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Localized Magnetic States in Three Dimensional Dirac Solids
Uppsala University, Disciplinary Domain of Science and Technology, Physics, Department of Physics and Astronomy, Materials Theory. Sharif Univ Technol, Dept Phys, Tehran 111559161, Iran..
Sharif Univ Technol, Dept Phys, Tehran 111559161, Iran..
Sharif Univ Technol, Dept Phys, Tehran 111559161, Iran.;Sharif Univ Technol, Ctr Excellence Complex Syst & Condensed Matter CS, Tehran 1458889694, Iran..
2016 (English)In: Journal of the Physical Society of Japan, ISSN 0031-9015, E-ISSN 1347-4073, Vol. 85, no 1, 014707Article in journal (Refereed) Published
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Abstract [en]

Formation of localized magnetic states in a metallic host is a classic problem of condensed matter physics formalized by P. W. Anderson within the so called single impurity Anderson model (SIAM). The general picture in a host of a simple one-band metal is that a large Hubbard U in the impurity orbital is pre-requisite for the formation of localized magnetic states. In recent years three dimensional (3D) Dirac solids have emerged the hallmark of which is strong spin-orbit interaction. In this work we show that such a strong spin-orbit interaction allows to form localized magnetic states even with small values of Hubbard U. This opens up the fascinating possibility of forming magnetic states with s or p orbital impurities - different from traditional paradigms of d or f orbital based magnetic moments.

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2016. Vol. 85, no 1, 014707
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URN: urn:nbn:se:uu:diva-275538DOI: 10.7566/JPSJ.85.014707ISI: 000367710300022OAI: oai:DiVA.org:uu-275538DiVA: diva2:900652
Available from: 2016-02-04 Created: 2016-02-04 Last updated: 2017-11-30Bibliographically approved

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Mashkoori, Mahdi

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