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Topological Singularities in Periodic Media: Ginzburg–Landau and Core-Radius Approaches
We describe the emergence of topological singularities in periodic media within the Ginzburg–Landau model and the core-radius approach. The energy functionals of both models are denoted by E ε , δ , where ε represent the coherence length (in the Ginzburg–Landau model) or the core-radius size (in the...
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Published in: | Archive for rational mechanics and analysis 2022-02, Vol.243 (2), p.559-609 |
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Main Authors: | , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We describe the emergence of topological singularities in periodic media within the Ginzburg–Landau model and the core-radius approach. The energy functionals of both models are denoted by
E
ε
,
δ
, where
ε
represent the coherence length (in the Ginzburg–Landau model) or the core-radius size (in the core-radius approach) and
δ
denotes the periodicity scale. We carry out the
Γ
-convergence analysis of
E
ε
,
δ
as
ε
→
0
and
δ
=
δ
ε
→
0
in the
|
log
ε
|
scaling regime, showing that the
Γ
-limit consists in the energy cost of finitely many vortex-like point singularities of integer degree. After introducing the scale parameter
λ
=
min
{
1
,
lim
ε
→
0
|
log
δ
ε
|
|
log
ε
|
}
(upon extraction of subsequences), we show that in a sense we always have a separation-of-scale effect: at scales smaller than
ε
λ
we first have a concentration process around some vortices whose location is subsequently optimized, while for scales larger than
ε
λ
the concentration process takes place “after” homogenization. |
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ISSN: | 0003-9527 1432-0673 1432-0673 |
DOI: | 10.1007/s00205-021-01731-7 |