404 research outputs found
Analysis of heterogeneous collaboration in the German research system with a focus on nanotechnology
The German research system is functionally differentiated into various institutional pillars, most importantly the university system and the extra-university sector including institutes of the Helmholtz Association, the Max Planck Society, the Leibniz Association and the Fraunhofer Society. While the research organisations heterogeneous institutional profiles are widely regarded as a key strength of the German research landscape, tendencies towards segmentation and institutional self-interests have increasingly impeded inter-institutional collaboration. Yet, in young and highly dynamic fields, many research breakthroughs are stimulated at the intersection of established scientific disciplines and across fundamental and applied technological research. Therefore, inter-institutional collaboration is an important dimension of the performance of the German research system. There is tension between the need for effective inter-institutional collaboration on the one hand, and the governance structures in the public research sector on the other hand. The paper presents preliminary results of an ongoing DFG project on collaborations between the various research institutions in Germany, particularly in the field of nano S&T. It introduces key facts of the German research system including institutional dynamics between 1990 and 2002. It discusses rationales for cooperative research relationships and elaborates on institutional factors that either facilitate or interfere with the transfer of knowledge and expertise between research organizations. For this purpose, the paper refers to a governance cube as a heuristic tool that captures three institutional dimensions which are important in facilitating heterogeneous research cooperation. --
Magnetically hindered chain formation in transition-metal break junctions
Based on first-principles calculations, we demonstrate that magnetism impedes
the formation of long chains in break junctions. We find a distinct softening
of the binding energy of atomic chains due to the creation of magnetic moments
that crucially reduces the probability of successful chain formation. Thereby,
we are able to explain the long standing puzzle why most of the
transition-metals do not assemble as long chains in break junctions and provide
thus an indirect evidence that in general suspended atomic chains in
transition-metal break junctions are magnetic.Comment: 5 pages, 3 figure
Competing magnetic anisotropies in atomic-scale junctions
Using first-principles calculations, we study the magnetism of 5d
transition-metal atomic junctions including structural relaxations and
spin-orbit coupling. Upon stretching monatomic chains of W, Ir, and Pt
suspended between two leads, we find the development of strong magnetism and
large values of the magnetocrystalline anisotropy energy (MAE) of up to 30 meV
per chain atom. We predict that switches of the easy magnetization axis of the
nanocontacts upon elongation should be observable by ballistic anisotropic
magnetoresistance measurements. Due to the different local symmetry, the
contributions to the MAE of the central chain atoms and chain atoms in the
vicinity of the leads can have opposite signs which reduces the total MAE. We
demonstrate that this effect occurs independent of the chain length or geometry
of the electrodes.Comment: accepted for publication in Phys. Rev.
Thermodynamic Analogy for Structural Phase Transitions
We investigate the relationship between ground-state (zero-temperature)
quantum phase transitions in systems with variable Hamiltonian parameters and
classical (temperature-driven) phase transitions in standard thermodynamics. An
analogy is found between (i) phase-transitional distributions of the
ground-state related branch points of quantum Hamiltonians in the complex
parameter plane and (ii) distributions of zeros of classical partition
functions in complex temperatures. Our approach properly describes the first-
and second-order quantum phase transitions in the interacting boson model and
can be generalized to finite temperatures.Comment: to be published by AIP in Proc. of the Workshop "Nuclei and
Mesoscopic Physics" (Michigan State Univ., Oct 2004); 10 pages, 3 figure
Learning from errors: effects of teachers training on studentsâ attitudes towards and their individual use of errors
Constructive error handling is considered an important factor for individual learning processes. In a quasi-experimental study with Grades 6 to 9 students, we investigate effects on students’ attitudes towards errors as learning opportunities in two conditions: an error-tolerant classroom culture, and the first condition along with additional teaching of strategies for analyzing errors. Our findings show positive effects of the error-tolerant classroom culture on the affective level, whereas students are not influenced by the cognitive support. There is no evidence for differential effects for student groups with different attitudes towards errors
Dzyaloshinskii-Moryia interaction at an antiferromagnetic interface: first-principles study of FeIr bilayers on Rh(001)
We study the magnetic interactions in atomic layers of Fe and 5d
transition-metals such as Os, Ir, and Pt on the (001) surface of Rh using
first-principles calculations based on density functional theory. For both
stackings of the 5d-Fe bilayer on Rh(001) we observe a transition from an
antiferromagnetic to a ferromagnetic nearest-neighbor exchange interaction upon
5d band filling. In the sandwich structure 5d/Fe/Rh(001) the nearest neighbor
exchange is significantly reduced. For FeIr bilayers on Rh(001) we consider
spin spiral states in order to determine exchange constants beyond nearest
neighbors. By including spin-orbit coupling we obtain the Dzyaloshinskii-Moriya
interaction (DMI). The magnetic interactions in Fe/Ir/Rh(001) are similar to
those of Fe/Ir(001) for which an atomic scale spin lattice has been predicted.
