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Optics Letters

Single-beam, ponderomotive-optical trap for free electrons and neutral atoms

J. L. Chaloupka, Y. Fisher, T. J. Kessler, David D. Meyerhofer

Published Jul 1, 1997• 39 citations
Publisher

Abstract

A ponderomotive-optical trap for energetic free electrons has been generated with a single, high-peak-power laser beam. The focal region consists of an intensity minimum at the center of the focus, with increasing intensities in all directions. The focus can be generated with a two-zone binary phase plate, or with a novel, coaxially segmented wave plate. This scheme can also be used to trap neutral atoms.

DOI
10.1364/ol.22.001021

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Quantum Electronics and Laser Science Conference•Jun 25, 2003•1 citation
A ponderomotive-optical trap for energetic free electrons has been generated with a single, high-peak-power laser beam. The focal region consists of an intensity minimum at the center of the focus, with increasing intensities in all directions. The focus can be generated with a two-zone binary phase plate, or with a novel, coaxially segmented wave plate. This scheme can also be used to trap neutral atoms.
Single neutral atom mechanics is controllable by focused, high‐intensity optical vortices. The intensity‐dependent, laser‐driven motion of the atom's active electrons subsumes to a net transfer of the orbital angular momentum of the light to the neutral atom. The ponderomotive force on these electrons translates so into an unbounded or a bounded radial drift of the atom depending on its initial kinetic energy, as set by the temperature. Appropriate combination of laser beams results in sub‐wavelength, dynamical radial traps for tweezing atoms controllably, an effect that can be exploited for atom guiding, structuring, and lithographic applications. image
Rapidly oscillating, inhomogeneous electromagnetic field from laser exert a force that repels charged particles from regions of high light intensity. We propose and analyze a flat-bottomed hollow-beam ponderomotive optical trap for an ultracold neutral plasma (UNP), driven by a high-power CO_{2} laser. Molecular dynamics simulations show that the plasma and Rydberg atoms are effectively trapped within a nearly uniform dark region bounded by repulsive light walls. In contrast to RF traps, flat-bottomed traps yield a small density-weighted mean ponderomotive energy per electron, while the UNP collision frequency is far below the laser frequency, thereby making collisional absorption negligible and does not limit the lifetime of the trap. This approach could enhance antimatter production and storage.
In order to confine any object, it is necessary to exchange kinetic for potential energy in the trapping field, and in neutral atom traps, the potential energy must be stored as internal atomic energy. Thus practical traps for ground-state neutral atoms are necessarily very shallow compared with thermal energy because the energy level shifts that result from conveniently sized fields are typically considerably smaller than k B T , even for T = 1 K. Neutral atom trapping therefore depends on substantial cooling of a thermal atomic sample, and is often connected with the cooling process. In most practical cases, atoms are loaded from magneto-optical traps, where they have been efficiently accumulated and cooled to mK temperatures (see Sec. 20.3), or from optical molasses, where they have been optically cooled to μK temperatures (see Sec. 19.4). The small depth of typical neutral atom traps dictates stringent vacuum requirements, because an atom cannot remain trapped after a collision with a thermal energy background gas molecule. Since these atoms are vulnerable targets for thermal energy background gas, the mean free time between collisions must exceed the desired trapping time. The cross-section for destructive collisions is quite large because even a gentle collision (i.e. large impact parameter) can impart enough energy to eject an atom from a trap. At pressure P sufficiently low to be of practical interest, the trapping time is ~(10 -8 / P ) s, where P is in torr. This chapter begins with a discussion of ordinary, single-center traps, but also considers arrays of traps. Such “optical lattices” are playing an increasingly important role in research in atomic physics, so discussion of their properties is an appropriate part of the education of a student of the subject. Dipole force optical traps Single-beam optical traps for two-level atoms The simplest imaginable optical trap consists of a single, strongly focused Gaussian laser beam (see Fig. 20.1) [214, 215] whose intensity at the focus varies transversely with r as where is the beam waist size. Such a trap has a well-studied and important macroscopic classical analog in a phenomenon called optical tweezers (see App. 1.C) [216–218].
In the field of atom optics, there has been much interests in developing components such as lenses, mirrors, beam splitters and waveguides to manipulate neutral atoms. Especially many clever methods to focus neutral atoms have been developed. The lenses have been constructed using the static electrical and magnetic fields, Fresnel zone plates, and radiation pressure forces. Before the laser cooling and trapping techniques were invented, the electrostatic fields could not be used for manipulating neutral atoms because of its weak interaction energy with atoms. After the cold atoms were available, it has been possible to manipulate atoms with weak electrostatic interaction energy. We developed an atom lens system using electrostatic fields.
Summary form only given. Blue-detuned optical traps confine neutral atoms mostly in the dark, therefore reducing the perturbations induced by the trapping light on the atoms. Recently, traps based on a single laser beam were demonstrated, providing greater experimental simplicity and enabling dynamical changes of the trap geometry and strength. However, all these traps have a large difference in the potential strength in the radial and axial directions, resulting in a very inefficient use of the available laser power, and a poor loading efficiency from the magneto-optical trap. In this work we present a novel optical scheme to generate an optimal trap, which maximizes the trap depth, and greatly reduces the light-induced perturbations to the atoms. This is achieved by surrounding a dark volume with a light envelope having (a) an almost minimal surface area for a given volume, (b) the minimal wall thickness allowed by diffraction, and (c) an almost constant wall height on every point on the envelope. The stiffness of the walls, combined with the large detuning allowed by the efficient distribution of light intensity, yield a very low photon scattering rate for the trapped atoms.