We conducted the first thermodynamic experiment on an
optically-trapped
Fermi gas of atoms in the regime of strong interparticle interactions
[Science magazine, online
publication].
In addition to measuring the heat capacity of this
unique physical
system, our study represents the first attempt at direct thermometry in
the strongly interacting regime. Making use of novel energy input
and temperature
measurement techniques, we observe a transition in the heat capacity
which theory interprets as the onset of a high temperature superfluid
state.
Our precision study of the heat capacity is made possible by a
novel energy input technique.
The optical trap is briefly turned
off, and the atomic cloud is allowed to expand. When the trap is turned
on
again, the cloud has grown in size, and this increased size is
converted to additional energy when the gas returns to equilibrium. By
varying the duration of time that the trap is off, we can precisely
control the energy input to the gas. A measurement of the heat capacity
of the gas then involves adding various amounts of energy to the system
and measuring the resulting temperature.
Measuring the temperature of a strongly-interacting
Fermi gas is no small task. Unlike thermometry for noninteracting
systems, there is no universally agreed-upon technique for measuring
temperature in the strongly-interacting regime. However, in
collaboration with a theoretical group at the University of Chicago
headed by Kathryn Levin, we have suggested a pragmatic temperature
measurement scheme inspired by the close resemblance of
strongly-interacting clouds of atoms to noninteracting clouds.
While our temperature measurement technique may prove to
be only approximately correct, it is the first attempt at direct
thermometry in the strongly-interacting regime. The
use of this thermometry technique allows for quantitative comparison
between theory and experimental results. We find that our heat capacity
measurements in the strongly interacting regime are in excellent
agreement with predictions made by the Chicago theoretical group.
Furthermore, their theory interprets our observation of a transition in
the heat capacity of a strongly-interacting Fermi gas as evidence for a
superfluid phase transition.
Remarkably, the Chicago group's theoretical formalism was originally
developed to explain the
behavior of high temperature superconductors. While dilute Fermi gases
and high temperature superconductors might seem like very disparate
systems, the underlying physics may be quite similar. In fact,
the good agreement between experiment and theory in our study of the
heat capacity lends
some support to the idea that particles in a strongly-interacting Fermi
gas can undergo pairing at temperatures higher than the superfluid
transition temperature. This process may be analogous to the
transition from a normal to a superconducting state in a high
temperature superconductor.
These results have been highlighted in a Duke University press
release and Nature
magazine's research
highlights.