.1007/s10948-018-4586-y
ORIGINAL PAPER
Numerical Simulation of Phase Transitions in Type-II Annular
Superconductor Using Time-dependent Ginzburg-Landau Equations
Hasnain Mehdi Jafri
1
· Xingqiao Ma
1
· Congpeng Zhao
1,2
· Houbing Huang
1
· Tauseef Anwar
3
· Zhuhong Liu
1
·
Long-Qing Chen
4
Received: 8 January 2018 / Accepted: 24 January 2018
© Springer Science+Business Media, LLC, part of Springer Nature 2018
Abstract
Time-dependent Ginzburg-Landau equations were solved by finite element method in two-dimensional space for order
parameter and energy components of the annular superconducting sample in steady magnetic fields. Vortices preferred to
penetrate from the inner surface of the annulus due to lesser energy required at the concave surface. A transition magnetic
field strength was observed in spatial averages of carrier concentration and energy components, showing small bumps
and abrupt variations, indicating phase transition from a non-vortex to vortex state. These effects were observed to repeat
with every subsequent entry of a set of vortices into the sample; transition magnetic field strength was found to depend
inversely on the annular width of the sample. The present work gives a better understanding of energy variations during
phase transition from non-vortex to vortex state and predicts that vortex state can be avoided by tuning the wire thickness in
practical applications, e.g., superconducting electromagnets.
Keywords Ginzburg-Landau model · Abrikosov vortices · Type-II superconductor
1 Introduction
In mesoscopic superconductors (dimensions of the order of
coherence length ξ or penetration depth λ) surface effects are
responsible for properties which are not present in bulk samples
[1–5]. As a result, the vortex configurations in mesoscopic
samples are strongly sample geometry-dependent [4] contrary
to triangular vortex pattern observed in bulk samples [6].
Xingqiao Ma
xqma@sas.ustb.edu.cn
1
Department of Physics, University of Science and Technology
Beijing, Beijing 100083, China
2
ASIC, China Center for Information Industry Development,
Beijing 100083, China
3
Energy Research Centre, COMSATS Institute of Information
Technology, Lahore, Pakistan
4
Department of Materials Science and Engineering,
The Pennsylvania State University, University Park,
PA 16802, USA
Appearance of two different states, i.e., multi-vortex state
[7, 8] and giant vortex state [9–11] at mesoscopic size, have
prompted studies with surprising results such as the paramag-
netic Meissner effect [12], symmetry-induced antivortices
[13], giant [11] and fractional-flux [14] vortices, and vortices
trapped in blind holes [15].
According to famous Bardeen-Cooper-Schrieffer (BCS)
theory, the ground state of condensate consists of oppo-
site spin electron pairs (spin singlet state) bound by phonon
interactions [16]. Ginzburg pointed out that this fragile
state is destroyed by the development of homogeneous fer-
romagnetic order of spins if its corresponding magnetic
field exceeds thermodynamical critical magnetic field of
that superconductor. Ginzburg-Landau (GL) theory [17]
is probably the most successful macroscopic description
of superconductivity. The proposed macroscopic quantum
theory by Ginzburg and Landau makes use of a quartic
potential and the Higgs mechanism of spontaneous symme-
try breaking [18–21] to generate a local mass term of vector
potential. It successfully describes the Meissner-Ochsenfeld
effect [20, 22–25] for magnetic flux expulsion, the phe-
nomenology associated with phase transition [26–28], and