Motivated by the recent observation of the tetraquark $$ {T}_{cc}^{+} $$
T
cc
+
, we investigate the magnetic dipole moments of the possible single and double strange partners, $$ {T}_{QQ\overline{q}\overline{s}} $$
T
QQ
q
¯
s
¯
and $$ {T}_{QQ\overline{s}\overline{s}} $$
T
QQ
s
¯
s
¯
, with the spin-parity JP = 1+ by means of the QCD light-cone sum rules. To this end, we model these states as diquark-antidiquark states with different organizations and interpolating currents. The results of magnetic dipole moments obtained using different diquark-antidiquark structures differ from each other, considerably. The magnetic dipole moment is the leading-order response of a bound system to a soft external magnetic field. Therefore, it provides an excellent platform for investigation of the inner structures of hadrons governed by the quark-gluon dynamics of QCD.