478 research outputs found
Magnetization reversal and nonexponential relaxation via instabilities of internal spin waves in nanomagnets
A magnetic particle with atomic spins ordered in an unstable direction is an
example of a false vacuum that decays via excitation of internal spin waves.
Coupled evolution of the particle's magnetization (or the vacuum state) and
spin waves, considered in the time-dependent vacuum frame, leads to a peculiar
relaxation that is very fast at the beginning but slows down to a
nonexponential long tail at the end. The two main scenarios are linear and
exponential spin-wave instabilities. For the former, the longitudinal and
transverse relaxation rates have been obtained analytically. Numerical
simulations show that the particle's magnetization strongly decreases in the
middle of reversal and then recovers.Comment: 6 EPL pages, 4 figure
Quantum Dynamics of a Nanomagnet driven by Spin-Polarized Current
A quantum theory of magnetization dynamics of a nanomagnet as a sequence of
scatterings of each electron spin with the macrospin state of the magnetization
results in each encounter a probability distribution of the magnetization
recoil state associated with each outgoing state of the electron. The quantum
trajectory of the magnetization contains the average motion tending in the
large spin limit to the semi-classical results of spin transfer torque and the
fluctuations giving rise to a quantum magnetization noise and an additional
noise traceable to the current noise.Comment: 4 pages, 4 figure
Evidence for spin-flip scattering and local moments in dilute fluorinated graphene
The issue of whether local magnetic moments can be formed by introducing
adatoms into graphene is of intense research interest because it opens the
window to fundamental studies of magnetism in graphene, as well as of its
potential spintronics applications. To investigate this question we measure, by
exploiting the well-established weak localization physics, the phase coherence
length L_phi in dilute fluorinated graphene. L_phi reveals an unusual
saturation below ~ 10 K, which cannot be explained by non-magnetic origins. The
corresponding phase breaking rate increases with decreasing carrier density and
increases with increasing fluorine density. These results provide strong
evidence for spin-flip scattering and points to the existence of adatom-induced
local magnetic moment in fluorinated graphene. Our results will stimulate
further investigations of magnetism and spintronics applications in
adatom-engineered graphene.Comment: 9 pages, 4 figures, and supplementary materials; Phys. Rev. Lett. in
pres
Kondo Temperature in Multilevel Quantum Dots
We develop a general method to evaluate the Kondo temperature in a multilevel
quantum dot that is weakly coupled to conducting leads. Our theory reveals that
the Kondo temperature is strongly enhanced when the intradot energy-level
spacing is comparable to or smaller than the charging energy. We propose an
experiment to test our result, which consists of measuring the size-dependence
of the Kondo temperature.Comment: 4 pages, 1 figure and supplementary material. Revised and improved
version, to appear in Phys. Rev. Let
Analysis of the Kondo effect in ferromagnetic atomic-sized contacts
Atomic contacts made of ferromagnetic metals present zero-bias anomalies in
the differential conductance due to the Kondo effect. These systems provide a
unique opportunity to perform a statistical analysis of the Kondo parameters in
nanostructures since a large number of contacts can be easily fabricated using
break-junction techniques. The details of the atomic structure differ from one
contact to another so a large number of different configurations can be
statistically analyzed. Here we present such a statistical analysis of the
Kondo effect in atomic contacts made from the ferromagnetic transition metals
Ni, Co and Fe. Our analysis shows clear differences between materials that can
be understood by fundamental theoretical considerations. This combination of
experiments and theory allow us to extract information about the origin and
nature of the Kondo effect in these systems and to explore the influence of
geometry and valence in the Kondo screening of atomic-sized nanostructures.Comment: 17 pages, 11 figure
Comment on "Isotope effect in multi-band and multi-channel attractive systems and inverse isotope effect in iron-based superconductors" by T. Yanagisawa, et al
In a recent paper Yanagisawa et al. [1] claim from a theoretical analysis of
a multi-channel multi-band superconductor model that an inverse isotope
exponent on the superconducting transition temperature Tc can be realized in
iron-based superconductors. Simultaneously, a subgroup of the authors of Ref. 1
performed the corresponding isotope effect experiment on (Ba, K)Fe2As2 by
investigating the iron isotope exchange effect on Tc [2]. In accordance with
their theoretical analysis they indeed report an unusually large sign reversed
isotope exponent of {\alpha} \simeq -0.18(3) which is in strong contrast to
previous experiments on the nominally same system with the same composition in
Ba, K content, namely Ba0.6K0.4Fe2As2 [3], where the exponent was determined to
be {\alpha} \simeq 0.37(3). This conflict remains unsolved until now with the
exception of Ref. 4 where the iron isotope exponent has been determined for
FeSe. In accordance with the results of Ref. 3 a large positive isotope
exponent has been seen thus questioning the outcome of Ref. 1 and implicitly
the findings of Ref. 2. Here, we do not comment on the controversial
experimental situation but address the theoretical analysis of Ref. 1, where a
variety of misleading assumptions have led to the conclusion that a sign
reversed isotope exponent can be realized in a multi-band and multi-channel
attractive model for iron based superconductors.Comment: 4 page
Magnetic reordering in the vicinity of a ferromagnetic/antiferromagnetic interface
The magnetic arrangement in the vicinity of the interface between a
ferromagnet and an antiferromagnet is investigated, in particular its
dependence on the exchange couplings and the temperature. Applying a Heisenberg
model, both sc(001) and fcc(001) lattices are considered and solved by a mean
field approximation. Depending on the parameter values a variety of different
magnetic configurations emerge. Usually the subsystem with the larger ordering
temperature induces a magnetic order into the other one (magnetic proximity
effect). With increasing temperature a reorientation of the magnetic
sublattices is obtained. For coupled sc(001) systems both FM and AFM films are
disturbed from their collinear magnetic order, hence exhibit a similar
behavior. This symmetry is absent for fcc(001) films which, under certain
circumstances, may exhibit two different critical temperatures. Analytical
results are derived for simple bilayer systems.Comment: accepted for publication in Eur. Phys. J.
Fourier transform spectroscopy of d-wave quasiparticles in the presence of atomic scale pairing disorder
The local density of states power spectrum of optimally doped
BiSrCaCuO (BSCCO) has been interpreted in terms of
quasiparticle interference peaks corresponding to an "octet'' of scattering
wave vectors connecting k-points where the density of states is maximal. Until
now, theoretical treatments have not been able to reproduce the experimentally
observed weights and widths of these "octet'' peaks; in particular, the
predominance of the dispersing "q'' peak parallel to the Cu-O bond
directions has remained a mystery. In addition, such theories predict
"background'' features which are not observed experimentally. Here, we show
that most of the discrepancies can be resolved when a realistic model for the
out-of-plane disorder in BSCCO is used. Weak extended potential scatterers,
which are assumed to represent cation disorder, suppress large-momentum
features and broaden the low-energy "q''-peaks, whereas scattering at order
parameter variations, possibly caused by a dopant-modulated pair interaction
around interstitial oxygens, strongly enhances the dispersing "q''-peaks.Comment: 7 pages, 3 figure
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