Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Magnetismus Montag<br />
structurally different island types can clearly be distinguished by their<br />
spin-averaged electronic structure. Spin-polarized measurements allow a<br />
separation of spectral contributions arising from different island stacking<br />
or from opposite magnetization states, respectively. We compare these<br />
results with ab initio electronic band structure calculations.<br />
In an applied magnetic field both island types are found to be magnetized<br />
perpendicular to the surface, with large values of saturation field,<br />
remanence, and coercivity. It is found that for one island type the saturation<br />
field is significantly higher than for the other.<br />
As was shown in spin-averaged measurements [1], bias-voltage dependent<br />
oscillation patterns of the local density of states (LDOS) due to<br />
electron confinement can be observed on the Co islands. Here we present<br />
spin-polarized data revealing the oscillation amplitude to depend on the<br />
spin direction.<br />
[1] L. Diekhöner et al., Phys. Rev. Lett. 90, 236801 (2003).<br />
MA 4.8 Mo 12:00 H22<br />
Magnetism of Fe on W(001) — •Kirsten von Bergmann,<br />
Matthias Bode, and Roland Wiesendanger — University of<br />
Hamburg, Institute of Applied Physics, Jungiusstr. 11, 20355 Hamburg,<br />
Germany<br />
There has been a lot of interest in the magnetic properties of the highly<br />
strained pseudomorphic layers of Fe on W(001). Using spatially averaging<br />
methods contrary results have been reported concerning the anisotropy<br />
axis [1-3]. To overcome this discrepancy we used spin-polarized scanning<br />
tunneling microscopy (SP-STM) to investigate this system: the method<br />
is magnetically sensitive and has a high spatial resolution which allows<br />
not only the investigation of magnetic properties but also a direct correlation<br />
to electronic structure measurements and detailed topographic<br />
studies.<br />
The domain structure of Fe on W(001) in the low coverage regime is<br />
imaged and the four fold anisotropy can directly be deduced from maps<br />
of differential conductance (dI/dU). Quantitative analysis of the intensity<br />
of the dI/dU signal reveals a layer-dependent anisotropy axis in the<br />
pseudomorphic regime: the magnetic easy axis rotates by 45 ◦ from 〈110〉<br />
in layers with a local coverage of 2 and 3ML to 〈100〉 at a local coverage<br />
of 4ML.<br />
[1] G. A. Mulhollan et al., Phys. Rev. B 43, 13645 (1991).<br />
[2] T. L. Jones and D. Venus, Surf. Sci. 302, 126 (1994).<br />
[3] W. Wulfhekel et al., Europhys. Lett. 49, 651 (2000).<br />
MA 4.9 Mo 12:15 H22<br />
Spin-orbit interaction at the Gd(0001) and O/Gd(0001) surfaces<br />
— •O. Krupin 1 , G. Bihlmayer 2 , S. Gorovikov 3 , J. E. Prieto<br />
1 , K. Döbrich 1 , G. Kaindl 1 , S. Blügel 2 , and K. Starke 1 —<br />
1 Institut für Experimentalphysik, Freie Universität Berlin — 2 Institut<br />
für Festkörperforschung (IFF), Forschungszentrum Jülich — 3 MAX-Lab,<br />
Lund University, Sweden<br />
We compare experimental angle-resolved photoemission investigations<br />
with first-principles DFT calculations, including spin-orbit interaction,<br />
of Gd(0001) and O/Gd(0001) surface states. For both systems, experimental<br />
and theoretical results reveal that the energy dispersion of the<br />
surface state depends on the relative orientation of the propagation direction<br />
of the electrons and the spin-quantisation axis. While for the clean<br />
Gd surface only the majority state of the exchange split surface states is<br />
occupied, both the minority and majority states appear below the Fermi<br />
level upon oxygen adsorption. Angle-resolved photoemission experiments<br />
on these two surface states directly demonstrate that the observed effect<br />
on the energy dispersion is caused by spin-orbit interaction. In addition,<br />
oxygen adsorption leads to a modified near-surface electronic structure<br />
that results in an increased spin-orbit interaction.<br />
MA 4.10 Mo 12:30 H22<br />
Rashba splitting of surface states at Gd(0001) surfaces — •G.<br />
