(Back to
the menu - click here.)
Date: |
Download-files: |
Time: |
Thursday, 26. Sept. 2013 |
Low resolution for MediaPlayer (Windows), optimized for slow
network-connection: Low resolutions for MAC: High
resolutions video (any system with MP4-support): |
15:15 – 16:15 |
Abstract
We present an
introduction to the field of ultracold gases where many-body quantum physics
can be studied
with
unprecedented accuracy and controllability of the system parameters. One
fascinating possibility is to
distort the
symmetry of the two spins in the usual BCS-type superconductivity scenario.
We present
experimental advances on this topic as well as several examples of our related
work.
One such
example is the the Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) state where
spin-density imbalance
and
superconductivity can coexist due to spatial oscillations of the superconduting
order parameter.
We consider
ultracold Fermi gases with two pseudospin components and present three
different topics
where the
ability to control and manipulate the pseudospins separately plays a key role.
1) We show that the FFLO state is stabilized
in lattice geometries [1] and present a full finite-temperature
phase diagram for the one-dimensional (1D)
to three-dimensional (3D) crossover of the FFLO state
in an attractive Hubbard model of
3D-coupled chains in a harmonic trap, calculated with dynamical mean field
theory [2].
2) We show that imposing different potentials
(voltages) for the spins reveals an inherent single particle
interference effect in Josephson
oscillations [3].
3) We propose a novel way of distorting the
two spin species that are forming Cooper pairs: namely,
a mixed-geometry system of fermionic
species selectively confined in lattices of different geometry [4].
A rich phase diagram of interband pairing
with gapped and gapless excitations is found at zero temperature.
We also
show that the Fermi surface topology further divides the gapless phase into
subclasses between which
the system
undergoes density-driven Lifshitz transitions.
[1] T.K.
Koponen, T. Paananen, J.-P. Martikainen, and P. Törmä, Phys. Rev. Lett. 99,
120403 (2007).
[2] M.O.J.
Heikkinen, D-H. Kim, and P. Törmä, Phys. Rev. B 87, 224513 (2013).
[3] M.O.J.
Heikkinen, F. Massel, J. Kajala, M.J. Leskinen, G.S. Paraoanu, and P. Törmä,
Phys. Rev. Lett. 105, 225301 (2010).
[4] D-H.
Kim, J.S.J. Lehikoinen, and P. Törmä, Phys. Rev. Lett. 110, 055301 (2013).