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 $$E_{\varepsilon ,\delta }$$
E
ε
,
δ
, where $$\varepsilon $$
ε
represent the coherence length (in the Ginzburg–Landau model) or the core-radius size (in the core-radius approach) and $$\delta $$
δ
denotes the periodicity scale. We carry out the $$\Gamma $$
Γ
-convergence analysis of $$E_{\varepsilon ,\delta }$$
E
ε
,
δ
as $$\varepsilon \rightarrow 0$$
ε
→
0
and $$\delta =\delta _\varepsilon \rightarrow 0$$
δ
=
δ
ε
→
0
in the $$|\log \varepsilon |$$
|
log
ε
|
scaling regime, showing that the $$\Gamma $$
Γ
-limit consists in the energy cost of finitely many vortex-like point singularities of integer degree. After introducing the scale parameter $$\begin{aligned} \lambda =\min \Bigl \{1,\lim _{\varepsilon \rightarrow 0} {|\log \delta _\varepsilon |\over |\log \varepsilon |}\Bigr \} \end{aligned}$$
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 $$\varepsilon ^\lambda $$
ε
λ
we first have a concentration process around some vortices whose location is subsequently optimized, while for scales larger than $$\varepsilon ^\lambda $$
ε
λ
the concentration process takes place “after” homogenization.