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Physical Review A

Near-field optical potential for a neutral atom

Kiyoshi Kobayashi, Suguru Sangu, Hajime Ito, Motoichi Ohtsu

Published Dec 11, 2000• 88 citations
Publisher

Abstract

We study an effective interaction potential between a neutral atom and a nanometric probe tip in optical near-field systems. The wave-number dependence of the coupling coefficients of exciton polaritons is described with the effective-mass approximation, where massive virtual photons are exchanged between the atom and the probe tip. The near-field optical potential is shown as the sum of the Yukawa functions with several kinds of effective masses or interaction ranges, and is characterized in terms of detuning for the resonance energies of the atom and the probe tip. Consequently, we find that a potential minimum is produced for a blue detuning case. This result indicates that an atom can be trapped in the near-field optical potential well. Furthermore, we numerically investigate deflection and trapping of a single atom by means of optical near fields generated from a nanometric probe tip. The dependence on the probe-tip size, the kinetic energy of the cold atom, and the excitation energies of both probe tip and atom is clarified.

DOI
10.1103/physreva.63.013806

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We study an effective interaction potential between a neutral atom and a nanometric probe tip in optical near-field systems. The wave-number dependence of the coupling coefficients of exciton polaritons is described with the effective-mass approximation, where massive virtual photons are exchanged between the atom and the probe tip. The near-field optical potential is shown as the sum of the Yukawa functions with several kinds of effective masses or interaction ranges, and is characterized in terms of detuning for the resonance energies of the atom and the probe tip. Consequently, we find that a potential minimum is produced for a blue detuning case. This result indicates that an atom can be trapped in the near-field optical potential well. Furthermore, we numerically investigate deflection and trapping of a single atom by means of optical near fields generated from a nanometric probe tip. The dependence on the probe-tip size, the kinetic energy of the cold atom, and the excitation energies of both probe tip and atom is clarified.
Summary form only given. Recently, atom manipulation by using optical near fields has been attracting a lot of interests. Optical near field can be localized in a nanometric region, being free from the diffraction limit in contrast to propagation light. The intensity distribution of optical near field decays rapidly as an exponential-like function. Because such a spatially inhomogeneous light field can affect the resonant force on an atom (the so called dipole force), the optical near field produces the strong dipole force. Using the dipole force of the optical near field, we can expect to manipulate an atom with high spatial accuracy. Moreover, due to the resonant character of the dipole force, we can manipulate an atom species- and state-selectively. The optical near field localized in a nanometric region can be generated on the tip of a sharpened fiber-probe. This kind of fiber probe can be used for deflection of the atomic motion, and then trapping of an atom. To this end, it is very important to fabricate the fiber probe suitable for the atoms used. In this case, we must consider several parameters: a size and a shape of the tip, light intensity, frequency detuning, etc. In order to examine the optimal conditions for the fabrication, we measured and evaluated the optical near-field intensity distribution of the fiber-probe.
We present a new scheme of atom manipulation by means of a sharpened optical fiber with near-field light. In particular, we discuss the feasibility of deflecting and trapping Rb atoms. The optical potential produced by the dipole force is estimated from numerical calculations based on the Yukawa-type intensity distribution. We show that a slow Rb atom can be deflected at a large deflection angle. A static atom trap can be made near the tip of a sharpened fiber. A cold Rb atom is captured at the minimum of the trap potential composed of the repulsive optical potential and the attractive van der Waals potential. A spatial intensity distribution of an optical near-field produced near the tip of a protrusion-type fiber is measured in the fiber-to-probe configuration with a shear-force technique. We also describe an atom funnel to form a cold atomic beam required for the near-field light manipulation.
We describe guiding of neutral atoms through a hollow optical fiber with a micron-sized hollow core. Two-step photoionization experiment shows the frequency dispersion properties of the dipole interaction between an atom and an optical near field. These characteristics are advantageous to species- and state-selective manipulation of atoms. Then we discus a new scheme of atom deposition by means of the guiding technique, including a numerical simulation. We also present two methods for controlling atomic motion using a sharped optical fiber with a nanometric optical n ear field, i.e., atom deflection and atom trap. Deflection angle and trap potential are estimated based on a near-field intensity distribution derived from a Yukawa-type screened potential. The manipulation techniques are useful for precise control of atoms with a spatial accuracy beyond diffraction limit, which will lead to atomic-scale crystal growth.
Summary form only given. The conventional atom-manipulation techniques with propagating light are limited in spatial accuracy by diffraction effects of light waves. In order to overcome the diffraction limit and increase the manipulation accuracy, we can use the optical near field localized in a nanometer region. Such an optical near field is produced by a fiber probe with a nanometric aperture. We consider manipulating atoms by means of the dipole force from the localized optical near field. In this paper we report on the experimental progress toward the realization of atom manipulation with the nanometric fiber probe.
Near-fields around nanophotonic structures and waveguides can be used to optically interface particles ranging from atoms and molecules to microscopic biological and synthetic particles. Due to the strong, non-linear dependence of the near-field coupling strength on the particles' position, a change of the spread of the particles' position will change their mean coupling strength. When the particles are trapped, this position spread depends on their temperature, generally leading to temperature-dependent coupling. Here, we experimentally demonstrate that this effect renders optical probing of trapped particles with near fields an inherently transient process. Specifically, we trap cold atoms in a two-color dipole trap surrounding an optical nanofiber and probe them with the evanescent field of guided, resonant light. The scattering of this probe light heats up the atoms, leading to a decrease of the coupling strength as well as loss of atoms. We observe both effects via a concurrent decrease of the absorption signal. In addition, we demonstrate that the coupling strength can be recovered by cooling the atoms back to their initial temperature. Our findings are relevant for numerous situations where stable coupling of trapped particles to a nanophotonic structure is required.
We theoretically propose blue-detuned optical trapping for neutral atoms via strong near-field interfacing in a plasmonic nanohole array. The optical field at resonance forms a nanoscale-trap potential with an FWHM of 200 nm and about ∼370  nm away from the nanohole; thus, a stable 3D atom trapping independent of the surface potential is demonstrated. The effective trap depth is more than 1 mK when the optical power of trapping light is only about 0.5 mW, while the atom scattering rate is merely about 3.31  s−1, and the trap lifetime is about 800 s. This compact plasmonic structure provides high uniformity of trap depths and a two-layer array of atom nanotraps, which should have important applications in the manipulation of cold atoms and collective resonance fluorescence.