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Physical Review Letters

Stopping Atoms with Laser Light

John V. Prodan, Alan L. Migdall, William D. Phillips, Ivan So, Harold J. Metcalf, Jean Dalibard

Published Mar 11, 1985• 185 citations
Publisher

Abstract

We have produced a sample of free sodium atoms at rest in the laboratory by decelerating atoms in an atomic beam using momentum transfer from a counterpropagating, resonant laser beam. These atoms have a density of about ${10}^{5}$ ${\mathrm{cm}}^{\ensuremath{-}3}$ and a velocity spread of about 15 m/s full width at half maximum corresponding to a kinetic temperature less than 100 mK.

DOI
10.1103/physrevlett.54.992

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We have produced a sample of free sodium atoms at rest in the laboratory by decelerating atoms in an atomic beam using momentum transfer from a counterpropagating, resonant laser beam. These atoms have a density of about 105{10}^{5}105 cm\ensuremath−3{\mathrm{cm}}^{\ensuremath{-}3}cm\ensuremath−3 and a velocity spread of about 15 m/s full width at half maximum corresponding to a kinetic temperature less than 100 mK.
A collection of stationary or nearly stationary atoms would be an ideal sample on which to perform high-resolution spectroscopy. Spectral width, shifts, and distortions that are due to second-order-Doppler and transit-time effects, which now limit high-resolution Doppler-free spectroscopies, would be virtually eliminated. Such low-energy atoms would also be useful for loading into the shallow optical1,2 or magnetic3,4 traps that have been proposed. By irradiating an atomic beam with a near-resonant counter- propagating laser, we have produced such a sample of atoms. The average velocity of the atoms is nearly zero, and the spread in velocities is equivalent to that of a gas at a temperature of about 1 K.
Atomic-beam sodium atoms were slowed to zero or negative velocities by counterpropagating laser radiation which was frequency chirped with precise electro-optic modulation techniques. The resulting "gas cloud" had a temperature below 50 mK and a density above 106{10}^{6}106 atoms/cm3{\mathrm{cm}}^{3}cm3. We mention future possibilities in atom slowing, deflection, and storage.
A thermal atomic Na beam is opposed by a resonantly tuned laser beam. The radiation pressure decelerates and compresses the thermal velocity distribution, bringing the average velocity to zero and reducing the width from ~1000 m/s to a few tens of m/s or less.1 The density of stopped atoms is > 106/cm3 within a bandwidth of a few m/ s. These densities and velocities are suitable for trapping by a number of proposed optical and magnetic traps. Using these stopped atoms, we have demonstrated the first electromagnetic trapping of neutral atoms. The trap, a magnetic quadrupole formed by two separated, coaxial, opposed current loops, confines the atoms by virtue of the force exerted on the Na magnetic dipole moment by the inhomogeneous magnetic field. The time constant for exponential decay of the atomic population in the trap is 0.83(7) s and is limited mainly by collisions with fast background gas atoms. The maximum velocity of atoms contained in the trap is 3.5 m/s, corresponding to a maximum energy of 17 mK.