000151298 001__ 151298 000151298 005__ 20230426083108.0 000151298 0247_ $$2doi$$a10.1103/PhysRevB.89.014411 000151298 0247_ $$2ISSN$$a0163-1829 000151298 0247_ $$2ISSN$$a1095-3795 000151298 0247_ $$2ISSN$$a1550-235X 000151298 0247_ $$2ISSN$$a0556-2805 000151298 0247_ $$2ISSN$$a1098-0121 000151298 0247_ $$2Handle$$a2128/5846 000151298 0247_ $$2WOS$$aWOS:000332208100003 000151298 0247_ $$2altmetric$$aaltmetric:1768560 000151298 037__ $$aFZJ-2014-01283 000151298 082__ $$a530 000151298 1001_ $$0P:(DE-Juel1)136941$$aCzaja, Philippe$$b0$$eCorresponding author$$ufzj 000151298 245__ $$aAnomalous Hall effect in ferromagnets with Gaussian disorder 000151298 260__ $$aCollege Park, Md.$$bAPS$$c2014 000151298 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s151298 000151298 3367_ $$2DataCite$$aOutput Types/Journal article 000151298 3367_ $$00$$2EndNote$$aJournal Article 000151298 3367_ $$2BibTeX$$aARTICLE 000151298 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000151298 3367_ $$2DRIVER$$aarticle 000151298 500__ $$3POF3_Assignment on 2016-02-29 000151298 520__ $$aUsing 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, L10-FePd, L10-FePt as well as thin bcc Fe(001) films. Within our approach we can transparently decompose the conductivity into intrinsic, side jump, 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. 000151298 536__ $$0G:(DE-HGF)POF2-422$$a422 - Spin-based and quantum information (POF2-422)$$cPOF2-422$$fPOF II$$x0 000151298 536__ $$0G:(DE-Juel1)HITEC-20170406$$aHITEC - Helmholtz Interdisciplinary Doctoral Training in Energy and Climate Research (HITEC) (HITEC-20170406)$$cHITEC-20170406$$x1 000151298 542__ $$2Crossref$$i2014-01-13$$uhttp://link.aps.org/licenses/aps-default-license 000151298 588__ $$aDataset connected to CrossRef, juser.fz-juelich.de 000151298 7001_ $$0P:(DE-Juel1)130643$$aFreimuth, Frank$$b1$$ufzj 000151298 7001_ $$0P:(DE-Juel1)143607$$aWeischenberg, Jürgen$$b2$$ufzj 000151298 7001_ $$0P:(DE-Juel1)130548$$aBlügel, Stefan$$b3$$ufzj 000151298 7001_ $$0P:(DE-Juel1)130848$$aMokrousov, Yuriy$$b4$$ufzj 000151298 77318 $$2Crossref$$3journal-article$$a10.1103/physrevb.89.014411$$bAmerican Physical Society (APS)$$d2014-01-13$$n1$$p014411$$tPhysical Review B$$v89$$x1098-0121$$y2014 000151298 773__ $$0PERI:(DE-600)2844160-6$$a10.1103/PhysRevB.89.014411$$gVol. 89, no. 1, p. 014411$$n1$$p014411$$tPhysical review / B$$v89$$x1098-0121$$y2014 000151298 8564_ $$uhttps://juser.fz-juelich.de/record/151298/files/FZJ-2014-01283.pdf$$yOpenAccess 000151298 8564_ $$uhttps://juser.fz-juelich.de/record/151298/files/FZJ-2014-01283.jpg?subformat=icon-144$$xicon-144$$yOpenAccess 000151298 8564_ $$uhttps://juser.fz-juelich.de/record/151298/files/FZJ-2014-01283.jpg?subformat=icon-180$$xicon-180$$yOpenAccess 000151298 8564_ $$uhttps://juser.fz-juelich.de/record/151298/files/FZJ-2014-01283.jpg?subformat=icon-640$$xicon-640$$yOpenAccess 000151298 909CO $$ooai:juser.fz-juelich.de:151298$$pdnbdelivery$$pVDB$$pdriver$$popen_access$$popenaire 000151298 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)136941$$aForschungszentrum Jülich GmbH$$b0$$kFZJ 000151298 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)130643$$aForschungszentrum Jülich GmbH$$b1$$kFZJ 000151298 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)143607$$aForschungszentrum Jülich GmbH$$b2$$kFZJ 000151298 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)130548$$aForschungszentrum Jülich GmbH$$b3$$kFZJ 000151298 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)130848$$aForschungszentrum Jülich GmbH$$b4$$kFZJ 000151298 9132_ $$0G:(DE-HGF)POF3-529H$$1G:(DE-HGF)POF3-520$$2G:(DE-HGF)POF3-500$$aDE-HGF$$bKey Technologies$$lFuture Information Technology - 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