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arXiv:physics/0003091 · Optics Letters

Waveguide atom beam splitter for laser-cooled neutral atoms

Dirk Müller, Eric Cornell, M. Prevedelli, Peter D. D. Schwindt, Alex A. Zozulya, Dana Z. Anderson

Published Sep 15, 2000• 62 citations
arXivHTMLPDF

Abstract

A laser-cooled neutral-atom beam from a low-velocity intense source is split into two beams while it is guided by a magnetic-field potential. We generate our multimode beam-splitter potential with two current-carrying wires upon a glass substrate combined with an external transverse bias field. The atoms are guided around curves and a beam-splitter region within a 10-cm guide length. We achieve a maximum integrated flux of 1.5x10(5)atoms/s with a current density of 5x10(4)amp/cm (2) in the 100-microm -diameter wires. The initial beam can be split into two beams with a 50/50 splitting ratio.

DOI
10.1364/ol.25.001382

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Physics Today•Feb 1, 2001•0 citations
A laser-cooled neutral-atom beam from a low-velocity intense source is split into two beams while it is guided by a magnetic-field potential. We generate our multimode beam-splitter potential with two current-carrying wires upon a glass substrate combined with an external transverse bias field. The atoms are guided around curves and a beam-splitter region within a 10-cm guide length. We achieve a maximum integrated flux of 1.5x10(5)atoms/s with a current density of 5x10(4)amp/cm (2) in the 100-microm -diameter wires. The initial beam can be split into two beams with a 50/50 splitting ratio.
Laser-cooled neutral atoms from a low-velocity atomic source are guided via a magnetic field generated between two parallel wires on a glass substrate. The atoms bend around three curves, each with a 15-cm radius of curvature, while traveling along a 10-cm-long track. A maximum flux of $2\ifmmode\times\else\texttimes\fi{}{10}^{6}\phantom{\rule{0ex}{0ex}}\mathrm{atoms}/\mathrm{sec}$ is achieved with a current density of $3\ifmmode\times\else\texttimes\fi{}{10}^{4}\phantom{\rule{0ex}{0ex}}\mathrm{A}/{\mathrm{cm}}^{2}$ in the $100\ifmmode\times\else\texttimes\fi{}100$- $\ensuremath{\mu}\mathrm{m}$-cross-section wires. The kinetic energy of the guided atoms in one transverse dimension is measured to be $42\ensuremath{\mu}\mathrm{K}$.
A novel controllable cold neutral atom guiding scheme based on parallel current-carrying wires and bias magnetic field is proposed.Magnetic field distribution in cross-section at different transverse bias field B_(bx) is calculated.The centre of magnetic traps is discussed.Single-channel and double-channel magnetic guiding can be realized.Based on this scheme,an atom beam splitter,which has adjustable splitting ratio, is designed by adding a longitudinal magnetic bias field B_(by).The transverse distribution of magnetic trap is calculated,and the magnetic contour plane of the splitter is shown.By using the classical Monte-Carlo method,the splitting process is simulated,and this scheme is validated by the simulation results.Splitting ratio between left and right guide changes from 0.9/0.1 to 0.1/0.9 when longitudinal magnetic bias field B_(by) changes from -0.005 G to 0.005 G.
We propose a novel atomic beamsplitter for guided atoms composed of a U-shaped current carrying conductor and an additional bias magnetic field, and study the dynamic process of atomic beam splitting in the beamsplitter by Monte Carlo simulations. Our study shows that the splitting ratio of the beamsplitter can be continuously adjusted from 0 to 1 by changing the additional bias field. In addition, the transverse temperature of guided atoms at the outlets of the beamsplitter are also estimated and explained qualitatively.
Summary form only given. Just as optical waveguides play a central role in many aspects of modern optics, from communications to integrated optics, atom waveguides are likely to be an enabling technology for future atom-optics-based science. In particular, well-characterized atom waveguides may make possible inertial and rotation measurements of exquisite sensitivity via large-enclosed-area atom interferometers. The first guides for atoms were based on optical forces, where hollow glass fibers guide light, and the light in turn guides atoms. In this paper we have guided neutral atoms using photolithographically patterned current-carrying wires in two different configurations.
Have been demonstrated: a beam splitter, a conveyor belt, and a switch. Just as electrons drive electronics and photons drive photonics, many researchers hope that cold, neutral atoms will drive a future “atomtronics.” To process information, atoms will need to be manipulated on or near an “atom chip” using atom-based analogs of mirrors, lenses, waveguides, gratings, and other devices. The new devices reported here all exploit the interaction between a neutral atom’s magnetic moment and an external magnetic field with a gradient strong enough to create microscopic potentials. Jörg Schmiedmayer of the University of Heidelberg and his colleagues have designed a beam splitter for guided atoms, using a Y-shaped current-carrying wire nanofabricated on a surface. Depending on how current is sent through the Y, atoms can be directed to the output arms with any desired ratio. A group at the Max Planck Institute for Quantum Optics in Munich has been able to confine atom clouds in separate potential wells and transport them with 800-nm precision near a surface having time-dependent currents in a lithographically patterned conductor. The researchers have used their “magnetic conveyor belt” to merge separate clouds; their evidence shows that the process is adiabatic and can be reversed to coherently split wavepackets. Also using lithography, and following their own beam splitter, a group at the University of Colorado and NIST in Boulder has devised a switch that can direct a guided beam of neutral atoms to either of two output ports separated by 8 mm. Both the incoming and outgoing atoms are guided between two parallel wires having current flowing in the same direction. In the switch region, the atoms are guided alongside two wires with oppositely flowing current. (D. Cassettari et al., Phys. Rev. Lett. 85, 5483, 2000 http://dx.doi.org/10.1103/PhysRevLett.85.5483 . W. Hänsel et al., Phys. Rev. Lett. 86, 608, 2001 http://dx.doi.org/10.1103/PhysRevLett.86.608 . D. Müller et al., Opt. Lett. 25, 1382, 2000 http://dx.doi.org/10.1364/OL.25.001382 ; D. Müller et al., Phys. Rev. A , in press.)© 2001 American Institute of Physics.