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AIP conference proceedings

Bouncing atoms: A coherent nano-probe

Nathalie Westbrook

Published Jan 1, 2001• 0 citations
Publisher

Abstract

We describe experiments with atoms reflecting from atomic mirrors. We show that the Zeeman structure of the atoms permits the realization of an nano scale interferometer which can be used to probe the van der Waals interaction between an atom an a dielectric surface. We also discuss preliminary results on an experiment to observe sub-angstrom surface roughness using stimulated Raman transitions to achieve velocity selection of 0.3 times the single photon recoil velocity. This resolution corresponds to a 1.5 mrad maximum deviation in the effective reflecting surface.

DOI
10.1063/1.1354363

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We describe experiments with atoms reflecting from atomic mirrors. We show that the Zeeman structure of the atoms permits the realization of an nano scale interferometer which can be used to probe the van der Waals interaction between an atom an a dielectric surface. We also discuss preliminary results on an experiment to observe sub-angstrom surface roughness using stimulated Raman transitions to achieve velocity selection of 0.3 times the single photon recoil velocity. This resolution corresponds to a 1.5 mrad maximum deviation in the effective reflecting surface.
After a brief introduction to the field of atom optics and to atomic mirrors, we present experimental results obtained in our group during the last two years while studying the reflection of rubidium atoms by an evanescent wave. These involve the first measurement of the van der Waals force between an atom in its ground state and a dielectric wall, as well as the demonstration of a reflection grating for atoms at normal incidence. We also consider the influence of quantum reflection and tunnelling phenomena. Further studies using the atomic mirror as a probe of the van der Waals interaction, and of very small surface roughness are briefly discussed.
Summary form only given. Evanescent wave atomic mirrors have been shown to be very sensitive to the surface roughness of the glass substrate on which the evanescent wave is formed. Non-specular reflection of slow atoms at normal incidence has been observed for surface roughness as low as 0.1 nm. We interpret this behaviour in terms of diffraction of the atomic De Broglie wave on the modulated potential created by the interference of the evanescent wave with light scattered by the rough surface. However these experiments could not separate the specular peak of reflected atoms from the diffuse part. We have developed a new method to measure the velocity distribution of the atoms after the bounce with a much better resolution, using Raman transitions. Two phase locked counterpropagating laser beams induce a Raman transition between the ground state hyperfine levels of the /sup 85/Rb atoms falling from a magneto-optical trap. The resonance condition is only fulfilled for atoms with a transverse velocity controlled by the interaction time between the atoms and the beams. These velocity selected atoms bounce on the mirror and their velocity distribution after reflection can be measured using the same Raman beams, by scanning their difference in frequency.
The atomic response to resonant light irradiation near vapor-dielectric interfaces is monitored via high-resolution reflection spectroscopy. One demonstrates that this Doppler-free spectroscopic technique yields a novel probe of atomic dynamics and QED atom-surface long- range interaction. It provides for the first time a spectral evidence of van der Waals attraction, and the method is intrinsically applicable to the observation of surface interaction exerted on excited atoms. Effects related with atomic excitation level, nature of the dielectrics, and atomic collisions are discussed.
We analyze the possibilities of approaching atom-surface interactions through their contribution to the atomic matter de Broglie wave phase, in an interferometer based on an evanescent light atomic mirror. The surface interactions produce an additional phase shift that is evaluated to a few times \ensuremath{\pi} for a neon atom in a metastable state. We propose and investigate an experimental procedure that uses the principles of polarization (for instance, Stern-Gerlach) interferometers in order to monitor these long-range interactions (van der Waals, Casimir-Polder, etc.) between a ground-state or metastable-state atom and either a metallic or a dielectric surface. Our approach gives access to the differential phase shift between Zeeman sublevels, and should then be sensitive to an eventual anisotropy of the atom-surface interaction.
The paper presents an experiment based on an efficient coupling between atomic Zeeman states (for atoms with internal angular momentum) allowed by the quadrupolar component of the surface- induced van der Waals (vdW) interaction. This exo-energetic "vdW - Zeeman" transition provides a tuneable (magnetic field intensity dependent) beam splitter that was theoretically illustrated by the simplest possible interferometer: an atomic counterpart of Fresnel biprism. The velocity - adjustable atomic beam is here coming across two opposite surfaces (single slit of a nano-grating). For a transverse coherent radius large enough, the atom wave packet is strongly inelastically diffracted by the two opposite surfaces at some distances from the slit to yield non localised interference fringes. The calculation has been done for Ar metastable atoms with a grating of 100 nm period and different velocities of the atoms (560 to 10 m/s). Via the interference pattern (Schlieren image), this device should give access to such novel information as the oscillating part of the complex vdW - interaction transition amplitude. This simplest configuration is not sensitive to inertial effect. As a next step, a loop - closing transmission grating was added to realize a new type of compact interferometer.
The authors propose a novel experiment based on atoms trapped close to a macroscopic surface, to study the interactions between the atoms and the surface at very small separations (0.6 to 10 mum). In this range the dominant potential is the QED interaction (Casimir-Polder and Van der Waals) between the surface and the atom. Additionally, several theoretical models suggest the possibility of Yukawa type potentials with sub-mm range, arising from new physics related to gravity. The paper proposes a set-up very similar to neutral atom optical lattice clocks, but with the atoms trapped in lattice sites close to the reflecting mirror. A sequence of pulses of the probe laser at different frequencies is then used to create an interferometer with a coherent superposition between atomic states at different distances from the mirror (in different lattice sites). Assuming atom interferometry state of the art measurement of the phase difference and a duration of the superposition of about 0.1s we expect to be able to measure the potential difference between separated states with an uncertainty of about 10-4Hz. A preliminary analysis of systematic effects for different atoms (Sr, Yb, Rb, Cs) indicates no fundamentally limiting effect at the same level of uncertainty, but does influence the choice of atom and isotope. Based on those estimates, we expect that such an experiment would improve the best existing measurements of the atom-wall QED interaction by <2 orders of magnitude, whilst gaining up to 4 orders of magnitude on the best present limits on new interactions in the range between 100 nm and 100mum