Study of coherence properties of Bose-Einstein condensate in an wave-guide Michelson interferometer

A Michelson interferometer using Bose-Einstein condensates is demonstrated with coherence times of up to $44\phantom{\rule{0.3em}{0ex}}\mathrm{ms}$ and arm separations up to $180\phantom{\rule{0.3em}{0ex}}\mathrm{\ensuremath{\mu}}\mathrm{m}$. This arm separation is larger than that observed for any previous atom interferometer. The device uses atoms weakly confined in a magnetic guide and the atomic motion is controlled using Bragg interactions with an off-resonant standing-wave laser beam.A Michelson interferometer using Bose-Einstein condensates is demonstrated with coherence times of up to $44\phantom{\rule{0.3em}{0ex}}\mathrm{ms}$ and arm separations up to $180\phantom{\rule{0.3em}{0ex}}\mathrm{\ensuremath{\mu}}\mathrm{m}$. This arm separation is larger than that observed for any previous atom interferometer. The device uses atoms weakly confined in a magnetic guide and the atomic motion is controlled using Bragg interactions with an off-resonant standing-wave laser beam.

arXiv:cond-mat/0603772Physical Review ASep 11, 200685 citations

Coherence properties of Bose-Einstein condensates

WORLD SCIENTIFIC eBooksSep 1, 20111 citation

Atom Michelson Interferometer on a Chip Using a Bose-Einstein Condensate

Ying-Ju Wang, Dana Z. Anderson, Victor M. Bright +7 more

An atom Michelson interferometer is implemented on an "atom chip." The chip uses lithographically patterned conductors and external magnetic fields to produce and guide a Bose-Einstein condensate. Splitting, reflecting, and recombining of condensate atoms are achieved by a standing-wave light field having a wave vector aligned along the atom waveguide. A differential phase shift between the two arms of the interferometer is introduced by either a magnetic-field gradient or with an initial condensate velocity. Interference contrast is still observable at 20% with an atom propagation time of 10 ms.An atom Michelson interferometer is implemented on an "atom chip." The chip uses lithographically patterned conductors and external magnetic fields to produce and guide a Bose-Einstein condensate. Splitting, reflecting, and recombining of condensate atoms are achieved by a standing-wave light field having a wave vector aligned along the atom waveguide. A differential phase shift between the two arms of the interferometer is introduced by either a magnetic-field gradient or with an initial condensate velocity. Interference contrast is still observable at 20% with an atom propagation time of 10 ms.

arXiv:cond-mat/0407689Physical Review LettersMar 11, 2005385 citations

Decoherence effects in Bose–Einstein condensate interferometry I. General theory

Bryan J. Dalton

arXiv:1007.0100Annals of PhysicsNov 10, 20105 citations

A Michelson interferometer using Bose-Einstein condensates is demonstrated with coherence times of up to

44\phantom{\rule{0.3em}{0ex}}\mathrm{ms}

and arm separations up to $180\phantom{\rule{0.3em}{0ex}}\mathrm{\ensuremath{\mu}}\mathrm{m}$. This arm separation is larger than that observed for any previous atom interferometer. The device uses atoms weakly confined in a magnetic guide and the atomic motion is controlled using Bragg interactions with an off-resonant standing-wave laser beam.