  We use Bloch oscillations to accelerate coherently Rubidium atoms. The
variation of the velocity induced by this acceleration is an integer number
times the recoil velocity due to the absorption of one photon. The measurement
of the velocity variation is achieved using two velocity selective Raman
pi-pulses: the first pulse transfers atoms from the hyperfine state 5S1/2 |F=2,
mF=0> to 5S1/2, |F=1, mF = 0> into a narrow velocity class. After the
acceleration of this selected atomic slice, we apply the second Raman pulse to
bring the resonant atoms back to the initial state 5S1/2, |F=2, mF = 0>. The
populations in (F=1 and F=2) are measured separately by using a one-dimensional
time-of-flight technique. To plot the final velocity distribution we repeat
this procedure by scanning the Raman beam frequency of the second pulse. This
two pi-pulses system constitutes then a velocity sensor. Any noise in the
relative phase shift of the Raman beams induces an error in the measured
velocity. In this paper we present a theoretical and an experimental analysis
of this velocity sensor, which take into account the phase fluctuations during
the Raman pulses.
