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Bose-Einstein condensates and degenerate Fermi gases

Cameron S. Fletcher

Published Jan 1, 2005• 0 citations
Publisher
DOI
10.25911/5d6511db137ea

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We report on an improved scheme to generate Bose-Einstein condensates (BECs) and degenerate Fermi gases of strontium. This scheme allows us to create quantum gases with higher atom number, a shorter time of the experimental cycle, or deeper quantum degeneracy than before. We create a BEC of 84{}^{84}84Sr exceeding 107{10}^{7}107 atoms, which is a 30-fold improvement over previously reported experiments. We increase the atom number of 86{}^{86}86Sr BECs to $2.5\ifmmode\times\else\texttimes\fi{}{10}^{4}$ (a fivefold improvement) and refine the generation of attractively interacting 88{}^{88}88Sr BECs. We present a scheme to generate 84{}^{84}84Sr BECs with a cycle time of 2 s. We create deeply degenerate 87{}^{87}87Sr Fermi gases with T/TFT/{T}_{F}T/TF​ as low as 0.10(1), where the number of populated nuclear spin states can be set to any value between one and ten. Furthermore, we report on a total of five different double-degenerate Bose-Bose and Bose-Fermi mixtures. These studies prepare an excellent starting point for applications of strontium quantum gases anticipated in the near future.
After a brief historical introduction to Bose-Einstein condensation and Fermi degeneracy, we discuss theoretical results we have recentely obtained for trapped degenerate quantum gases by means of a thermal field theory approach. In particular, by using Gross-Pitaevskii and Bogoliubov-Popov equations, we consider thermodynamical properties of two Bosonic systems: a gas of Lithium atoms and a gas of Hydrogen atoms. Finally, we investigate finite-temperature density profiles of a dilute Fermi gas of Potassium atoms confined in a harmonic potential.