However, small deviations between both systems remain due to the different
lattice constants and the Rh vs. Ir surface layers. This leads to slightly
different exchange constants and DMI and the easy magnetization direction
switches from out-of-plane for Fe/Ir(001) to in-plane for Fe/Ir/Rh(001).
Therefore a fine tuning of magnetic interactions is possible by using single 5d
transition-metal layers which may allow to tailor antiferromagnetic skyrmions
in this type of ultrathin films. In the sandwich structure Ir/Fe/Rh(001) we
find a strong exchange frustration due to strong hybridization of the Fe layer
with both Ir and Rh which drastically reduces the nearest-neighbor exchange.
The energy contribution from the DMI becomes extremely large and DMI beyond
nearest neighbors cannot be neglected. We attribute the large DMI to the low
coordination of the Ir layer at the surface. We demonstrate that higher- order
exchange interactions are significant in both systems which may be crucial for
the magnetic ground state
Conductance fingerprints of non-collinear magnetic states in single atom contacts: a first-principles Wannier functions study
We present a first-principles computational scheme for investigating the
ballistic transport properties of one-dimensional nanostructures with
non-collinear magnetic order. The electronic structure is obtained within
density functional theory as implemented in the full-potential linearized
augmented plane-wave (FLAPW) method and mapped to a tight-binding like
transport Hamiltonian via non-collinear Wannier functions. The conductance is
then computed based on the Landauer formula using the Green's function method.
As a first application we study the conductance between two ferromagnetic Co
monowires terminated by single Mn apex atoms as a function of Mn-Mn separation.
We vary the Mn-Mn separation from the contact (about 2.5 to 5 {\AA}) to the far
tunneling regime (5 to 10 {\AA}). The magnetization direction of the Co
electrodes is chosen either in parallel or antiparallel alignment and we allow
for different spin configurations of the two Mn spins. In the tunneling and
into the contact regime the conductance is dominated by --states.
In the close contact regime (below 3.5 {\AA}) there is an additional
contribution for a parallel magnetization alignment from the - and
-states which give rise to an increase of the magnetoresistance as it
is absent for antiparallel magnetization. If we allow the Mn spins to relax a
non-collinear spin state is formed close to contact. We demonstrate that the
transition from a collinear to such a non-collinear spin structure as the two
Mn atoms approach leaves a characteristic fingerprint in the distance-dependent
conductance and magnetoresistance of the junction. We explain the effect of the
non-collinear spin state on the conductance based on the spin-dependent
hybridization between the -states of the Mn spins and their coupling
to the Co electrodes.Comment: 13 pages, 5 figure
Stability and magnetic properties of Fe double-layers on Ir (111)
We investigate the interplay between the structural reconstruction and the
magnetic properties of Fe doublelayers on Ir (111)-substrate using
first-principles calculations based on density functional theory and mapping of
the total energies on an atomistic spin model. We show that, if a second Fe
monolayer is deposited on Fe/Ir (111), the stacking may change from hexagonal
close-packed to bcc (110)-like accompanied by a reduction of symmetry from
trigonal to centered rectangular. Although the bcc-like surface has a lower
coordination, we find that this is the structural ground state. This
reconstruction has a major impact on the magnetic structure. We investigate in
detail the changes in the magnetic exchange interaction, the magnetocrystalline
anisotropy, and the Dzyaloshinskii Moriya interaction depending on the stacking
sequence of the Fe double-layer. Based on our findings, we suggest a new
technique to engineer Dzyaloshinskii Moriya interactions in multilayer systems
employing symmetry considerations. The resulting anisotropic
Dzyaloshinskii-Moriya interactions may stabilize higher-order skyrmions or
antiskyrmions
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