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arXiv:cond-mat/0508423 · Applied Physics B

Production of a chromium Bose–Einstein condensate

Axel Griesmaier, J. Stühler, Tilman Pfau

Published Dec 15, 2005• 41 citations
arXivHTMLPDF
DOI
10.1007/s00340-005-2070-4

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We report on the production of 52Cr^{52}\mathrm{Cr}52Cr Bose-Einstein condensates with an all-optical method. We first load $5\ifmmode\times\else\texttimes\fi{}{10}^{6}$ metastable chromium atoms in a one-dimensional (1D) far-off-resonance optical trap (FORT) from a magneto-optical trap, by combining the use of radio-frequency sweeps and depumping toward the 5S2^{5}S_{2}5S2​ state. The atoms are then pumped to the absolute ground state, and transferred into a crossed FORT in which they are evaporated. The fast loading of the 1D FORT (35ms35\phantom{\rule{0.3em}{0ex}}\mathrm{ms}35ms 1∕e1∕e1∕e time) and the use of relatively fast evaporative ramps allow us to obtain in 20s20\phantom{\rule{0.3em}{0ex}}\mathrm{s}20s about 1500015\phantom{\rule{0.2em}{0ex}}00015000 atoms in an almost pure condensate.
We have observed Bose-Einstein condensation of chromium atoms [1], whose large magnetic dipole moment is unique among all species that have been Bose-condensed so far. The arising magnetic forces are of anisotropic and long-range character and therefore introduce a novel type of interaction in the physics of ultracold quantum gases. In addition, it is expected that the character of the interaction present in a chromium BEC can be varied from mainly contact to purely dipolar utilizing one of the recently observed Feshbach resonances in 52Cr-collisions.