27 research outputs found
Scattering-Independent Anomalous Nernst Effect in Ferromagnets
Using the full-potential linearized augmented plane-wave method within the
density functional theory, we compute all contributions to the scattering
independent part of the thermoelectric conductivity tensor, namely the
intrinsic contribution and the side-jump contribution. For the ferromagnetic
materials bcc Fe, hcp Co, fcc Ni and L1_0 ordered alloys FePd and FePt, our
investigations of the energy and temperature dependence of the intrinsic and
side-jump contributions show that they are both of equal importance. Overall,
our calculations are able to correctly reproduce the order of magnitude and
sign of the experimentally measured signal, suggesting that the scattering
independent part plays an important role in the anomalous Nernst effect of
ferromagnets.Comment: 5 pages, 2 figures plus supplement, accepted for publication as a
Rapid Communication in Physical Review
Anomalous Hall effect in ferromagnets with Gaussian disorder
Using the Kubo formalism we derived expressions and implemented the method
for calculating the anomalous Hall conductivity (AHC) in ferromagnets with
short-range Gaussian disorder directly from first-principles electronic
structure of the perfect crystal. We used this method to calculate the AHC in
bcc Fe, fcc Co, L1o-FePd, L1o-FePt as well as thin bcc Fe(001) films. Within
our approach we can transparently decompose the conductivity into intrinsic
(IC), side jump (SJ) and intrinsic skew-scattering (ISK) contributions. The
existence of ISK, which originates from asymmetric Mott scattering but is
clearly distinguishable from conventional skew-scattering in that it converges
to a finite value in clean limit, was pointed out by Sinitsyn et al. [Phys.
Rev. B 75, 045315 (2007)]. Here, we collect all contributions to the AHC in
ferromagnets which result in "scattering-independent" AHE in clean limit, and
analyze their relative magnitude from first principles calculations. By
comparing our results to existing experiments we show that the Gaussian
disorder is well suited to model various types of disorder present in real
materials, to some extent including the effect of temperature. In particular,
we show that in addition to intrinsic and side-jump AHE, the intrinsic
skew-scattering can be a major player in determining the magnitude of the AHE
in ferromagnets.Comment: 10 pages, 3 figure
Ab Initio Theory of Scattering-Independent Anomalous Hall Effect
We report on first-principles calculations of the side-jump contribution to
the anomalous Hall conductivity (AHC) directly from the electronic structure of
a perfect crystal. We implemented our approach for a short-range scattering
disorder model within the density functional theory and computed the full
scattering-independent AHC in elemental bcc Fe, hcp Co, fcc Ni, and L1o FePd
and FePt alloys. The full AHC thus calculated agrees systematically with
experiment to a degree unattainable so far, correctly capturing the previously
missing elements of side-jump contributions, hence paving the way to a truly
predictive theory of the anomalous Hall effect and turning it from a
characterization tool to a probing tool of multi-band complex electronic band
structures.Comment: PRL in pres
Anisotropy of spin relaxation and transverse transport in metals
Using first principles methods we explore the anisotropy of the spin
relaxation and transverse transport properties in bulk metals with respect to
the direction of the spin quantization axis in paramagnets or of the
spontaneous magnetization in ferromagnets. Owing to the presence of the
spin-orbit interaction the orbital and spin character of the Bloch states
depends sensitively on the orientation of the spins relative to the crystal
axes. This leads to drastic changes in quantities which rely on interband
mixing induced by the spin-orbit interaction. The anisotropy is particularly
striking for quantities which exhibit spiky and irregular distribution in the
Brillouin zone, such as the spin-mixing parameter or the Berry curvature of the
electronic states. We demonstrate this for three cases: (i) the Elliott-Yafet
spin-relaxation mechanism in paramagnets with structural inversion symmetry;
(ii) the intrinsic anomalous Hall effect in ferromagnets; and (iii) the spin
Hall effect in paramagnets. We discuss the consequences of the pronounced
anisotropic behavior displayed by these properties for spin-polarized transport
applications.Comment: Psi-k Highlight 111 (2012