Progress

July 2019

Analyzed cracking behaviour of Argon solid. Cracks are reproducible and arise due to the contraction of Argon as substrate cools. Shards of with surface area of 1 mm2 can maintain transparency over multiple days.
Photo of Argon solid after growth before any cracks form.
Photo of Argon solid after cooling to temperatures at which cracks form.

June 2019

Installed CCD camera to observe transparency across entire substrate during and after growth. Transparency across whole cyrogenic Argon solid is maintained at 95% across multiple days. Gain over

Apr 2019

Designed an Einzel lens system used to focus the ions transported by the ion guide onto the cryogenic argon crystal. The middle element of the lens allows either for the transmission of the ions or the deflection of the ions onto a Faraday cup for counting. A picture of a split Einzel lens.

Feb 2019

Began experiments to analyze Ar purification techniques in a dedicated vacuum chamber. Our goal is to obtain impurity levels lower than 1 part in 1012. A picture of a vaccuum chamber wrapped in tin foil.

Jan 2019

Detected fluorescence spectrum (averaged over 18 hours) of the sapphire substrate on which Ar crystals are grown. The substrate was illuminated during this time by a 500-mW frequency-doubled Nd:YAG laser. The fluorescence peak at 694 nm is due to Cr impurities in the sapphire, with the other features being due to spectral impurities in the Nd:YAG laser light. A graph showing fluorescence off the sapphire substrate on which Ar crystals are grown. Two peaks are visible: an 806 nm peak coming from the Nd:YAG and a 694 nm peak due to Cr impurities.

Dec 2018

Probed microscopic changes in Argon solid surface topology by observing the speckle pattern created by laser light as it scatters through an evaporating argon crystal as it is heated from 20 to 200 kelvin. Two hours of this experiment is captured in the video below.

November 2018

Grew an 360-μm-thick argon cryogenic solid over a period of 4.5 hours at a rate of just under 6 interference fringes (1.5 μm) per minute. Below is a snapshot of the first half hour of growth. A plot showing half an hour of growth at a rate of just under 6 fringes per minute.

October 2018

Connected Hexapole Ion Guide to Commercial Electrospray Ion Source. Transported BaF+ ions with near-100% efficiency to end of hexapole guide by using angular deviations in the ion path to reduce on-axis neutrals. Differential pumping in the transfer system permitted chamber pressures on the order of 10-8 torr.
Two photos of a lab space. Lots of shelving is shown. A corner of an optical table is seen .
A data collection station with a computer and two racks are seen. A vacuum sstem is slightly visble above the smaller rack. The optical table and some benches are also visible.

September 2018

Published article describing hyperfine structure of oriented polar molecules and details proposed EDM3 experimental method. Our publication, <b>Orientation-dependent hyperfine structure of polar molecules in a rare-gas matrix: a scheme for measuring the electron electric dipole moment</b> featured as the Editor's Choice for Physical Review A

August 2018

Inserted coldhead into vacuum system and create first cryogenic Ar solid.
A sin graph showing signal with high frequency before frequency lowers for a period and the signal levels off
A close up of a thin window.
A side view of the open vaccuum system, showing a copper coldhead inside

July 2018

Acquired and tested three laser systems: an external-cavity diode laser with a wavelength tunable from 790 to 870 nm for spectroscopy of BaF embedded in solid Ar, a stabilized HeNe (632 nm) for interferometry, and a Nd:YAG green laser with a power of 500 mW for photoluminescence. A side view of three lasers

June 2018

Completed vacuum system to house the experiment. A side view of the vaccuum system. Two large supercrosses are seen connected, with a large turbo pump coming out of the top of the further one. Several wires are seen attached.

May 2018

First attempt at Ar annealing. Three graphs side by side. <br> The leftmost shows normalized transmission (units arbitrary) against time in minutes from 45-90 min. The graph dips from 45-60 min
		before rising from 60-70 min at which point it plateaus.<br> The next graph shows temperature of 2nd stage(K) vs time in minutes (from 45-90). A fairly linear upwards sloping line (with slight negative curvature) is seen. The line increases at a rate of about 0.42 K per min starting from around 22 K at 45 min<br> The last graph is pressure (Torr) vs time and shows a graph which plateau until 50 min, until it rises steadily until peaking around 70 min before declining.

April 2018

Finished renovation on new 2000 square-foot laboratory space.
Two photos of a lab space. Lots of shelving is shown. A corner of an optical table is seen .
A data collection station with a computer and two racks are seen. A vacuum system is slightly visible above the smaller rack. The optical table and some benches are also visible.

March 2018

Observed isotopically pure 138Ba19F from an electrospray source.
A mass spectrometer graph showing distinct peaks one 136.80, 157.50 and 154.50.