  We propose a device consisting in an antidot periodically driven in time by a
magnetic field as a fractional quantum Hall counterpart of the celebrated
mesoscopic capacitor-based single electron source. We fully characterize the
setup as an ideal emitter of individual quasiparticles and electrons into
fractional quantum Hall edge channels of the Laughlin sequence. Our treatment
relies on a master equation approach and identifies the optimal regime of
operation for both types of sources. The quasiparticle/quasihole emission
regime involves in practice only two charge states of the antidot, allowing for
an analytic treatment. We show the precise quantization of the emitted charge,
we determine its optimal working regime, and we compute the phase noise/shot
noise crossover as a function of the escape time from the emitter. The emission
of electrons, which calls for a larger amplitude of the drive, requires a full
numerical treatment of the master equations as more quasiparticle charge states
are involved. Nevertheless, in this case the emission of one electron charge
followed by one hole per period can also be achieved, and the overall shape of
the noise spectrum is similar to that of the quasiparticle source, but the
presence of additional quasiparticle processes enhances the noise amplitude.
