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Physical Review Letters

Supersymmetry and the Binding of a Magnetic Atom to a Filamentary Current

Lene Vestergaard Hau, J. A. Golovchenko, Michael M. Burns

Published Apr 17, 1995• 42 citations
Publisher

Abstract

We suggest the binding of neutral atoms to a current carrying wire through the interaction between the atomic magnetic dipole moment and the wire's magnetic field. The theoretical description is based upon an extension of the concept of supersymmetry to multicomponent wave functions. A solution for spin $\frac{1}{2}$ particles is obtained directly in coordinate space. Spin 1 particles are considered as well. Experimentally, the system should be immediately realizable for 25 mK sodium atoms around a wire with a diameter of $0.5\ensuremath{\mu}\mathrm{m}$ and a current of 400 mA.

DOI
10.1103/physrevlett.74.3138

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We suggest the binding of neutral atoms to a current carrying wire through the interaction between the atomic magnetic dipole moment and the wire's magnetic field. The theoretical description is based upon an extension of the concept of supersymmetry to multicomponent wave functions. A solution for spin 12\frac{1}{2}21​ particles is obtained directly in coordinate space. Spin 1 particles are considered as well. Experimentally, the system should be immediately realizable for 25 mK sodium atoms around a wire with a diameter of 0.5\ensuremathμm0.5\ensuremath{\mu}\mathrm{m}0.5\ensuremathμm and a current of 400 mA.
We consider a waveguide for cold neutral atoms with a magnetic moment proportional to their spin angular momentum. The waveguide consists of a thin wire carrying a constant current. For the spin-1 case, we find bound states for the two-dimensional part of the motion around the wire, and present numerical and approximate analytic results for these bound states. In an experiment, the bound states can decay due to various effects, and we calculate the time scales involved. \textcopyright{} 1996 The American Physical Society.
We suggest a method of binding atoms to ferromagnetic wire through the interaction between the atomic magnetic moment and the magnetic field of the wire. It is shown that the two-dimensional $1/{\ensuremath{\rho}}^{2}$ potential arises between the atom and the wire with magnetization perpendicular to the latter, the three-dimensional 1/r2{1/r}^{2}1/r2 potential arises between the atom and the end of the wire with magnetization parallel to the wire, the two-dimensional $1/\ensuremath{\rho}$ potential arises when magnetization of the wire is parallel to the wire, and the magnitude of magnetization changes linearly along the wire. We also discuss the possibility of experimental realization of binding of sodium atoms to the ferromagnetic iron wire.
We consider the quantized motion of neutral atoms at very low temperature in a two-dimensional magnetic quadrupole structure formed, for example, by four current-carrying wires along the z direction. The magnetic field B\mathbf{B}B in the guide is proportional to the vector $(x,\ensuremath{-}y).$ We show that this field can be used to make a single-mode atomic de Broglie waveguide which has bound states of low angular momentum, even though the field at the center of the guide goes to zero. We investigate the spectrum and decay rate of the transverse modes for spin-1/2 and spin-1 atoms.
The spectrum and the wave function of neutral atoms in the magnetic field of a Kepler-guide are presented by reducing a two-dimensional stationary Schrdinger equation to a one-dimensional hydrogen atom in Rydberg states. In addition, we set the scale for the atomic orbits and binding energy i n the quantum regime, and compare it with the outcome of the experiment. At the same time, we find that reducing the current and radius of the wire properly wil l increase the loading efficiency of the Kepler-guide.