Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Tiefe Temperaturen Donnerstag<br />
With the recent advances in nanofabrication techniques it has become<br />
possible to manipulate and explore the electronic transport through<br />
individual molecules. This has posed an exciting theoretical challenge,<br />
namely the understanding of the conduction mechanisms at the molecular<br />
scale. So far, the effort has been concentrated in the analysis of the<br />
role of the electronic structure, but little has been done on the role of<br />
the internal degree of freedom of molecules. In this talk I will present our<br />
efforts to understand what are the effects of the vibrational modes in the<br />
molecular conduction. Making use of the density functional theory, we<br />
have developed an ab inito approach to describe the influence in the electrical<br />
current of the inelastic electron-phonon processes. This approach<br />
allows us to address many different questions such as (i) what makes<br />
that in some experimental situations the vibrational modes enhance the<br />
current and some others they reduce it? (ii) What are the possible signatures<br />
of these modes in the current-voltage characteristics? (iii) What<br />
are the selection rules that explain why some vibrational modes do not<br />
show up in the transport experiments?<br />
TT 27.8 Do 11:45 H19<br />
Controlled contacting of single-walled carbon nanotubes<br />
— •Daniel Secker 1 , Ralph Krupke 1 , Heiko B. Weber 1 ,<br />
and Hilbert v. Löhneysen 2,3 — 1 Forschungszentrum Karlsruhe,<br />
Institut für Nanotechnologie, PO-Box 3640, D-76021 Karlsruhe —<br />
2 Forschungszentrum Karlsruhe, Institut für Festkörperphysik, PO-Box<br />
3640, D-76021 Karlsruhe — 3 Physikalisches Institut, Universität<br />
Karlsruhe, D-76128 Karlsruhe<br />
We present a method to encapsulate the ends of single-walled carbon<br />
nanotubes (SWNT) in metallic leads. For this purpose we employed an<br />
inorganic shadow mask of Si3N4 patterned by e-beam lithography on a<br />
PMMA/Si3N4/SiO2/Si substrate [1]. The SWNTs are deposited between<br />
the contacts after a first evaporation step by applying an ac electric field<br />
making use of the dielectrophoretic force [2]. A second evaporation step<br />
encapsulates the ends of the SWNTs by the metallic leads. Therefore<br />
in contrast to marker-assisted e-beam lithography any exposure of the<br />
SWNTs to organic substances like PMMA is avoided. We present lowtemperature<br />
electrical transport measurements with samples thus prepared.<br />
[1] T. Hoss et al., Microel. Engin. 46 (1999) 149-152<br />
[2] R. Krupke et al., Appl. Phys. A 76 (2003) 397-400<br />
TT 27.9 Do 12:00 H19<br />
Parallel and Perpendicular Magnetoresistance of Multiwall<br />
Carbon Nanotubes — •Bernhard Stojetz 1 , Christoph<br />
Hendlmeier 1 , Christian Hagen 1 , Edina Ljubović 2 , Lazlo<br />
Forró 2 , and Christoph Strunk 1 — 1 Institut für Experimentelle und<br />
Angewandte Physik, Universität Regensburg — 2 Institute of Physics of<br />
Complex Matter, FBS Swiss Federal Institute of Technology (EPFL),<br />
Lausanne, Switzerland<br />
We report resistance measurements for single multiwall carbon nanotubes<br />
in magnetic fields both parallel and perpendicular to the tube axis.<br />
The tubes were trapped onto pre-patterned Al gate electrodes by means<br />
of an ac electric field. The strong electrostatic coupling of the nanotube<br />
to the gate allows a considerable variation of the doping level of the<br />
tube. Magnetoresistance traces were measured for many values of the<br />
gate voltage, which allows an ensemble averaging of the conductance<br />
fluctuations induced by quantum interference. The ensemble averaging<br />
reduces the conductance fluctuations while leaving the weak localization<br />
contribution to the resistance unchanged. The data can be consistently<br />
interpreted in terms of quantum transport in presence of weak disorder.<br />
TT 27.10 Do 12:15 H19<br />
Scaling of the Performance of Schottky barrier Carbon Nanotube<br />
Transistors — •Stefan Heinze 1 , Marko Radosavljević 2 ,<br />
Jerry Tersoff 3 , and Phaedon Avouris 3 — 1 Institute of Applied<br />
Physics, University of Hamburg, Jungiusstr. 11, 20355 Hamburg, Germany<br />
— 2 Novel Device Group, Intel Corporation, Hillsboro, OR 97124,<br />
USA — 3 IBM Research Division, T. J. Watson Research Center, Yorktown<br />
