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000016691 0247_ $$2DOI$$a10.1103/PhysRevLett.107.106601
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000016691 084__ $$2WoS$$aPhysics, Multidisciplinary
000016691 1001_ $$0P:(DE-Juel1)143607$$aWeischenberg, J.$$b0$$uFZJ
000016691 245__ $$aAb Initio Theory of the Scattering-Independent Anomalous Hall Effect
000016691 260__ $$aCollege Park, Md.$$bAPS$$c2011
000016691 300__ $$a106601
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000016691 440_0 $$04925$$aPhysical Review Letters$$v107$$x0031-9007$$y10
000016691 500__ $$3POF3_Assignment on 2016-02-29
000016691 500__ $$aWe gratefully acknowledge Julich Supercomputing Centre for computing time and funding under the HGF-YIG Programme VH-NG-513. J.S. was supported under Grant Nos. ONR-N000141110780 and NSF-DMR-1105512 and by the Research Corporation Cottrell Scholar Award.
000016691 520__ $$aWe report on first-principles calculations of the side-jump contribution to the anomalous Hall conductivity (AHC) directly from the electronic structure of a perfect crystal. We implemented our approach for a short-range scattering disorder model within the density functional theory and computed the full scattering-independent AHC in elemental bcc Fe, hcp Co, fcc Ni, and L1(0) FePd and FePt alloys. The full AHC thus calculated agrees systematically with experiment to a degree unattainable so far, correctly capturing the previously missing elements of side-jump contributions, hence paving the way to a truly predictive theory of the anomalous Hall effect and turning it from a characterization tool to a probing tool of multiband complex electronic band structures.
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000016691 7001_ $$0P:(DE-Juel1)130643$$aFreimuth, F.$$b1$$uFZJ
000016691 7001_ $$0P:(DE-HGF)0$$aSinova, J.$$b2
000016691 7001_ $$0P:(DE-Juel1)130548$$aBlügel, S.$$b3$$uFZJ
000016691 7001_ $$0P:(DE-Juel1)VDB37182$$aMokrousov, Y.$$b4$$uFZJ
000016691 773__ $$0PERI:(DE-600)1472655-5$$a10.1103/PhysRevLett.107.106601$$gVol. 107, p. 106601$$p106601$$q107<106601$$tPhysical review letters$$v107$$x0031-9007$$y2011
000016691 8567_ $$uhttp://dx.doi.org/10.1103/PhysRevLett.107.106601
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