The electroweak (EW) sector of the Minimal Supersymmetric Standard Model (MSSM), with the lightest neutralino as Dark Matter (DM) candidate, can account for a variety of experimental data. This includes the DM content of the universe, DM direct detection limits, EW SUSY searches at the LHC and in particular the so far persistent $$3-4\,\sigma $$
3
-
4
σ
discrepancy between the experimental result for the anomalous magnetic moment of the muon, $$(g-2)_\mu $$
(
g
-
2
)
μ
, and its Standard Model (SM) prediction. The recently published “MUON G-2” result is within $${0.8}\,\sigma $$
0.8
σ
in agreement with the older BNL result on $$(g-2)_\mu $$
(
g
-
2
)
μ
. The combination of the two results was given as $$a_\mu ^{\mathrm{exp}} = (11 659 {206.1}\pm {4.1}) \times 10^{-10}$$
a
μ
exp
=
(
11659
206.1
±
4.1
)
×
10
-
10
, yielding a new deviation from the SM prediction of $$\Delta a_\mu = ({25.1}\pm {5.9}) \times 10^{-10}$$
Δ
a
μ
=
(
25.1
±
5.9
)
×
10
-
10
, corresponding to $${4.2}\,\sigma $$
4.2
σ
. Using this improved bound we update the results presented in Chakraborti et al. (Eur Phys J C 80(10):984, 2020) and set new upper limits on the allowed parameters space of the EW sector of the MSSM. We find that with the new $$(g-2)_\mu $$
(
g
-
2
)
μ
result the upper limits on the (next-to-) lightest SUSY particle are in the same ballpark as previously, yielding updated upper limits on these masses of $$\sim 750 \,\, \mathrm {GeV}$$
∼
750
GeV
. In this way, a clear target is confirmed for future (HL-)LHC EW searches, as well as for future high-energy $$e^+e^-$$
e
+
e
-
colliders, such as the ILC or CLIC.