Stark Deceleration

Alternating gradient Stark decelerator
Alternating gradient Stark decelerator

In a supersonic expansion source, gas expands through the nozzle of a high pressure valve into a vacuum chamber, thereby cooling to low temperatures. The mean speed of the gas is high, typically 300-1000 m/s, but the distribution of speeds is very narrow, corresponding to a low translational temperature. A wide variety of molecules can be introduced into the supersonically expanding gas, and their translational and internal degrees of freedom also cool to low temperatures, typically to about 1K. 

This cold, high speed jet of molecules can be slowed down using a Stark decelerator. When a molecule moves into a region of high electric field it will gain kinetic energy if it is a high-field-seeker, and lose kinetic energy if it is a low-field-seeker. In the Stark decelerator, molecules move through a series of electric field gradients that are switched on and off so that the molecules are gradually slowed down. This deceleration process can work for both strong-field and weak-field seekers - it is simply a matter of choosing the correct switching sequence. However, strong-field-seekers are far more difficult to focus through the decelerator because they tend to crash into the electrodes where the field is strongest. This is unfortunate, since cold, heavy molecules are all strong-field seekers in the large electric fields of the Stark decelerator.  We use an alternating gradient focussing scheme to transport our strong-field-seeking molecules through the decelerator. Each deceleration stage acts as a lens that focusses the molecules in one transverse direction, and defocusses them in the other. By alternating the focussing and defocussing directions of successive lenses, overall focussing is possible in both transverse directions. 

Stark Deceleration

A model of the Stark decelerator
A model of the Stark decelerator

We have produced beams of cold LiH molecules in the first rotationally excited state, which is a weak-field seeking state. We decelerate these molecules to low velocity using a 100 stage Stark decelerator operated at a field strength of 100kV/cm. The electric field of the decelerator is switched on and off so that the molecules are always moving out of regions of weak field and into regions of strong field. This slows the molecules down, reducing their speed nearly to zero at the exit of the decelerator.

The figure below shows data demonstrating the deceleration of lithium hydride molecules.  The molecules entered the decelerator with a speed of 420m/s. The graphs show the time of flight profiles of the molecules, measured by laser induced fluorescence at the exit of the decelerator, as the degree of deceleration is increased. The decelerated bunch moves to later arrival times as the molecules slow down. The arrows show arrival times predicted from a simple model, with the final speed shown next to each. The slowest molecules we have produced are moving at 53m/s, slow enough to begin trapping experiments.

Stark deceleration of lithium hydride
Stark deceleration of lithium hydride

 

Deceleration of ground state CaF molecules
Deceleration of ground state CaF molecules

We have worked on the deceleration of  YbF and CaF molecules, in weak-field and strong-field seeking states.

The molecules are created at temperatures of about 3K by ablating Yb or Ca into a carrier gas containing sulphur hexafluoride. They pass through the decelerator and are then detected by laser induced fluorescence. To decelerate molecules in strong-field seeking states, we developed an alternating gradient Stark deceletrator. Each electrode pair of the decelerator forms one lens of the alternating gradient structure. Each lens focusses in one plane and defocusses in the other. The focussing and defocussing planes alternate. Deceleration occurs in the gap between one lens and the next.

The figure shows the deceleration of ground state CaF molecules. The molecules enter the decelerator at a speed of 435m/s. The arrival time of the molecules at the detector tells us about their speeds. The figure shows this arrival time, relative to the central arrival time when the decelerator is turned off. A narrow peak appears in the time profiles, which is delayed more and more as the number of deceleration stages used increases. These are the decelerated molecules. 

Most recently, in collaboration with Gerard Meijer's group, we have shown how to decelerate YbF molecules in a travelling wave decelerator.

The alternating gradient guide
The alternating gradient guide

Ground state molecules can be transported in an alternating gradient guide. The operating principle is the same as for the decelerator. We have demonstrated a guide that has a four-rod geometry designed to minimize the lens aberrations which tend to reduce the transmission. The guide is useful for transporting molecules from a cold source, such as a buffer gas source. 

Traveling wave deceleration of heavy polar molecules in low-field seeking states, N.E. Bulleid, R.J. Hendricks, E.A. Hinds, Samuel A. Meek, Gerard Meijer, Andreas Osterwalder, and M.R. Tarbutt, Phys. Rev. A 86, 021404(R) (2012)

Stark deceleration of CaF molecules in strong- and weak-field seeking states, T. E. Wall, J. F. Kanem, J. M. Dyne, J. J. Hudson, B. E. Sauer, E. A. Hinds and M. R. Tarbutt, Phys. Chem. Chem. Phys. 13, 18991 (2011)

Nonadiabatic Transitions in a Stark Decelerator, T. E. Wall, S.K. Tokunaga, E.A. Hinds, M.R. Tarbutt, Physical Review A 81, 033414 (2010)

Stark deceleration of lithium hydride molecules, S. K. Tokunaga, J. M. Dyne, E. A. Hinds and M. R. Tarbutt, New Journal of  Physics 11, 055038 (2009)

Transport of pol ar molecules by an alternating gradient guide, T.E. Wall, S. Armitage, J.J. Hudson, B.E. Sauer, J.M. Dyne, E.A. Hinds, M.R. Tarbutt, Physical Review A, Vol. 80, 043407, (2009)