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Eur. Phys. J. D 33, 173-179 (2005)
DOI: 10.1140/epjd/e2005-00064-2
Noise sensitivity of an atomic velocity sensor
Theoretical and experimental treatment
P. Cladé1, S. Guellati-Khélifa2, C. Schwob1, F. Nez1, L. Julien1 and F. Biraben11 Laboratoire Kastler Brossel, École Normale Supérieure, CNRS, UPMC, 4 place Jussieu, 75252 Paris Cedex 05, France
2 CNAM-INM, Conservatoire National des Arts et Métiers, 292 rue Saint Martin, 75141 Paris Cedex 03, France
guellati@spectro.jussieu.fr
(Received 26 October 2004 / Received in final form 7 January 2005 / Published online 3 May 2005)
Abstract
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
-pulses: the first pulse transfers atoms from the hyperfine state
,
to
,
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
,
. 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
-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.
32.80.Pj - Optical cooling of atoms; trapping.
06.30.Gv - Velocity, acceleration and rotation.
© EDP Sciences, Società Italiana di Fisica, Springer-Verlag 2005
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