Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
Plenarvorträge - DPG-Tagungen
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Magnetismus Donnerstag<br />
additional weak interaction along the legs is treated in mean field approximation.<br />
Moessbauer spectroscopy on the Fe compound revealed a<br />
temperature dependent electric field gradient (EFG) due to crystal field<br />
splitting and prove a Fe(II) S=2 configuration. No magnetic order is<br />
found down to 2K.<br />
MA 21.6 Do 11:30 H22<br />
ESR analysis of the cyclic cluster [Na@Fe6(tea)6]·ClO4·2MeOH<br />
— •Ilka Keilhauer 1 , Bernd Pilawa 1 , Danira Marinov 2 , Arthur<br />
Grupp 3 , and Stefan Knorr 3 — 1 Physikalisches Institut, Universität<br />
Karlsruhe (TH), D-76128 — 2 Anorganische Chemie, LMU, D-81377<br />
München — 3 2. Physikalisches Institut, Universität Stuttgart,D-70550<br />
Stuttgart<br />
The six Fe III -ions of Na@Fe6(tea)6 (1) are antiferromagnetically coupled.<br />
The magnetic anisotropy can be analysed by ESR measurements.<br />
The crystal structure of (1) is triclinic with two magnetically nonequivalent<br />
Fe6 clusters per unit cell. This gives rise to complicated spectra<br />
composed of the resonances of the two clusters X and Y. It will be shown<br />
that the splittings of the first excited states S=1,2 and 3 and the orientation<br />
of the molecular symmetry axes can be determined for both clusters<br />
by the analysis of the ESR spectra taken at 7K and 20K. The parameters<br />
of the single ion on-site anisotropy are d/kB=−0.2875±0.0023K and<br />
d/kB=−0.2921±0.0035K, respectively.<br />
The relative angle between the cluster axes of 69.7 ◦ ±1 ◦ determined at<br />
low temperature deviates considerably from the room temperature value<br />
of 54 ◦ . This might indicate a structural phase transition which can be<br />
caused by the temperature dependent motion of the ClO4 tetraeders.<br />
MA 21.7 Do 11:45 H22<br />
1 H-NMR on Fe2(hpdta), Fe4(hpdta)2 and Fe6(hpdta)3 clusters<br />
— •Roland Leppin and Bernd Pilawa — Physikalisches Institut,<br />
Universität Karlsruhe (TH)<br />
1 H-NMR measurements on cyclic Fe6 clusters have shown the importance<br />
of the energy level scheme for the nuclear relaxation. The investigation<br />
of the Fe2(hpdta) dimer is an interesting approach for a better<br />
understanding of the spindynamics, as it can be used as a building block<br />
MA 22 Spinabhängiger Transport I<br />
for more complex clusters like the Fe4(hpdta)2 and Fe6(hpdta)3 systems,<br />
where the metal ions form a square and roof-like structure, respectively.<br />
The 1H T −1<br />
1 rate measurements at 52 MHz in a magnetic field of 1.2<br />
T show differences between the systems. For the Fe2 dimer, the T −1<br />
1 rate<br />
increases monotonously. For Fe4 it starts at a comparatively high value<br />
at low temperatures, goes down to a minimum around 15 K and increases<br />
again with increasing temperature. For the Fe6 sample there is a broad<br />
maximum around 30 K which reminds the results obtained for the cyclic<br />
Fe6(tea)6 samples.<br />
MA 21.8 Do 12:00 H22<br />
Magnetic Resonance Spectroscopic Studies of Magnetization<br />
Relaxation in Single-Crystalline Mn12Ac — •Joris van<br />
Slageren 1 , Suriyakan Vongtragool 1 , Nadeschda Kirchner 1 ,<br />
Martin Dressel 1 , Alexander Mukhin 2 , and Boris Gorshunov 2<br />
— 1 1. Physikalisches Institut, Universität Stuttgart, Stuttgart, Germany<br />
— 2 General Physics Institute, Russian Academy of Sciences, Moscow,<br />
Russia<br />
New, spectroscopic experiments on the magnetization relaxation of the<br />
single molecule magnet Mn12Ac are presented. These studies were performed<br />