Heights, NY 10598, USA<br />
Today, the performance of carbon nanotube field-effect transistors<br />
(CNFETs) is already competitive with that of state-of-the-art silicon<br />
transistors [1]. However, a metal-semiconductor junction as in CNFETs<br />
fabricated to date necessitates a Schottky type contact which may present<br />
a significant barrier for transport. Most CNFETs thus behave as Schottky<br />
barrier transistors [2]. This leads to an unexpected scaling of CNFET<br />
performance as the device size is reduced [3]. Using an analytic model, we<br />
derive explicit scaling laws in the turn-on regime and for the transistor<br />
OFF state – in excellent agreement with experimental data [3]. An important<br />
consequence of the scaling behavior is an exponential increase of<br />
the OFF current with drain voltage for ultra-thin oxide CNFETs which<br />
limits the usable drain voltage and thus the achievable ON currents [4].<br />
[1] S. J. Wind et al., Appl. Phys. Lett. 80, 3817 (2002).<br />
[2] S. Heinze et al., Phys. Rev. Lett. 89, 106801 (2002).<br />
[3] S. Heinze et al., cond-mat/0302175 and Phys. Rev. B (in press).<br />
[4] M. Radosavljević et al., Appl. Phys. Lett. 83, 2435 (2003).<br />
TT 27.11 Do 12:30 H19<br />
Transport through a Carbon Nanotube with Superconducting<br />
Contacts — •Wolfgang Belzig, Mark Buitelaar, Thomas<br />
Nussbaumer, Christoph Bruder, and Christian Schöneberger<br />
— Universität Basel, Klingelbergstr. 82, 4056 Basel, Schweiz<br />
We report on experimental and theoretical studies of transport through<br />
multi-walled carbon nanotubes strongly coupled to superconducting<br />
leads. In the normal state of the leads the conductance displays a Kondo<br />
behaviour for odd numbers of electrons on the nanotube dot. If superconductivity<br />
is turned on, the transport characteristic changes dramatically.<br />
A large zero bias conductance (with G ≫ 2e 2 /h) and a strongly nonlinear<br />
differential conductance are observed. Both effects depend on the<br />
gate voltage. We explain the experimental observations theoretically by a<br />
subtle interplay between Kondo physics and proximity effect on the dot.<br />
Multiple Andreev reflections play a key-role to explain the features seen<br />
in the differential conductance.<br />
TT 28 FV-internes Symposium ”Theoretical Modeling of Materials with Correlated<br />
Electrons”<br />
Zeit: Donnerstag 14:00–18:10 Raum: H20<br />
Hauptvortrag TT 28.1 Do 14:00 H20<br />
Opportunities and challenges from electron spectroscopy for<br />
realistic correlated electron theory — •J. W. Allen — Randall<br />
Laboratory of Physics, University of Michigan, Ann Arbor, MI 48109,<br />
USA<br />
In the past 25 years electron spectroscopy has developed steadily to<br />
take its place with optical and Raman spectroscopy and with neutron<br />
scattering as an established general technique for studying the electronic<br />
structure of condensed matter systems. Already the current quality<br />
of available data on strongly correlated electron systems calls for theory<br />
beyond that of the model Hamiltonian and the need is expected to increase<br />
with further improvements in the experimental technique. I will<br />
give current examples in the context of the elucidation of Landau Fermi<br />
liquid theory quasi-particles and their absence in photoemission spectra.<br />
Hauptvortrag TT 28.2 Do 14:25 H20<br />
Dynamical Mean Field Theory (DMFT) and Electronic Structure<br />
Calculation — •G. Kotliar — Department of Physics and<br />
Astronomy, Rutgers University, Piscataway, NJ 08854-8019, USA<br />
We will discuss how a many body technique, DMFT is interfaced with<br />
band structure methods so as to obtain quantitative system specific information<br />
about correlated materials. Our talk will cover, computation<br />
of total energies, photoemission spectra, thermodynamical quantities<br />
transport properties phonon spectra, and optical conductivity. We will<br />
illustrate the method drawing examples from a simple system d electron<br />
system undergoing a density driven Mott transition (LaSrTiO3) and from<br />
lanthanide and actinide materials.<br />
Fachvortrag TT 28.3 Do 14:50 H20<br />
How Chemistry Controls Electron Localization in 3d 1 Perovskites<br />
— •O. K. Andersen — Max-Planck Institute for Solid State<br />
Research, D-70506 Stuttgart