Research/Forschung
Research work concentrates on molecular nanostructures, functionalization
of molecular nanostructures,
dimensionality and quantum size effects, template grown nanomaterial, nanoreactors, etc.
Examples are:
fullerenes, fullerene derived materials, nanotubes,
nanostructured carbon systems, nanodiamond
nanodiamond nanocoatings, etc.
Information about research in the lab:
Current research projects:
FULPROP : TMR project,
more links to
the FULPROP homepage
local
links to the FULPROP research and training activities at the IMP
FUNCARS: IHP project,
more,
links to the FUNCARS homepage
local links
to the FUNCARS research and training activities at the IMP
MEA-PPNCD : GROWTH project, more
NANOCARB : INTAS project, more
links to the NANOCARB homepage
local
links to the NANOCARB research and training activities at the IMP
NANOTEMP: TMR project, more links to the NANOTEMP homepage
local
links to the NANOTEMP research and training activities at the IMP
VDWAALS: project supported
by FWF, more
links to the project homepage
RÖHRCHEN: project supported by FWF,
more
links to the project homepage
MASKEN: project
supported by FWF, more
links to the project homepage
Description of research work:
Our current work is mostly in the field of nanomaterials. The Nanotech-Now site has lots of useful
infos and links about this subject in general.
The discovery of the quantum Gyroscop:
Details can be found here.
Fullerenes:
Fullerenes are molecular cages consisting of only carbon atoms. The
arrangement of the atoms is almost exclusively in the form of hexagons
and pentagons. 12 pentagons and 20 hexagons make
the most famous C60 cage. This cage was first identified experimentally
by H.W. Kroto, R.E. Smalley, and R.F. Curl in 1985.
These researchers were awarded the Nobel prize
in Chemistry for their discovery in 1996, after W. Krätschmer and D. Hufman had developed
a technique for the growth of fullerenes in large quantities.
C60 fullerenes are the most stable and the most abundant species. C60
crystals exhibit several interesting phase transitions and they are photophysically
active in several ways. They can be doped to a metallic and even
superconducting state. Transition temperatures in the latter matrerial are
as high as 30 K.
C60 fullerene
Polymeric Fullerenes:
A new class of fullerenic materials!
Fullerenes of the above type can polymerize to a covalently connected
string, pane, or even threedimensional arrangement of individual molecules.
The connection can be either by one single bond between carbons on neighboring
cages or by a pair of single bonds between the cages.
Doped species as well as undoped material is
available. The new polymers can be semiconducting
or metallic but no superconductivity has been observed sofar.
Polymerization has been reported for C60 but also for C70 cages.
Threedimensional polymerization can leed to ultrahard
material, material which is harder than diamond.
Doping of the polymer can be performed by intercalation
of electron donors inbetween the cages but also by substitution of carbon atoms by donors on the
cage. For dimers intercalation doped systems and substitution doped systems
exhibit very similar electronic properties.
Doped polymers can have very unusual magnetic properties.
Dimeric (C59N)2
Nanocage Encapsulates:
Metallic (transition metals or rare earths) or nonmetallic atoms (N,
P, He) can be encapsulated into the fullerene cages. Such materials exhibit
an other class of new fullerenic materials. The endohedral chemistry of
such systems was found to be quite different to the conventional exohedral
chemistry.
Endohedral metallofullerene Sc3@C84
Carbon Nanotubes:
Carbon nanotubes are rolled up sheets of graphene where the geometry
for the rolling up process is determined by a lattice vector (folding vector or Hamada
vector) of the plane. The two components of the lattice vector,
expressed as integers (n,m), determine the geometry of the tubes like
its diameter and helicity and its electronic structure. Typical
values of the former are 1.4 nm. With respect to the latter semiconducting tubes, narrow gap tubes and metallic tubes are known. The extension of the
described systmes is exactly ondimensional with respect to its periodicity
in space. As a consequence the electronic density of states exhibits well
expressed Van Hove singularities.
Tubes of the above type are called single wall
carbon nanotubes (SWCNTs). In contrast tubes consist often
of a set of concentrically arranged SWCNTs. In this case the tubes are
called multiwall carbon nanotubes (MWCNTs). Single wall carbon nanotubes are usually aggregated into
bundles with a hexagonal lattice structure in the cross section but with
a highly incommensurate arrangement of the tubes in the bundle. Similarly,
for the MWCNTs the concentic tubes are necessarily arranged in an incommensurate
manner as the have different diameter and different helicity.
Electronic and latticdynamical properties if the tubes exhibit macroscopic quantum effects which, among several
other interesting technical properties, triggered the dramatically growing
interest in such systems.
A single wall carbon nanotube
Results of electronic density of states (DOS) calculations are available
by following this link.
Nanocrystalline Diamond:
Nanocrystalline diamond can exhibit optimum properties for many applications
in high technology electronics, heat technology or mechanical technology.
Low wear and low friction are obtained for ultra smooth films. New technologies
are to be developed for the preparation of thin films by CVD with very
good lamination to substrates such as cutting tools, bearings, or packaging
material. .
Stand 22.11. 2001
Betreuung durch Hans Kuzmany