PACS 37.10.Vz -Mechanical effects of light on atoms, molecules, and ions PACS 37.10.Gh -Atom traps and guides PACS 37.90.+j -Other topics in mechanical control of atoms, molecules, and ions Abstract -We report the transport of ultracold atoms with optical tweezers in the non-adiabatic regime, i.e. on a time scale on the order of the oscillation period. We have found a set of discrete transport durations for which the transport is not accompanied by any excitation of the centre of mass of the cloud after the transport. We show that the residual amplitude of oscillation of the dipole mode is given by the Fourier transform of the velocity profile imposed to the trap for the transport. This formalism leads to a simple interpretation of our data and simple methods for optimizing trapped particles displacement in the non-adiabatic regime.

Abstract. -We report the achievement of an optically guided and quasi-monomode atom laser, in all spin projection states (mF = −1, 0 and +1) of F = 1 in rubidium 87. The atom laser source is a Bose-Einstein condensate (BEC) in a crossed dipole trap, purified to any one spin projection state by a spin-distillation process applied during the evaporation to BEC. The atom laser is outcoupled by an inhomogenous magnetic field, applied along the waveguide axis. The mean excitation number in the transverse modes is n = 0.65 ± 0.05 for mF = 0 and n = 0.8 ± 0.3 for the low field seeker mF = −1. Using a simple thermodynamical model, we infer from our data the population in each excited mode.When atoms are coherently extracted from a BoseEinstein condensate (BEC) they form an atom laser, a coherent matter wave in which many atoms occupy a single quantum mode. Atom lasers are orders of magnitude brighter than thermal atom beams, and are first and second order coherent [1,2]. They are of fundamental interest, for example, for studies of atom-light entanglement, quantum correlations of massive particles [3] and quantum transport phenomena [4][5][6][7][8][9][10]. They are of practical interest for matter-wave holography through the engineering of their phase [11], and for atom interferometry because of their sensitivity to inertial fields [12].Many prospects for atom lasers depend upon a high degree of control over the internal and external degrees of freedom and over the flux. The control of the output flux in a pulsed or continuous manner has been investigated using different outcoupling schemes: short and intense radiofrequency pulses [13], gravity induced tunneling [14], optical Raman pulses [15], long and weak radiofrequency fields [16], and by decreasing the trap depth [17].The control of their internal state is intimately related to the outcoupling strategy. Atoms are either outcoupled in the magnetically insensitive (to first order) Zeeman state m F = 0 or another Zeeman state, each offering different advantages. Atom lasers in m F = 0 are ideal for precision measurement [18] because of their low magnetic sensitivity. Atoms in other Zeeman states, however, are ideal for measurements of magnetic fields because of their high magnetic sensitivity [19].The control of the external degrees of freedom has been investigated through the atom laser beam divergence while propagating downwards due to gravity [20,21]. Inhomogeneous magnetic field have been used to realize atom optical elements [22]. Recently, a guided and quasi-continuous atom laser from a magnetically trapped BEC has been reported [23].In this Letter, we report on a new approach to generate guided atom laser. This method can produce an atom laser in any Zeeman state. In addition, our nonstate changing outcoupling scheme leads to an intrinsically good transverse mode-matching, that enables the production of a quasi-monomode guided atom laser. Therefore, we achieve simultaneously a high degree of control of the internal and external degrees of freedom.The atom laser...

We have experimentally demonstrated a high level of control of the mode populations of guided atom lasers (GALs) by showing that the entropy per particle of an optically GAL, and the one of the trapped Bose Einstein condensate (BEC) from which it has been produced are the same. The BEC is prepared in a crossed beam optical dipole trap. We have achieved isentropic outcoupling for both magnetic and optical schemes. We can prepare GAL in a nearly pure monomode regime (85 % in the ground state). Furthermore, optical outcoupling enables the production of spinor guided atom lasers and opens the possibility to tailor their polarization.Isentropic transformations have been used extensively to manipulate classical and degenerate quantum gases. For instance, the reversible formation of a molecular BEC from ultra-cold fermionic atoms having two spin components was performed by adiabatically tuning the interspecies scattering length from positive to negative values [1,2,3,4,5]. Another illustration is the adiabatic change of the shape of the confining trap of cold atoms giving the possibility to change the phase space density in a controlled manner [6,7]. A spectacular demonstration of this idea has been the multiple reversible formation of BEC by adiabatically superimposing an optical dimple trap on a magnetically trapped and pre-cooled sample of atoms [7]. For an ideal transformation, the entropy of the initial cloud should remain constant. However, the limitations of the experimental setup always introduce an extra source of entropy. The challenge for the experimentalists is to minimize this latter contribution.In this experiment, we demonstrate the control and the characterization of a guided atom laser (GAL) [8,9]. The experiments performed to date on the beam quality were addressing the spatial mode of free-falling atom lasers. The importance of the outcoupling scheme or the role played by atom-atom interactions has been extensively studied [10,11,12]. GALs are characterized by the population of the transverse modes of the guide. We have extended the use of isentropic analysis to propagating matter waves in order to relate quantitatively these populations to the characteristics of the BEC from which the GAL originates. This approach turns out to be possible because of both the validity of the local thermal equilibrium and the sufficiently large reduction of the extra entropy production generated by the experimental manipulation. Improvements to the production and characterization of the GAL are crucial for fundamental studies such as quantum transport [13], and applications in metrology [14], among others.The experiment starts by loading 3 × 10 7 87 Rb-atoms in a crossed beam optical dipole trap at a wavelength of 1070 nm from an elongated magneto-optical trap (MOT). To transfer the atoms in the lower hyperfine level F = 1, we align the horizontal arm (1) of the optical trap with the longŷ-axis of the MOT (see inset of Fig. 1.a) and we mask the repump light in the overlapping region between the two traps. The other ar...

We study an experimental setup in which a quantum probe, provided by a quasimonomode guided atom laser, interacts with a static localized attractive potential whose characteristic parameters are tunable. In this system, classical mechanics predicts a transition from regular to chaotic behavior as a result of the coupling between the different degrees of freedom. Our experimental results display a clear signature of this transition. On the basis of extensive numerical simulations, we discuss the quantum versus classical physics predictions in this context. This system opens new possibilities for investigating quantum scattering, provides a new testing ground for classical and quantum chaos, and enables us to revisit the quantum-classical correspondence.