Older Highlights

observation of p-wave contacts

Observation of two new physical quantities, the p-wave contacts, via time-resolved spectroscopy. We study how correlations in our system develop after "quenching" the atoms into a state with near resonant p-wave interactions. The contacts appear as a unique frequency scaling in the spectra. These observations suggest a new way to characterize any gas with short-ranged p-wave interactions.

Luciuk et al., Nat. Phys. (2016)
Yu et al., PRL 115, 135304 (2015)

Observation of the Leggett-Rice Effect in a unitary Fermi Gas

Our paper on spin transport in a strongly interacting Fermi gas investigates how transverse spin currents are twisted by the spins that are responsible for their generation (a). We measure the Leggett-Rice parameter gamma that characterizes this precession (b), as well as the transverse spin diffusivity (c), as a function of temperature and interaction parameter kFa.

Trotzky et al., PRL 114, 015301 (2015)

Planckian transport bound in spin diffusivity

Spin Transport at the Planck Limit in a unitary Fermi gas. Using a spin echo, we measure the transverse demagnetization dynamics of a Fermi gas at a scattering resonance. We find that the magnetization dynamics are diffusive, described with a transverse spin diffusion constant Ds, whose value saturates to hbar/m at low tempeature.

Bardon et al., Science 344, 722 (2014)

Quantum transport across a barrier

The frequency with which an ultracold rubidium superfluid oscillates between the two sides of a barrier, as a function of barrier height. The white dots are measured frequencies, and the black lines are ab-initio theory calculations. JM is the two-mode Josephson Model, HD is a hydrodynamic model, and GPE is the Gross Pitaevskii equation. The barrier height is shown divided by the chemical potential of the condensate.

LeBlanc et al, PRL 106, 025302 (2011)

a degenerate Fermi gas

The pictures above are absorption images of Potassium 40 atoms at several temperatures. As the temperature is reduced, fermions occupy lower and lower energy levels in the trap, and the cloud sized is reduced. However, at temperatures below the Fermi temperature, lower energy states are completely occupied, and eventually filled up to the Fermi energy (indicted by the red circle above). This quantum degenerate state was acheived by sympathetic cooling in the microfabricated magnetic trap using a reservoir of Rubidium 87 atoms

August 2005

Bose-Einstein condensation

Images of a cloud of Rubidium 87 atoms above and below the Bose-Einstein phase transition. left: 120,000 thermal atoms at 960nK; center: 70,000 atoms at 360nK, just below Tc; right: a nearly pure Bose-Einstein condensate of 45,000 atoms. Images are roughly 1mm by 1mm, and taken after 10ms of free expansion. Height in these plots corresponds to observed atomic density.

April 2005

first MOT!

Image of our first magneto optical trap! Long live the lab!

December 2003