Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Magnetismus Montag<br />
MA 4 Oberflächenmagnetismus<br />
Zeit: Montag 10:15–13:15 Raum: H22<br />
MA 4.1 Mo 10:15 H22<br />
Structure and magnetism in the MnCu/Cu(001)-c(2x2) and<br />
p2gg-(4x2) surface alloys — •Popescu R. 1 , Meyerheim H.L. 1 ,<br />
Sander D. 1 , Ernst A. 1 , Robach O. 2 , Ferrer S. 2 , Kirschner J. 1 ,<br />
and Bruno P. 1 — 1 MPI für Mikrostrukturphysik, Weinberg 2, 06120<br />
Halle, Germany — 2 ESRF, BP 220, F-38043 Grenoble, France<br />
The two-dimensional magnetic alloy phases formed by deposition of Mn<br />
on Cu(001) in the coverage range between about 0.5 and 1 monolayer<br />
(ML, 1ML=1.53×10 15 atoms/cm 2 ) were investigated by surface x-ray<br />
diffraction (SXRD) and calculations based on the full potential layered<br />
Korringa-Kohn-Rostoker-method implemented within the DFT. While<br />
for the c(2x2) phase formed at 0.5 ML the basic two dimensional alloy<br />
structure model with Mn-atoms replacing every other Cu surface atom<br />
is confirmed (Mn at 0.20± 0.05 ˚Aabove the Cu-layer), in detail an accurate<br />
fit to the 228 reflections (unweighted R≈ 0.07) is only obtained by<br />
taking into account 0.5 ML of Cu atoms above the alloy layer and a fraction<br />
of 20 percent anti-phase domains. The calculations show, that the<br />
magnetic moment of the Mn-atoms is in the 3.8 µB-range independent<br />
of the presence or absence of the Cu-adlayer. The p2gg-(4x2) superstructure<br />
is also characterized by a single MnxCu1−x alloy layer, where the<br />
Mn-concentration (x) is in the range of about 0.8 and the corrugation in<br />
the 0.4˚Arange. The implications of the increased Mn-concentration (x)<br />
on the magnetic moment is discussed.<br />
MA 4.2 Mo 10:30 H22<br />
Magnetism-induced symmetry breaking in photoelectron<br />
diffraction patterns — A. Chassé 1 , •W. Kuch 2 , M. Kotsugi 3 ,<br />
Xingyu Gao 2 , F. Offi 2 , S. Imada 3 , S. Suga 3 , H. Daimon 4 , and<br />
J. Kirschner 2 — 1 Fachbereich Physik, Martin-Luther-Universität<br />
Halle-Wittenberg, D-06099 Halle — 2 Max-Planck-Institut für<br />
Mikrostrukturphysik, Weinberg 2, D-06120 Halle — 3 Graduate School of<br />
Engineering Science, Osaka University, 1–3 Machikaneyama, Toyonaka<br />
560-8531, Japan — 4 Graduate School of Materials Science, Nara<br />
Institute of Science and Technology, Ikoma, Nara 630-0192, Japan, and<br />
CREST-JST, Japan<br />
The influence of spin-polarized photoelectron scattering on the circular<br />
dichroism of 2p3/2 photoelectrons from a ferromagnetic Fe(001)<br />
single crystal surface is studied experimentally and theoretically. Twodimensional<br />
photoelectron intensity angular distribution patterns are<br />
presented. They were recorded at 482.5 eV kinetic energy for both helicities<br />
and for opposite magnetization directions by a display-type spherical<br />
mirror analyzer, which allows simultaneous energy and momentum analysis<br />
of emitted photoelectrons. Multiple-scattering cluster photoelectron<br />
diffraction calculations agree well with the experiment, and reproduce<br />
even fine details of the observed photoelectron diffraction features. A<br />
breaking of symmetry in the circular dichroism of the Fe 2p3/2 photoelectron<br />
angular distribution patterns, related to the presence of magnetic<br />
moments on the Fe atoms, is observed both in the experiment and the<br />
calculation. Backed by theoretical calculations, such measurements bear<br />
the potential to study also systems with complicated spin structures.<br />
MA 4.3 Mo 10:45 H22<br />
Search for structural relaxations upon spin reorientation of<br />
Ni-monolayers by x-ray diffraction and MOKE — •Meyerheim<br />
H. L. 1 , Sander D. 1 , Popescu R. 1 , Robach O. 2 , Ferrer S. 2 , and<br />
Kirschner J. 1 — 1 MPI für Mikrostrukturphysik, Weinberg 2, 06120<br />
Halle, Germany — 2 ESRF, BP 220, F-38043 Grenoble, France<br />
Using surface x-ray diffraction (SXRD) and magneto-optical Kerr effect<br />
(MOKE) measurements, the correlation between adlayer induced<br />
spin reorientation and structure relaxation was investigated in the trilayer<br />
system Ni/Fe/Ni on W(110). While the deposition of one Fe layer<br />
on the Ni film [Ni-thickness: 5, 8 and 10 layers on W(110)] induces a<br />
switching of the easy axis from in-plane to out-of-plane, subsequent deposition<br />
of another Ni layer reverts the easy axis back to in-plane. SXRD<br />
measurements along the reciprocal lattice rods before and after ad-layer<br />
deposition indicate that changes of peak positions, if present at all, must<br />
be below about 5×10 −4 reciprocal lattice units. This corresponds to a<br />
