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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

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