  In non-central heavy-ion collisions, spectator protons that do not
participate in the interaction create strong magnetic fields. The strength of
these fields allows testing an effect based on the hypothesized properties of
QCD. The presence of so-called topological configurations can give rise to
domains that carry net chirality. Coupled with the aforementioned magnetic
fields, they may induce a charge separation of the particles generated in the
collisions. This charge separation is called the Chiral Magnetic Effect (CME)
and can be measured through charged-particle angular correlations. Measurements
of the $\gamma_{1,1}$ correlator, which is sensitive to the CME, are shown for
Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV as well as for Xe--Xe
collisions at $\sqrt{s_{\mathrm{NN}}} = 5.44$ TeV. These are found to have a
significant charge dependence between opposite-sign and same-sign charge pairs.
This behavior is consistent with a CME-like signal. However, the $\delta_{1}$
correlator, which measures charge correlations unrelated to any symmetry plane
(i.e. background), was measured in Xe--Xe collisions and also shows a
significant charge dependence. This prevents a clear interpretation of the
$\gamma_{1,1}$ correlator. Novel methods to constrain the CME contribution to
the $\gamma_{1,1}$ correlator are necessary.
