  We present exact results for the fluctuations in the number of particles
crossing the origin up to time $t$ in a collection of non-interacting run and
tumble particles in one dimension. In contrast to passive systems, such active
particles are endowed with two inherent degrees of freedom: positions and
velocities, which can be used to construct density and magnetization fields. We
introduce generalized disorder averages associated with both these fields and
perform annealed and quenched averages over various initial conditions. We show
that the variance $\sigma^2$ of the current in annealed versus quenched
magnetization situations exhibits a surprising difference at short times:
$\sigma^2 \sim t$ versus $\sigma^2 \sim t^2$ respectively, with a $\sqrt{t}$
behavior emerging at large times. Our analytical results demonstrate that in
the strictly quenched scenario, where both the density and magnetization fields
are initially frozen, the fluctuations in the current are strongly suppressed.
Importantly, these anomalous fluctuations cannot be obtained solely by freezing
the density field.
