In this study, the magnetic and quadrupole moments of the $$Z_b(10650)$$
Z
b
(
10650
)
state are determined using the compact diquark–antidiquark interpolating current through the QCD light-cone sum rule. The values that are obtained as a result of the analysis are as follows: $$\mu _{Z_b} = 2.35^{+0.34}_{-0.33}~\mu _N$$
μ
Z
b
=
2
.
35
-
0.33
+
0.34
μ
N
and $$\mathcal {D}_{Z_b} =(1.82^{+0.35}_{-0.31})\times 10^{-2}~\text{ fm}^2$$
D
Z
b
=
(
1
.
82
-
0.31
+
0.35
)
×
10
-
2
fm
2
. Examining the results obtained, it can be seen that the magnetic moments are large enough to be measured experimentally, while the quadrupole moment is obtained as a small but non-zero value, corresponding to a prolate charge distribution. The magnetic moment is the leading-order response of a bound system to a weak external magnetic field. It therefore provides an excellent platform to probe the internal structures of hadrons governed by the quark-gluon dynamics of QCD.