Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
Oberflächenphysik Montag<br />
UHV conditions lowers the density of thiole molecules at the Au(111)<br />
surface which results in an alignment of the thiole molecules parallel to<br />
the Au surface. The focus is on the properties of the line-structure phase<br />
with the lowest surface density [1][2]. Al clusters are evaporated on the<br />
regions of the thiol line-structure in order to investigate where the Al<br />
atoms adsorb. With the STM we find that the Al clusters preferably<br />
adsorb onto the sulphur head of the thiol. Additionally, we investigate<br />
in AFM measurements with Al functionalized tips the forces acting on<br />
different parts of the thiol chain.<br />
[1] Poirer G.E. Langmuir 1999, 15, 1167-1175<br />
[2] Staub R., Toerker M., Fritz T., Schmitz-Hübsch T., Sellam F., Leo<br />
K. Langmuir 1998, 14, 6693-6698<br />
O 14.75 Mo 18:00 Bereich C<br />
Nanoscale Conductivity Spectroscopy on Solid Electrolytes using<br />
an Atomic Force Microscope — •Ahmet Taskiran, Andre<br />
Schirmeisen, Harald Fuchs, Frank Natrup, and Harmut<br />
Bracht — Physikalisches Institut and CeNTech, University of Muenster,<br />
Wilhelm-Klemm-Str.10, 48149 Muenster, Germany<br />
Ion conducting solid materials play an important role as electrolytes<br />
in energy conversion systems, such as batteries and fuel cells, and also in<br />
electrochemical sensors. An important prerequisite for further progress<br />
in this field is a better understanding of the ion transport mechanisms<br />
on microscopic and nanoscopic length scales.<br />
We are using atomic force microscopy (AFM) to measure the ionic<br />
conductivity in nanoscale volumes of dielectric glasses. The AFM is operated<br />
in the non-contact mode in vacuum. After a sudden change of the<br />
tip voltage, the relaxation of the electrostatic force between tip and sample<br />
is measured as a function of time. We measure these relaxation curves<br />
as a function of sample temperatures ranging from 100K to 675K. The<br />
observed relaxation curves are fitted well with a stretched exponential<br />
function and we can determine the activation energy of the conduction<br />
processes of the ions. First results indicate a good agreement of the activation<br />
energies for several prototype ionic glas conductors with values<br />
from macroscopic measurements. This method allows us to study fundamental<br />
processes of ionic transport and is in particular interesting for the<br />
investigation of nanostructured solid electrolytes.<br />
O 14.76 Mo 18:00 Bereich C<br />
Optical phase effects and resonance shift in scattering-type<br />
near-field infrared microscopy — •Thomas Taubner 1 , Fritz<br />
Keilmann 1 , and Rainer Hillenbrand 2 — 1 Max-Planck-Institut für<br />
Biochemie, Am Klopferspitz 18a, 82152 Martinsried — 2 Nano-Photonics<br />
Group, Max-Planck-Institut für Biochemie, Am Klopferspitz 18a, 82152<br />
Martinsried<br />
A scattering-type near-field optical microscope (s-SNOM) detects light<br />
scattered at the sharp tip of a probing needle and allows imaging with<br />
subwavelength resolution, independent of the wavelength used for illumination[1].<br />
We now study amplitude and phase of light scattered from a s-<br />
SNOM’s tip probing a flat SiC sample, at mid-infrared frequencies where<br />
surface phonon polaritons resonantly enhance the tip-sample near-field<br />
interaction [2]. A nanometer-scale variation of the gap width between tip<br />
and sample causes the optical phase to change dramatically and the resonance<br />
to shift. Both effects can be explained by theory that treats the<br />
system as a point dipole (tip) interacting with its image dipole (sample),<br />
in electrostatic approximation. The phase effects and resonance shifts are<br />
not restricted to phonon polariton excitation in polar dielectrics like SiC,<br />
but should be observable also for resonances related to plasmons and<br />
excitons.<br />
[1] T. Taubner, R. Hillenbrand and F. Keilmann, Journal of Microscopy<br />
210, 311 (2003)<br />
[2] R. Hillenbrand, T. Taubner and F. Keilmann, Nature 418, 159<br />
(2002)<br />
O 14.77 Mo 18:00 Bereich C<br />
Investigations on nanocrystals in silicondioxide by atomic force<br />
microscopy — •E. Beyreuther 1 , R. Beyer 1 , K. Walzer 1 , S.<br />
Behrendt 1 , V. Beyer 2 , J. von Borany 2 , J. Weber 1 , and L. Eng 1<br />
— 1 Technische Universität Dresden, Institut für Angewandte Physik, D-<br />
01062 Dresden — 2 Forschungszentrum Rossendorf, Institut für Ionenstrahlphysik<br />
und Materialforschung, PF 510119, D-01314 Dresden<br />
Nanocrystals in SiO2 are promising structures for future optoelectronic<br />
and memory devices. Optimization of the synthesis process needs detailed<br />
information about structure and morphology.<br />
Within the present work SiO2 layers of 100 nm thickness were ther-<br />
