5 research outputs found

    Atom gratings produced by large angle atom beam splitters

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    An asymptotic theory of atom scattering by large amplitude periodic potentials is developed in the Raman-Nath approximation. The atom grating profile arising after scattering is evaluated in the Fresnel zone for triangular, sinusoidal, magneto-optical, and bichromatic field potentials. It is shown that, owing to the scattering in these potentials, two \QTR{em}{groups} of momentum states are produced rather than two distinct momentum components. The corresponding spatial density profile is calculated and found to differ significantly from a pure sinusoid.Comment: 16 pages, 7 figure

    λ8\frac{\lambda}{8}-period optical potentials

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    A Raman configuration of counterpropagating traveling wave fields, one of which is lin⊥linlin\bot lin polarized and the other lin∥linlin\Vert lin polarized, is shown to lead to optical potentials having λ8\frac{\lambda}{8} periodicity. Such optical potentials may be used to construct optical lattices having λ8% \frac{\lambda}{8} periodicity. Using numerical diagonalization, we obtain the optical potentials for 85^{\text{85}}Rb atoms.Comment: 3 pages, 2 figure

    An improved measurement of the electric dipole moment of the neutron

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    International audienceWe describe the status of the new measurement of the neutron electric dipole moment (nEDM) to be performed at the strong source of ultra-cold neutrons at the Paul Scherrer Institut. The experimental technique is based on Ramsey's method of separated oscillatory fields, applied to UCN stored in vacuum in a chamber at room temperature. Our approach is performed in three phases: in phase one, new components have been developed and tested at the Institut Laue-Langevin. Phase two is being performed at PSI, where the apparatus was moved in 2009. Here, together with the optimization of the magnetic environment, the prospective UCN density of not, vert, similar 100 cm-3 should enable an improvement of the currently best limit by a factor of five within two years of data taking. In the third phase, a new spectrometer will then gain another order of magnitude in sensitivity. The improvements will be mainly due to (1) much higher UCN intensity, (2) improved magnetometry and magnetic field control, and (3) a double chamber configuration with opposite electric field directions
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