2DMOT Base pressure

No leaks during a bakeout of up to 450 C, the base pressure with just the ion pumps is in the low 10-11 torr range, and the residual gas analyzer shows nothing but a little hydrogen left. I think we can call this a success.Base PressureThe outside of the chamber isn’t quite as aesthetically pleasing as it was, but the inside is very, very clean, and ready for installation of windows, and the lithium vapor sources. Next: move it to the main table and get ready to attach the main chamber.

 

We have a new 2DMOT chamber

We’ve made some major progress this week with the assembly, pump-down, and bake out of the new 2DMOT chamber for 6Li and 7Li.

There are no indications of leaks so far with the blanked-off chamber baking at 250 C.  If things still look good tomorrow, we’ll we’ll heat most of the chamber (especially the appendages that will house the lithium vapor sources) to >400 C to drive hydrogen out of the chamber walls.

Temperature Stability Issues Resolved

The temperature in the central part of our lab is now stable to within ±0.05 C.Temp. 09_25_2014 thru 10_02_2014

It’s been a complicated and needlesly drawn out technical battle to get to this point. For comparison, here’s a plot of what the HVAC system was doing to the lab temperature shortly after it was commissioned, over a year ago. (Emerson/Liebert, you are permanently blacklisted as far as we’re concerned)

TempHumid Sept 16-24

Needless to say it wasn’t easy to make progress getting the lasers stabilized in an environment like that. Now that we’ve got a proper laboratory to work in, we should be able to make a lot more progress in the next 12 months!

Publication in PRA

Phys. Rev. A 88, 063633 (2013)

Threshold for creating excitations in a stirred superfluid ring

K. C. Wright, R. B. Blakestad, C. J. Lobb, W. D. Phillips, and G. K. Campbell

Abstract: We have measured the threshold for creating long-lived excitations when a toroidal Bose-Einstein condensate is stirred by a rotating (optical) barrier of variable height. When the barrier height is on the order of or greater than half of the chemical potential, the critical barrier velocity at which we observe a change in the circulation state is much less than the speed for sound to propagate around the ring. In this regime we primarily observe discrete jumps (phase slips) from the noncirculating initial state to a simple, well-defined, persistent current state. For lower barrier heights, the critical barrier velocity at which we observe a change in the circulation state is higher, and approaches the effective sound speed for vanishing barrier height. The response of the condensate in this small-barrier regime is more complex, with vortex cores appearing in the bulk of the condensate. We find that the variation of the excitation threshold with barrier height is in qualitative agreement with the predictions of an effective one-dimensional hydrodynamic model.