Our research interests are centered around the following topics:
Density functional theory
Within density functional theory (DFT) the complicated
quantum mechanical many-body problem of interacting electrons and
nuclei is mapped exactly, without introducing empirical parameters,
onto an effective single particle problem. The single particle problem
can then be solved very efficiently using highly parallelized computer
codes and thus allows the accurate ab initio calculation of a
large variety of materials properties. The huge impact of DFT on
today's understanding of materials properties was recognized by the
Nobel Prize in chemistry for Walter Kohn in 1998 (see Figure on the
right).
The ultimate goal for the development of such a "first principles"
method is to be able to calculate all properties of an arbitrary
material using as input only its chemical composition. This is
obviously an extremely ambitious goal, but achieving this goal would
be a tremendous achievement with huge impact on both materials science
and engineering. Modern first principles methods are already extremely
powerful in accurately determining many properties for a large variety
of materials, and the improvement of currently used methods to include
larger classes of materials and formerly unaccessible quantities is
therefore a very active and important field of research.
In addition, first principles calculations provide an ideal
environment where atoms can be accurately placed at certain positions,
defects can be excluded and then re-introduced in a controlled way,
and even certain interactions can be "switched off" to see the
resulting effect on the physical properties. The insights gained by
such "computer experiments" are extremely useful for guiding modeling
efforts and interpreting/understanding experimental observations.
Combining DFT with model approaches
Even though the possibility to calculate the values of all observables
for an arbitrary material would be a tremendous achievement, it would
not necessarily lead to further physical insights. To gain such
insights, one has to develop models that explain a certain effect in
relatively simple terms. First principles methods represent a very
useful tool for such model development, since it is possible to
analyze in detail how a certain result comes about. After a model has
been developed, the corresponding input parameters can be calculated
by first principles methods to see whether the model leads to
physically reasonable results.
Furthermore, a very promising way to improve the description of
"correlated electron materials" (such as most of the complex oxides
that are decribed below) is to combine DFT with numerical many-body
techniques. These techniques are usually applied to very simplified
models with only a few number of bands, but can describe effects that
are not captured by current DFT methods. However, recent progress in
"dynamical mean-field theory" (DMFT) has now opened up the possibility
for many-body calculations based on realistic materials-specific
band-structures.
Complex transition metal oxides are fascinating materials both from a basic
science perspective as well as from a technological viewpoint (see Figures on
the right for some examples). The unique electronic structure of these
materials leads to a very strong coupling between structural, electronic, and
magnetic properties. To understand this complex interplay between the various
degrees of freedom is a great challenge for modern condensed matter
physics. In addition, the same interplay leads to a tremendous variety of
physical properties, such as for example metallic, semiconducting, or
insulating behavior, high dielectric constants, piezoelectricity,
ferroelectricity, ferromagnetism, metal-insulator transitions, and high
temperature superconductivity. These functional properties are
extremely attractive for use in modern electronic devices such as nonvolatile
memory, integrated circuits, or new types of sensors and actuators, and in
addition offer great prospects for the development of future technologies.
The unique features of transition metal oxides are a result of the partial
occupation of the electronic d shell on the transition metal
cation. The corresponding electronic orbitals are intermediate between being
atomic-like and band-like, i.e. between being localized at
the cation sites and being delocalized throughout the crystal by the formation
of covalent chemical bonds. The extent to which these d electrons form
chemical bonds crucially depends on volume, transition metal-oxygen bond
length, bond angle (the angle formed by a transition metal-oxygen-transition
metal structural unit), and the symmetry of the crystal-field, which
is caused by the anion polyhedra surrounding the metal cation. One very common
and probably the most studied crystal structure of complex transition metal
oxides, the perovskite structure, is depicted on the left. In the perovskite
structure the transition metal cations form a simple cubic lattice and are
surrounded by octahedra of oxygen anions; additional (non-transition metal)
cations occupy the space in between these octahedra. Small distortions from
the perfect perovskite structure or small changes in volume or electron count
(i.e. doping) can tip the balance toward either more localized or more
covalent, thereby eventually changing the system from insulating to metallic
or fundamentally affecting the degree and overall character of the magnetic
ordering.
Multiferroic materials are materials that combine two or more of the
primary forms of ferroic order, i.e. ferroeleasticity,
ferroelectricity, ferromagnetism, and ferrotoroidicity. However, most
of the recent research on multiferroics has focused on materials that
combine some form of magnetic order (ferromagnetic, antiferromagnetic,
non-collinear, ...) with ferroelectricity, so that the term
"multiferroics" is now often used synonymous with "magnetic
ferroelectrics".
Due to the combination of magnetic and dielectric properties, with
eventual cross-coupling between these properties, multiferroics have
immense potential for technological device applications and at the
same time they pose very interesting and rich fundamental physics
problems. It is probably this combination of applied and fundamental
research that is partly responsible for the strong attraction that
these materials have developed in recent years (in December 2007
Science Magazine listed multiferroic materials as one out of ten
"Areas to watch in 2008", the only entry from the Materials
Science/Condensed Matter area that was included in this list).
If you are interested in further details, you can also have look at
this lecture I gave at the 2008 APCTP winter school on multiferroics
in Pohang, South Korea (pdf-format,
5.1MB).
Last updated: 2010 02 05