https://doi.org/10.1007/s100530050061
Bright optical lattices in a longitudinal magnetic field. Experimental study of the oscillating and jumping regimes
Laboratoire Kastler Brossel, Département de Physique de
l'École Normale Supérieure, 24 rue Lhomond, 75231 Paris Cedex 05,
France
Corresponding author: a robi@physique.ens.fr
Received:
9
October
1997
Accepted:
6
November
1997
Published online: 15 January 1998
All the bright optical lattices studied so far have been designed to obtain
a circularly polarized light at the bottom of the optical potential wells.
This condition minimizes the departure rate of the atoms from the
fundamental adiabatic surface and permits an oscillating regime in a large
range of parameters. We present here an experimental study of cesium atoms
in a three-dimensional optical lattice, where the light is linearly
polarized at the bottom of the potential wells. Temperature measurements and
pump-probe spectroscopy give similar results for this lattice and for the
conventional lin lin lattice (which have circular polarizations at
the bottom of the wells) despite the fact that one lattice operates in the
jumping regime and the other in the oscillating regime. We study the
behaviour of the two types of lattices in a longitudinal magnetic field,
with particular emphasis on the zero field and strong field regimes. The
strong field situation is very simple because the eigenstates are then
almost pure Zeeman substates and the adiabatic and diabatic potential
surfaces are identical. The comparison between the zero-field and the
high-field situations shows that the diabatic potentials are more
appropriate to account for experimental observations in the novel lattice.
PACS: 32.80.Pj – Optical cooling of atoms; trapping / 32.60.+i – Zeeman and Stark effects
© EDP Sciences, Società Italiana di Fisica, Springer-Verlag, 1998