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Optics Express

Optics Express

  • Editor: Michael Duncan
  • Vol. 13, Iss. 8 — Apr. 18, 2005
  • pp: 2843–2851

A high frequency optical trap for atoms using Hermite-Gaussian beams

T. P. Meyrath, F. Schreck, J. L. Hanssen, C. -S. Chuu, and M. G. Raizen  »View Author Affiliations


Optics Express, Vol. 13, Issue 8, pp. 2843-2851 (2005)
http://dx.doi.org/10.1364/OPEX.13.002843


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Abstract

We present an experimental method to create a single high frequency optical trap for atoms based on an elongated Hermite-Gaussian TEM01 mode beam. This trap results in confinement strength similar to that which may be obtained in an optical lattice. We discuss an optical setup to produce the trapping beam and then detail a method to load a Bose-Einstein Condensate (BEC) into a TEM01 trap. Using this method, we have succeeded in producing individual highly confined lower dimensional condensates.

© 2005 Optical Society of America

OCIS Codes
(020.0020) Atomic and molecular physics : Atomic and molecular physics
(020.7010) Atomic and molecular physics : Laser trapping

ToC Category:
Research Papers

History
Original Manuscript: February 28, 2005
Revised Manuscript: March 30, 2005
Published: April 18, 2005

Citation
T. Meyrath, F. Schreck, J. Hanssen, C. Chuu, and M. Raizen, "A high frequency optical trap for atoms using Hermite-Gaussian beams," Opt. Express 13, 2843-2851 (2005)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-13-8-2843


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References

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  23. We use values for the D2 line of rubidium 87: Is ~ 1.67mW/cm2, ? _= 2? ? 6.065MHz, w0 _= 2? ? 384.23THz, and m _= 1.443�10-25 kg. In Eq. (3), it is important not to use the common rotating wave approximation (which is to assume |w0 -w|�w0 +w and neglect the second term in parenthesis) because the detuning is too far for this to be valid. This is a larger effect than explicitly including the D1 line which is typically done for nearer detunings.
  24. This is a gradium index lens with f /# = 2.2.
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