change in the interlayer spacing in the order of 0.002 ˚Aand represents<br />
the limit of the experimental accuracy. The analysis of the peak shapes<br />
does not provide any evidence for film structure in-homogeneities. The<br />
results are discussed in terms of strain and surface contributions to the<br />
magnetic anisotropy.<br />
MA 4.4 Mo 11:00 H22<br />
Convergence in ab initio nonlinar surface magneto-optics of a<br />
Ni/Cu (001) bilayer — •Torsten Andersen 1,2 , Rajeev Ahuja 1 ,<br />
and Wolfgang Hübner 2 — 1 CMT, Dept. of Physics, Uppsala Universitet<br />
(S) — 2 CMT, FB Physik, TU Kaiserslautern (D)<br />
We discuss some aspects of creating a well-converged optical secondharmonic<br />
spectrum from a Ni/Cu bilayer in an ab initio calculation. It<br />
turns out that the convergence of the nonlinear optical susceptibility<br />
requires much more than a simple convergence of the band structure to<br />
1/1000th of the optical energy. Whereas both magnetic and nonmagnetic<br />
symmetries can be resolved using the nonlinear optical intensity at this<br />
level convergence, the symmetries of the individual tensor elements in the<br />
nonlinear optical susceptibility can not. We show by varying the magnetization<br />
direction in the Ni/Cu bilayer that even nonmagnetic tensor<br />
elements require a much higher level of convergence than what is needed<br />
for a simple recognition of the crystal magnetic symmetry. Convergence<br />
is reached by increasing the demands on the band structure, and by a<br />
dense sampling in reciprocal space.<br />
MA 4.5 Mo 11:15 H22<br />
Ab initio study of the magnetic structure of fcc Fe grown on a<br />
Cu(001) substrate — •Bogdan Yavorsky and Ingrid Mertig —<br />
Fachbereich Physik, Martin-Luther-Universität Halle, Deutschland<br />
First-principle total energy studies of Fe films on a Cu (001) substrate<br />
are presented. The films are modeled by symmetric 6Fe/8Cu/6Fe slabs.<br />
Both collinear and noncollinear magnetic configurations are considered.<br />
The effect of the surface relaxation on the total energy of the system is<br />
discussed. It was found that the energy difference between the favored<br />
collinear double-layered antiferromagnetic state and the noncollinear configurations<br />
is reduced by contraction of the Fe sublayer but still remains<br />
positive. The possibility of stable noncollinear magnetic configurations in<br />
the system is discussed.<br />
MA 4.6 Mo 11:30 H22<br />
Spin waves in ultrathin Fe films on Co/Cu(001) — •Markus Etzkorn<br />
1 , P. S. Anil Kumar 1 , W. Tang 1 , R. Vollmer 1 , H. Ibach 2 ,<br />
and J. Kirschner 1 — 1 Max-Planck Institut für Mikrostrukturphysik,<br />
Weinberg 2, 06120 Halle — 2 Institut für Schichten und Grenzflächen<br />
ISG3, Forschungszentrum Jülich, 52425 Jülich<br />
By using spin polarized electron energy loss spectroscopy (SPEELS)<br />
we measured spin-wave excitations in 3 ML Fe on 1 ML Co/Cu(001).<br />
Similar to Co on Cu(001) [1], the spin waves appear as a single peak in<br />
the SPEEL-spectra that can be followed up to the surface Brillouin zone<br />
(SBZ) boundary. The spin-wave energy at the SBZ boundary is about<br />
140 meV. The ratio of spin-wave width to spin-wave energy is about one<br />
for large wave vector spin waves. This suggests that these spin waves<br />
strongly interact with Stoner excitations. In contrast to the case of Co<br />
the dispersion in Fe can not be fitted by a nearest neighbor (NN) Heisenberg<br />
model with a single exchange coupling constant J. In theoretical<br />
calculations [2] the exchange coupling constant of the surface layer of Fe<br />
on Cu(001) is enhanced by about a factor of 2 compared to its bulk value.<br />
Using a NN Heisenberg model with an enhanced surface exchange coupling<br />
constant J1 = 2J a spin-wave stiffness of about 150 meV˚A 2 results<br />
from the fit to the data. This is significantly lower than the value of bulk<br />
bcc Fe (280 meV˚A 2 ).<br />
[1] R. Vollmer, M. Etzkorn, P. S. Anil Kumar, H. Ibach, and J. Kirschner,<br />
Phys. Rev. Lett. 91 (2003) 147201.<br />
[2] M. Pajda, J. Kudrnovsk´y, I. Turek, V. Drchal, and P. Bruno, Phys.<br />
Rev. Lett. 85 (2000) 5424.<br />
MA 4.7 Mo 11:45 H22<br />
Spin-Polarized Scanning Tunneling Spectroscopy of Co Islands<br />
on Cu(111) — •Oswald Pietzsch, Stefan Heinze, André Kubetzka,<br />
Matthias Bode, and Roland Wiesendanger — Institute<br />
of Applied Physics, University of Hamburg, Jungiusstrasse 11, 20355<br />
Hamburg, Germany<br />
Spin-averaged and spin-polarized scanning tunneling spectroscopy at<br />
low temperature was performed on nanometer-scale triangular Co islands<br />
grown epitaxially on Cu(111) in the sub-monolayer coverage regime. Two