We study the pseudo-spin density response of a disordered two-dimensional spin-polarized Bose
gas of exciton polaritons to weak alternating magnetic eld, assuming that one of the spin states of
the doublet is macroscopically occupied and Bose-condensed while the occupation of the other state
remains much smaller. We calculate spatial and temporal dispersions of spin susceptibility of the
gas taking into account spin-
ip processes due to the transverse-longitudinal splitting. Further, we
use the Bogoliubov theory of weakly-interacting gases and show that the time-dependent magnetic
eld power absorption exhibits double resonance structure corresponding to two particle spin states
(contrast to paramagnetic resonance in regular spin-polarized electron gas). We analyze the widths
of these resonances caused by scattering on the disorder and show that, in contrast with the ballistic
regime, in the presence of impurities, the polariton scattering on them is twofold: scattering on the
impurity potential directly and scattering on the spatially
uctuating condensate density caused
by the disorder. As a result, the width of the resonance associated with the Bose-condensed spin
state can be surprizingly narrow in comparison with the width of the resonance associated with the
non-condensed state.