ATOMIC BEAM EXPERIMENTS
I. Stark measurements in an atomic thallium beam
-
- Julie Rapoport '97 designed and put together a new atomic beam
source and vacuum system which will ultimately provide a dense
collimated beam of atomic thallium (photo of
current system, simplified
schematic). With this tool we plan to measure Stark
interference and Stark shifts in the ground-state transitions of
thallium. Peter Nicholas '98 worked to bring the new beam
apparatus on-line (current top view of
source showing oven, nozzle, and collimation cone), and Rob Lyman
('99) and Andrew Speck ('00) completed construction of the final
beam line elements. Here is a current
schematic of the finished product.
-
- In 1999-2000, Andrew Speck '00 installed our laser locking
system whereby we lock the diode laser by comparing its frequency
to that of a known, stable HeNe reference laser. At this point the
only frequency changes occuring are caused by synthesizer tuning
of the AOM. Using double-pass geometry (and after frequency
doubling), the AOM frequency shif is multiplied four-fold in the
UV, allowing us sufficient tuning range to the maximum Stark shift
achievable in our system (90 MHz @ 30 kV/cm electric field). Our
measurement scheme involves locking the laser to the side of the
atomic absorption, then applying simultaneous E-field and AOM
frequency changes such that we stay at the same relative point on
the side of the line.
In Jan 2001 we obtained the first
spectra from the atomic beam apparatus thanks to the hard work of
many students, and most recently to postdoc David Richardson, and
Paul Friedberg '01 (see here)!
[The width is nearly 10 times narrower
than the equivalent data taken using the vapor cell (subject of Rob's
thesis and our most recent paper). The thallium oven/source inside
the beam unit was at 740 C for this data (our max is about 800 C). We
superimpose the cell data for comparison! It is very encouraging to
see absorption equivalent to almost one full optical depth in the
beam. For this data we 'chopped' both the laser beam and the atomic
beam.]
- During 2001-2002, with Charlie Doret
'02 completing his thesis and at the helm (and PKM on sabbatical
leave), we completed apparatus testing, took extensive data and
have now completed a new Stark shift measurement with 0.5%
accuracy. Among various other honors, Charlie was selected to give
an invited talk at the 2002 APS/DAMOP meeting (Williamsburg, VA,
May 29-June1). We are happy that he will be around in the lab to
help launch a new set of students in the summer of 2002 before
heading off to Harvard this fall.
- [pdf version of Charlie's
thesis defense talk, May 2002]
-
II. Future M1 spectroscopy in the Atomic Beam
-
- One goal of the atomic beam project is to create a dense beam,
and utilize signal processing techniques to allow transmission
spectroscopy for the case of the weak M1 transition. In this way
the Faraday rotation of 1.28 micron light as it passes through the
beam in a known magnetic field can be used as a density
normalization method as we measure the absorptivity change upon
application of a very large static electric field. Precise
measurements of the Stark shift and of the scalar and tensor
polarizability in this transition offer another excellent way to
independently test the atomic structure calculations. A possible
way to increase the IR absorption to more measurable levels would
be to introduce a ring enhancement cavity (see below) into this
experiment. The use of the chopping wheel and lock-in detection of
small absorption signals will be essential here. We are also
pursuing the idea of FM-modulation of the diode laser frequency
and subsequent demodulation to extract a clean, background-free
absorption signal.