Rydberg
Atoms in Bose-Einstein Condensates
Rydberg atoms immersed into a condensate of ultracold ground
state atoms
is a complex many-body problem.
We study systematic approaches to this intriguing situation where many
different
interactions take place. Different levels of approaches are
pursued
such as treating the condensate as a classical coherent state or taking
into
account the quantized excitations of the condensate. Experiments on
these
systems are under way at several groups.
Rydberg Atoms
Rydberg atoms, in contrast to atoms in their electronic ground states,
possess extraordinary properties. They are of gigantic extension
and the highly excited states possess extremely long radiative
lifetimes of the order of milliseconds. Pictorially speaking the
valence electron of a Rydberg atom is in a large loosely bound orbit.
Consequently Rydberg atoms possess large
polarizabilities and are extremely sensitive to external
fields. To take advantage of the susceptibility of Rydberg atoms to
external fields,
and iin particular to other Rydberg atoms,
ultracold Rydberg gases can be created.
Starting from laser cooled atomic clouds, the atoms are excited using a
laser tuned slightly below the ionization energy.
The so created strongly interacting
ultracold
Rydberg gases are ideal
candidates to study intriguing many-body physics and collective quantum
phenomena on a macroscopic scale.
Bose-Einstein Condensation
Ever since the experimental realization of Bose-Einstein condensation
(awarded with the Nobel prize in 2001; see
http://cua.mit.edu/ketterle_group/research.htm
for a nice website), ultracold atoms have been an enourmously popular
research object. Using the atoms' interaction with electric (Laser)
and magnetic fields, one can virtually `design' both their external
trapping forces and their interactions. That makes them an extremely
useful tool to study all kinds of fundamental
physics (such
as superconductivity/superfluidity). But there also
applications
exploiting their coherence: e.g., in atom interferometry or in quantum
computation.
Rydberg Atoms immersed in a
Bose-Einstein Condensate
The problem we investigate bridges the gap between the situations
described above, namely the cases of many Rydberg atoms and that of
many ground state atoms: We explore the spectral structure of a
Rydberg atom immersed into a Bose-Einstein condensate. This system is
of immediate physical interest and well-accessible within present-days
ultracold experimental techniques.
The electronic spectrum of the Rydberg atom depends crucially on
characteristic parameters of the condensate and of the quantum numbers
of the Rydberg state. Therefore it is possible
to determine these parameters of the condensate by spectroscopy of the
energy
spectrum of a single atom. As an example the dependency of the shift of
the energy spectrum due to the interaction with the condensate for the
n=30 states on the axial trapping frequency for an
axial symmetric harmonic trap is shown.

Another feauture of this system is that
one can simulate effective potentials for the Rydberg atom by tuning
the parameters of the condensate. This makes it possible to
investigate
atoms in potentials which cannot be realized by
electrmagnetic fields because of the restrictions due to
Maxwell's equations. As an example the shift of the energy
spectrum of an atom is shown
for an effective potential which corresponds to the diamagnetic part
of an atom in a
magnetic field where the trapping frequency corresponds to the magnetic
field.
Invitation
You are warmly welcome to join our efforts to uncover natures secrets:
please step by (INF 229 (Umweltphysik), 6th floor, room 620)
or drop a note (
stephan.middelkamp@pci.uni-heidelberg.de).