mally grown on Si(100). Subsequently Si or Ge nanocrystals were fabricated<br />
within those oxide films by ion implantation and rapid thermal<br />
annealing. Etching in buffered HF-solution with a low rate of 12nm/min<br />
removed the top oxide layer and uncovered the nanocrystals to a certain<br />
depth. The surfaces of several samples, which had undergone varied<br />
implantation and annealing conditions as well as different etching times<br />
were imaged by tapping-mode AFM down to scan sizes of 200x200 µm 2 .<br />
The apparent nanocrystal size and density were found to be dependent<br />
on the synthesis parameters and the position within the oxide layer.<br />
In comparison to TEM investigations of the same structures we discuss<br />
critically the determination of the cluster size.<br />
O 14.78 Mo 18:00 Bereich C<br />
Detection of dopant profiles in silicon by scanning capacitance<br />
microscopy and related techniques: the role of the passivation<br />
layer — •Reinhard Beyer 1 , Elke Beyreuther 1 , Bernd<br />
Schmidt 2 , Stefan Polzin 3 , and Jörg Weber 1 — 1 Technische Universität<br />
Dresden, Institut für Angewandte Physik, D-01062 Dresden —<br />
2 Forschungszentrum Rossendorf, Institut für Ionenstrahlphysik und Materialforschung,<br />
PF 510119, D-01314 Dresden — 3 Fraunhofer-Institut für<br />
Photonische Mikrosysteme, Grenzstrasse 28, D-01109 Dresden<br />
Scanning capacitance microscopy (SCM) was employed for the study<br />
of dopant profiles in silicon test structures. The samples were fabricated<br />
by implantation of boron and phosphorous into n-type silicon. The oxide<br />
mask for the implantation was shaped by photolithography. Hence,<br />
stripe patterns with a size of 2 µm of the implanted region and different<br />
widths of the interregion were obtained. The implantation dose was<br />
5 × 10 12 , 5 × 10 13 and 5 × 10 14 cm −2 for both implanted ions. Samples<br />
with native oxide coverage and with a 7 nm thick silicondioxide layer<br />
were compared in this study. SCM measurements were performed in the<br />
contact-mode. We show, that the contrast of the SCM signal between<br />
differently doped regions depends not only on the dc bias applied during<br />
the scan, but also on charge instabilities and trapping effects. The latter<br />
appeared mostly for samples with native oxide and resulted in hysteresis<br />
effects which could be observed with local dC/dV vs. V spectroscopy.<br />
The charge instabilities are discussed in a MOS-model. The results are<br />
compared with scanning spreading resistance measurements and with<br />
non-contact SCM.<br />
O 14.79 Mo 18:00 Bereich C<br />
Study of particle-substrate interaction by nanomanipulation experiments<br />
with dynamic scanning force microscopy — •Claudia<br />
Ritter 1 , Markus Heyde 2 , and Klaus Rademann 1 — 1 Humboldt-<br />
Universität zu Berlin, Institute of Chemistry, Brook-Taylor-Str. 2, D-<br />
12489 Berlin, Germany — 2 Fritz-Haber-Institute of the Max-Planck-<br />
Society, Faradayweg 4-6, D-14195 Berlin, Germany<br />
We utilise an advanced homebuilt SFM in the dynamic mode, in<br />
conjunction with a special homebuilt software, to perform precise<br />
nanomanipulation experiments. The corresponding experimental technique<br />
should be denoted as Dynamic Surface Modification (DSM), comprising<br />
both the dynamic technique of the SFM, as well as the manipulation<br />
(translation, in-plane rotation, cutting) of structurally unchanged<br />
particles on a given substrate surface. It is easily possible to switch between<br />
imaging mode and DSM mode, enabling the direct manipulation<br />
of nanoparticles under ambient conditions with high precision and simultaneously<br />
studying particle-substrate interaction to give evidence about<br />
motion and tribological values of the sample system. We have successfully<br />
manipulated miscellaneous nanoparticles on surfaces, e.g. antimony<br />
islands, gold islands, tin islands, nanotubes, small latex spheres as well<br />
as cells.<br />
O 14.80 Mo 18:00 Bereich C<br />
In-situ SPM usage at MOVPE-conditions — •Markus<br />
Breusing, Bert Rähmer, Raimund Kremzow, and Wolfgang<br />
Richter — TU-Berlin, Institut für Festkörperphysik, Hardenbergstr.<br />
36, 10623 Berlin<br />
In-situ scanning probe techniques which are applicable in an MOVPE<br />
growth environment to directly give quantitative information about the<br />
nano-scale topography of the sample do not exist up to now.<br />
Developing a SPM for in-situ MOVPE measurements requires a completely<br />
new setup. In comparison to the commercially available SPMsolutions,<br />
a number of additional problems have to be solved. The limited<br />
space in the MOVPE reactors and the high temperature caused by the<br />
thermal conductivity of the carrier gas during growth near the suszeptor<br />
requires a special design of the components of the SPM. On the other