using frequency domain magnetic resonance spectroscopy on single<br />
crystalline samples. Special attention is paid to the consequences of<br />
the known distribution of zero-field splitting parameters on the relaxation<br />
dynamics. It is also shown, that the resonance spectrum of the<br />
magnetized sample recorded in zero external field has a peculiar shape in<br />
Faraday geometry, due to a combination of the resonance phenomenon<br />
and the Faraday effect. The nonmagnetized sample shows a normal spectral<br />
shape. In this way it is possible to study magnetization relaxation<br />
in zero external field. Finally, we have succeeded in performing selective<br />
magnetodipolar excitations on one side of the potential energy double<br />
well, by using circularly polarized radiation. This offers another possibility<br />
for studying magnetization relaxation in zero external field, which is<br />
not possible when using linearly polarized radiation. These studies are<br />
important to investigate the role of accidental transverse magnetic field<br />
on the relaxation behaviour of single molecule magnets.<br />
Zeit: Donnerstag 12:15–13:00 Raum: H22<br />
MA 22.1 Do 12:15 H22<br />
Imaging tunnel magnetoresistance related to magnetic microdomain<br />
distribution along a La2/3Ca1/3MnO3 grain boundary<br />
— •Wagenknecht Michael 1 , Timo Nachtrab 1 , Markus Turad<br />
1 , Dieter Koelle 1 , Reinhold Kleiner 1 , Jan Boris Philipp 2 ,<br />
and Rudolf Gross 2 — 1 Physikalisches Institut-Experimentalphysik<br />
II, Universität Tübingen, Auf der Morgenstelle 14, D-72076 Tübingen,<br />
Germany — 2 Walther-Meißner-Institut, Bayerische Akademie der<br />
Wissenschaften, Walther-Meißner Straße 8, D-85748 Garching, Germany<br />
We present electrical transport measurements across an artificial grain<br />
boundary in a La2/3Ca1/3MnO3 thin film grown on a 24 ◦ bicrystal SrTiO3<br />
substrate. In the ferromagnetic-metallic phase below Tc ≈ 220K the grain<br />
boundary acts as a tunneling barrier. Applying an in-plane magnetic field<br />
up to 40mT parallel to the grain boundary we observe several discrete<br />
jumps in the magnetoresistance across the barrier. We explain the resistance<br />
steps by formation of microdomains along the grain boundary.<br />
Using low temperature laser scanning microscopy allows us to image the<br />
tunnelling conductance distribution along the grain boundary for the<br />
discrete resistance steps. By this we are able to map the fraction of parallel/antiparallel<br />
aligned microdomains versus magnetic field and to correlate<br />
the domain distribution with the overall resistance across the grain<br />
boundary.<br />
MA 22.2 Do 12:30 H22<br />
Magnetoresistance and resistance relaxation of La0.7Ca0.3MnO3<br />
step-edge junctions in pulsed magnetic fields up to 50 T — •K.<br />
Dörr 1 , N. Kozlova 1 , M. Ziese 2 , M. Kozlov 1 , K.-H. Müller 1 ,<br />
and L. Schultz 1 — 1 IFW Dresden, Postfach 270116, 01171 Dresden<br />
— 2 Division of Superconductivity and Magnetism, University of Leipzig,<br />
Linnéstrasse 5, 04103 Leipzig<br />
The magnetoresistance (MR) of step-edge junctions in La0.7Ca0.3MnO3<br />
films [1] has been investigated in magnetic fields up to 47 T between<br />
4.2 K and 125 K. Step-edge junctions show similar electrical properties<br />
as grain boundaries [1], including the low-field MR attributed to spin-<br />
polarized tunneling. A tendency towards saturation in high fields and a<br />
large hysteresis with pronounced remanent MR are characteristic results.<br />
Time-dependent resistance data R(t) recorded after field pulses of 7 T<br />
follow a logarithmic law for 30 ms < t