Bihlmayer 1 , O. Krupin 2 , J.E. Prieto 2 , S. Blügel 1 , G. Kaindl 2 ,<br />
and K. Starke 2 — 1 Institut für Festkörperforschung, Forschungszentrum<br />
Jülich, Germany — 2 Fachbereich Physik, Freie Universität Berlin,<br />
Germany<br />
By angle resolved photoemission measurements on clean and O-covered<br />
Gd(0001) surfaces a dependence of the dispersion of the surface state on<br />
the magnetization direction of the sample was found. We present results<br />
of first-principles calculations showing that this behavior is a direct<br />
manifestation of a relativistic effect, known as Rashba effect in the field<br />
of semiconductor heterostructures. Normally, this tiny effect is difficult<br />
to observe directly or to access with ab-inito calculations, but on some<br />
metal surfaces it is large; we discuss, why the strength of this ’spin-orbit<br />
splitting’ is big for some states (O/Gd(0001)) and rather small for others<br />
(clean Gd(0001)). Our results are in good quantitative agreement with<br />
measured data. The differences to the nonmagnetic surfaces, on which<br />
this effect also has been observed (e.g. Au(111)) are addressed. Other<br />
systems, on which this effect could be observed experimentally are suggested.<br />
MA 4.11 Mo 12:45 H22<br />
Theoretical study of magnetic and spectroscopic properties of<br />
supported transition metal clusters — •J. Minar 1 , H. Ebert 1 ,<br />
V. Popescu 1 , I. Cabria 2 , R. Zeller 2 , and P.H. Dederichs 2 —<br />
1 Dep. Chemie/Phys. Chemie, Universty of Munich, Muenchen, Germany<br />
— 2 Forschungszentrum Juelich, Juelich<br />
Magnetic clusters receive recently a lot of attention in academic but<br />
also in technological research. On the one hand side, the interest is caused<br />
by the fact that clusters provide a bridge between atoms and bulk material<br />
often showing quite peculiar properties. On the other hand, the<br />
ongoing need for miniaturizing, in particular in data storage technology,<br />
leads to smaller and smaller functional units leading finally to small clusters.<br />
In this work the fully relativistic spin-polarized KKR method has<br />
been used to study the magnetic and spectroscopic properties for supported<br />
clusters. For clusters supported on a transition metal substrate it<br />
is shown that the magnetic properties depend on many different parameters<br />
as substrate type, cluster size and shape and so on. This applies especially<br />
if one considers properties that are caused by spin-orbit coupling<br />
as the X-ray circular dichroism. In line with recent experimental findings<br />
a very pronounced magnetic circular dichroism in X-ray absorption is<br />
found for Co-clusters on Pt(111). The results for the MCXD spectra and<br />
their connection with the spin, orbital and spin dipolar moments will be<br />
discussed on the basis of the so-called sum rules.<br />
MA 4.12 Mo 13:00 H22<br />
Electronic structure versus spin polarization in NiMnSb —<br />
•Jürgen Braun, Hristo Kolev, Georgi Rangelov, and Markus<br />
Donath — Physikalisches Institut, Westfälische Wilhelms-Universität<br />
Münster, Wilhelm-Klemm Str. 10, 48149 Münster<br />
Half-metallic semi Heusler alloys like NiMnSb have been ascribed<br />
promising materials for spintronic devices, because of a theoretically<br />
predicted high spin polarization at the Fermi level. Unfortunately, from<br />
our spin-resolved Appearance Potential Spectroscopy (SRAPS) measurements<br />
an unexpected low spin polarization was observed. This result is<br />
in agreement with experimental findings from other groups but yet not<br />
understood. To investigate the physical origin of this discrepancy we<br />
performed a quantitative theoretical analysis of the experimental data.<br />
Using a fully relativistic theory of SRAPS, which describes the measured<br />
spectra as the self-convolution of the matrix-element weighted, orbitallyresolved<br />
unoccupied density of states, we are able to present a quantitative<br />
explanation for the small spin polarization experimentally found in<br />
(semi) Heusler alloys.