Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Magnetismus Dienstag<br />
MA 13.107 Di 15:00 Bereich A<br />
Well-Aligned Co-Filled Carbon Nanotubes: Preparation and<br />
Magnetic Properties — •Radinka Kozhuharova 1 , Dieter<br />
Elefant 1 , Andreas Graff 1,2 , Albrecht Leonhardt 1 , Ingolf<br />
Mönch 1 , Thomas Mühl 1 , Manfred Ritschel 1 , Claus M.<br />
Schneider 1,3 , and Stefka Zotova 1 — 1 Leibniz-Institute of Solid<br />
State and Materials Research Dresden, Helmholtzstr. 20, D-01069<br />
Dresden — 2 present address: Max Planck Institute of Microstructure<br />
Physics, Halle — 3 present address: Research Center Jülich GmbH,<br />
D-52425 Jülich<br />
Carpet-like flakes (area < 3mm x 3mm; thickness < 500nm) of wellaligned<br />
Co-filled multi walled carbon nanotubes were grown by decomposition<br />
of cobaltocene. The product was analysed by scanning (FE-SEM,<br />
Leo 1530)- and transmission (TEM, Tecnai F30 with GIF200)- electron<br />
microscopy. The phase composition and the crystalline structure were<br />
determined by X-ray difffraction and selected area electron diffraction.<br />
Using alternating gradient magnetometry the ferromagnetic behaviour<br />
of the filled nanotubes was investigated. The nanotubes have outer diameter<br />
of 50-90nm and diameter of the metal core of 15-30nm. They are<br />
discontinuously filled with fcc Co nanowires having a length of up to a few<br />
micrometers. Magnetometry measurements show a weak uniaxial magnetic<br />
anisotropy with the easy axis along the nanowires. A high coercivity<br />
of about 59mT at room temperature is observed, which is significantly<br />
higher than in bulk Co.<br />
MA 13.108 Di 15:00 Bereich A<br />
PAC-Untersuchungen an amorphen Ferromagnetika — •V. Samokhvalov<br />
1 , F. Schneider 1 , S. Unterricker 1 , M. Dietrich 2 und<br />
die ISOLDE - Collaboration 3 — 1 Institut für Angewandte Physik,<br />
TU Bergakademie Freiberg, D-09596 Freiberg/Sachsen — 2 Technische<br />
Physik, Universität des Saarlandes, D-66041 — 3 CERN, CH-1211 Geneva<br />
23, Switzerland<br />
Amorphe ferromagnetische Materialien, wie z. B. Fe80B20, sind mit<br />
dem Mößbauer-Effekt sehr ausführlich untersucht worden. Mit der Sonde<br />
57 Fe wurden dabei über die Verteilungen der Hyperfeinfelder wesentliche<br />
Aussagen zur Nahordnung in der Umgebung der Eisenatome gewonnen.<br />
Allerdings bereitet die Interpretation der immer vorhandenen<br />
Quadrupolwechselwirkung Probleme. Wir haben amorphes Fe80B20 mit<br />
der Methode PAC (= perturbed angular correlations) und den Sonden<br />
111m Cd, 111 In( 111 Cd) und 62 Zn( 62 Cu), die am ISOLDE-Separator mit einer<br />
Energie von 50 keV implantiert wurden, untersucht. Messungen nach<br />
unterschiedlichen Wärmebehandlungen werden vorgestellt und die auftretenden<br />
Feldverteilungen diskutiert.<br />
MA 13.109 Di 15:00 Bereich A<br />
Electronic Structure of Transition-Metal Dicyanamides<br />
Me[N(CN)2]2 (Me = Mn, Fe, Co, Ni, Cu) — •Takács Albert 1 ,<br />
Chiuzbăian Sorin 1 , Crainic Traian Ionica 1 , Demchenko D.<br />
O. 2 , Filkenstein L.D. 3 , Galakhov V.R. 3 , Kmety Carmen<br />
R. 4 , Kurmaev E. Z. 3 , Liu Amy Y. 2 , Moevs A. 5 , Neumann<br />
Manfred 1 , and Stevensson Knneth L. 6 — 1 Universität Osnabrück<br />
— 2 Department of Physics, Georgetown University, Washington —<br />
3 Institute of Metal Physics, Yekaterinburg — 4 Argonne National<br />
Laboratory, USA — 5 University of Saskatchewan, Canada — 6 Purdue<br />
University Indiana , USA<br />
The electronic structure of Me[N(CN)2]2 (Me=Mn, Fe, Co, Ni, Cu)<br />
molecular magnets has been investigated using x-ray emission spectroscopy<br />
(XES) and x-ray photoelectron spectroscopy (XPS) as well as<br />
theoretical density-functional-based methods. Both theory and experiments<br />
show that the top of the valence band is dominated by Me 3d<br />
bands, while a strong hybridization between C 2p and N 2p states determines<br />
the valence band electronic structure away from the top. The<br />
2p contributions from non-equivalent nitrogen sites have been identified<br />
using resonant inelastic x-ray scattering spectroscopy with the excitation<br />
energy tuned near the N 1s threshold. The binding energy of the Me 3d<br />
bands and the hybridization between N 2p and Me 3d states both increase<br />
in going across the row from Me = Mn to Me = Cu. Calculations<br />
indicate that the ground-state magnetic ordering is largely dependent on<br />
the occupation of the metal 3d shell and that structural differences in the<br />
superexchange pathways for different compounds play a secondary role.<br />
