Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Bulletin of the American Physical Society

Ultracold CaF molecules and Rb atoms in the same trap

H. J. Williams, Luke Caldwell, Sarunas Jurgilas, Noah J. Fitch, Jonas Rodewald, Thomas E. Wall, K. N. Jarvis, B. E. Sauer, Edward A. Hinds, Michael R. Tarbutt

Published May 30, 2019• 0 citations
OpenAlex

Related papers

Experiments with ultracold CaF and YbF molecules

Michael R. Tarbutt

Bulletin of the American Physical Society•May 29, 2018•0 citations

Observing Collisions of Two Ultracold Ground State CaF Molecules

Lawrence W. Cheuk

Bulletin of the American Physical Society•Jun 2, 2020•0 citations

Formation and Detection of Ultracold Rb 2 Molecules in a Magnetic Trap

Changhyun Ryu, R. S. Freeland, R. H. Wynar +2 more

APS•May 1, 2001•0 citations

Magnetic Trapping and Collisions of Ultracold Rb 2 Molecules

Changhyun Ryu, R. S. Freeland, W. Jaewoo Shim +1 more

APS•May 1, 2002•0 citations

Progress towards forming ultracold $^{85}$Rb$_2$ molecules in an optical trap

Hyewon Pechkis, Michael Bellos, Jayita RayMajumder +4 more

Bulletin of the American Physical Society•May 30, 2008•0 citations

Modeling sympathetic cooling of molecules by ultracold atoms

Jongseok Lim, Matthew D. Frye, Jeremy M. Hutson +1 more

We model sympathetic cooling of ground-state CaF molecules by ultracold Li and Rb atoms. The molecules are moving in a microwave trap, while the atoms are trapped magnetically. We calculate the differential elastic cross sections for CaF-Li and CaF-Rb collisions, using model Lennard-Jones potentials adjusted to give typical values for the $s$-wave scattering length. Together with trajectory calculations, these differential cross sections are used to simulate the cooling of the molecules, the heating of the atoms, and the loss of atoms from the trap. We show that a hard-sphere collision model based on an energy-dependent momentum transport cross section accurately predicts the molecule cooling rate but underestimates the rates of atom heating and loss. Our simulations suggest that Rb is a more effective coolant than Li for ground-state molecules, and that the cooling dynamics is less sensitive to the exact value of the $s$-wave scattering length when Rb is used. Using realistic experimental parameters, we find that molecules can be sympathetically cooled to $100\phantom{\rule{0.28em}{0ex}}\ensuremath{\mu}\mathrm{K}$ in about 10 s. By applying evaporative cooling to the atoms, the cooling rate can be increased and the final temperature of the molecules can be reduced to $1 \ensuremath{\mu}\mathrm{K}$ within 30 s.

arXiv:1508.03987•Physical Review A•Nov 13, 2015•55 citations
Progress towards forming ultracold 85^{85}85Rb2_22​ molecules in an optical trap
We model sympathetic cooling of ground-state CaF molecules by ultracold Li and Rb atoms. The molecules are moving in a microwave trap, while the atoms are trapped magnetically. We calculate the differential elastic cross sections for CaF-Li and CaF-Rb collisions, using model Lennard-Jones potentials adjusted to give typical values for the sss-wave scattering length. Together with trajectory calculations, these differential cross sections are used to simulate the cooling of the molecules, the heating of the atoms, and the loss of atoms from the trap. We show that a hard-sphere collision model based on an energy-dependent momentum transport cross section accurately predicts the molecule cooling rate but underestimates the rates of atom heating and loss. Our simulations suggest that Rb is a more effective coolant than Li for ground-state molecules, and that the cooling dynamics is less sensitive to the exact value of the sss-wave scattering length when Rb is used. Using realistic experimental parameters, we find that molecules can be sympathetically cooled to $100\phantom{\rule{0.28em}{0ex}}\ensuremath{\mu}\mathrm{K}$ in about 10 s. By applying evaporative cooling to the atoms, the cooling rate can be increased and the final temperature of the molecules can be reduced to $1 \ensuremath{\mu}\mathrm{K}$ within 30 s.