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Physical Review A

Magnetic trapping of an atomic ^5^5Mn-^5^2Cr mixture (3 pages)

Scott V. Nguyen, Joel S. Helton

Published Jan 1, 2005• 0 citations
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Related papers

Magnetic trapping of a cold Rb--Cs atomic mixture

P Tierney and S L Cornish M L Harris

Please see PDF file for details.

Journal of Physics B Atomic Molecular and Optical Physics•Feb 26, 2008•3 citations

Magnetic trapping of a cold Rb–Cs atomic mixture

Margaret Harris, Patrick Tierney, Simon L. Cornish

We present an apparatus for the study of an ultracold gaseous atomic mixture of 133Cs and 87Rb. The mixture is prepared using a double magneto-optical trap (MOT) system in which a two-species pyramid MOT acts as a source of cold atoms for a `science' MOT. Measurements of the interspecies trap loss rate coefficients beta_RbCs and beta_CsRb in the science MOT are reported. After the initial MOT phase, atoms in the mixture are optically pumped into the magnetically trappable |F=3,m_F=-3> and |F=1,m_F=-1> states of Cs and Rb (respectively) and loaded into an Ioffe-Pritchard magnetic trap. We demonstrate a novel technique for limiting the interspecies loss rate in the science MOT by spatially separating the two trapped atom clouds, which greatly enhances the number of atoms which can be loaded into the magnetic trap.

arXiv:0711.2598•Journal of Physics B Atomic Molecular and Optical Physics•Jan 22, 2008•25 citations

Magnetic Trapping of Neutral Atoms

Harold J. Metcalf, P. van der Straten

Graduate texts in contemporary physics•Jan 1, 1999•3 citations

Optimal cooling strategies for magnetically trapped atomic Fermi-Bose mixtures

Michael Brown-Hayes, Roberto Onofrio

We discuss cooling efficiency for different-species Fermi-Bose mixtures in magnetic traps. A better heat capacity matching between the two atomic species is achieved by a proper choice of the Bose cooler and the magnetically trappable hyperfine states of the mixture. When a partial spatial overlap between the two species is also taken into account, the deepest Fermi degeneracy is obtained for an optimal value of the trapping frequency ratio between the two species. This can be achieved by assisting the magnetic trap with a deconfining light beam, as shown in the case of fermionic $^{6}\mathrm{Li}$ mixed with $^{23}\mathrm{Na}$, $^{87}\mathrm{Rb}$, and $^{133}\mathrm{Cs}$, with optimal conditions found for the not yet explored $^{6}\mathrm{Li}\penalty1000-\hskip0pt^{87}\mathrm{Rb}$ mixture.

arXiv:cond-mat/0411560•Physical Review A•Dec 15, 2004•16 citations

The Hydrodynamic Equations of Superfluid Mixtures in Magnetic Traps

Tin-Lun Ho, Vivek B. Shenoy

The hydrodynamics equations of binary mixtures of Bose gases, Fermi gases, and mixtures of Bose and Fermi gases in the presence of external potentials are derived. These equations can be applied to current experiments on mixtures of atomic gases confined in magnetic traps.

arXiv:cond-mat/9710275•Oct 24, 1997•1 citation

Magnetic trapping of atomic nitrogen and cotrapping of NH

Matthew T. Hummon

Bulletin of the American Physical Society•Jan 1, 2010•0 citations
We present an apparatus for the study of an ultracold gaseous atomic mixture of 133Cs and 87Rb. The mixture is prepared using a double magneto-optical trap (MOT) system in which a two-species pyramid MOT acts as a source of cold atoms for a `science' MOT. Measurements of the interspecies trap loss rate coefficients beta_RbCs and beta_CsRb in the science MOT are reported. After the initial MOT phase, atoms in the mixture are optically pumped into the magnetically trappable |F=3,m_F=-3> and |F=1,m_F=-1> states of Cs and Rb (respectively) and loaded into an Ioffe-Pritchard magnetic trap. We demonstrate a novel technique for limiting the interspecies loss rate in the science MOT by spatially separating the two trapped atom clouds, which greatly enhances the number of atoms which can be loaded into the magnetic trap.
We discuss cooling efficiency for different-species Fermi-Bose mixtures in magnetic traps. A better heat capacity matching between the two atomic species is achieved by a proper choice of the Bose cooler and the magnetically trappable hyperfine states of the mixture. When a partial spatial overlap between the two species is also taken into account, the deepest Fermi degeneracy is obtained for an optimal value of the trapping frequency ratio between the two species. This can be achieved by assisting the magnetic trap with a deconfining light beam, as shown in the case of fermionic 6Li^{6}\mathrm{Li}6Li mixed with 23Na^{23}\mathrm{Na}23Na, 87Rb^{87}\mathrm{Rb}87Rb, and 133Cs^{133}\mathrm{Cs}133Cs, with optimal conditions found for the not yet explored $^{6}\mathrm{Li}\penalty1000-\hskip0pt^{87}\mathrm{Rb}$ mixture.