MA 13.110 Di 15:00 Bereich A<br />
X-ray magnetic and natural circular dichroism above and below<br />
the Verwey transition in a Fe3O4 single crystal — •S. Gold, E.<br />
Goering, and G. Schütz — Max-Planck-Institut für Metallforschung,<br />
70569 Stuttgart<br />
Recently Fe3O4 has become an intensive studied system, due to its<br />
proposed and experimentally observed high spin polarization at the fermi<br />
energy and its related applicability in future spin electronic devices. In<br />
addition, at the so called Verwey transition, which has been investigated<br />
over many decades, a dramatic change in the electrical resistivity appears.<br />
We show detailed X-ray magnetic circular dichroism (XMCD) experiments<br />
at 1T applied magnetic field performed above and below the<br />
Verwey transition and along different crystallographic directions ((100),<br />
(110) and (111)). We have observed very small changes in the XMCDspectra<br />
of this cubic system as a function of temperature and orientation,<br />
which has not been observed before in a cubic system. Changes in the<br />
differences of the projected orbital moments along the given crystallographic<br />
axes above and below the Verwey transition are consistent to the<br />
observed change of the easy axis. In addition a directly observable and<br />
unexpected large nonmagnetic natural circular dichroism (XNCD) signal<br />
has been observed by flipping the helicity of the synchrotron beam. This<br />
is a sign of an unexpected local non centro symmetric charge distribution<br />
at the 3d transition metal site. Our investigations give new insight to the<br />
microscopic ground state and excited state properties of Fe3O4 related<br />
to the magnetic behavior and the Verwey transition.<br />
MA 13.111 Di 15:00 Bereich A<br />
First principles electronic structure of spinel LiCr2O4: A<br />
possible half-metal? — •Markus Lauer 1 , Roser Valenti 2 ,<br />
H.C. Kandpal 3 , and Ram Seshadri 4 — 1 Fachrichtung Theoretische<br />
Physik, Universitaet des Saarlandes, Postfach 15 11 50, D-66041<br />
Saarbruecken — 2 Institut fuer Theoretische Physik, Universitaet<br />
Frankfurt, Robert-Mayer-Strasse 8, D-60043 Frankfurt — 3 Institut<br />
fuer Anorganische Chemie, Universitaet Mainz, Duesberg Weg 10-14,<br />
D-55099 Mainz — 4 Materials Department, University of California,<br />
Santa Barbara, CA 93106 USA<br />
We have employed first-principles electronic structure calculations to<br />
examine the hypothetical oxide spinel LiCr2O4 with the d 2.5 electronic<br />
configuration. The cell and internal (oxygen position) structural parameters<br />
have been obtained for this compound through structural relaxation<br />
in the first-principles framework. Within the one-electron band picture,<br />
we find that LiCr2O4 is magnetic, and a candidate half-metal. The<br />
electronic structure is substantially different from the closely related rutile<br />
half-metal CrO2. Comparisons with superconducting LiTi2O4, heavy<br />
fermion LiV2O4 and charge-ordering LiMn2O4 suggest the effectiveness<br />
of a nearly-rigid band picture involving simple shifts of the position of<br />
EF in these very different materials. Comparisons are also made with the<br />
electronic structure of ZnV2O4, a correlated insulator that undergoes a<br />
structural and antiferromagnetic phase transition.<br />
MA 13.112 Di 15:00 Bereich A<br />
Magnetic properties in chromium-chalcogenide systems —<br />
•Diana Benea 1 , Hubert Ebert 1 , Wolfgang Bensch 2 , and<br />
Zhong-Le Huang 2 — 1 Chemistry Department, University of Munich,<br />
Butenandtstr. 5-13, D-81377 München, Germany — 2 Institute for<br />
Inorganic Chemistry, Olshausenstr. 40, D-24098 Kiel, Germany<br />
A theoretical investigation of magnetic properties of the systems<br />
Cr1+x(Se,Te)2 and (Cr,Ti)1+xTe2 is presented. The crystallographic structure<br />
of these compounds was refined in the space group P¯3m1 with four<br />
crystallographically different sites for both metal and chalcogen atoms.<br />
The chalcogen layers are fully occupied, whilst in the metal layer there<br />
are vacancies. The preferential occupation of the metal layers is discussed.<br />
The density of states (DOS) are calculated and the influence of<br />
the Cr/Ti content on the magnetic moments in the system is discussed.<br />
The magnetic behaviour of the systems has been investigated using the<br />
Korringa-Kohn-Rostoker (KKR) band structure method. The disorder in<br />
the system has been accounted for by means of the Coherent Potential<br />
Approximation (CPA).