Magnetic structure and transport properties of noncollinear LaMn 2X2 (X=Ge,Si) systems

Electronic, magnetic, and transport properties of the noncollinear naturally multilayered compounds LaMn2Ge2 and LaMn 2Si2 are addressed by first-principles calculations based on the density-functional theory. At low temperatures, these systems show a magnetic state with the Mn moments ordered in a...

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Autor principal: Di Napoli, S.
Otros Autores: Llois, A.M, Bihlmayer, G., Blügel, S., Alouani, M., Dreyssé, H.
Formato: Capítulo de libro
Lenguaje:Inglés
Publicado: 2004
Acceso en línea:Registro en Scopus
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Registro en la Biblioteca Digital
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024 7 |2 cas  |a germanium, 7440-56-4; lanthanum, 16096-89-2, 7439-91-0; manganese, 16397-91-4, 7439-96-5; silicon, 7440-21-3 
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100 1 |a Di Napoli, S. 
245 1 0 |a Magnetic structure and transport properties of noncollinear LaMn 2X2 (X=Ge,Si) systems 
260 |c 2004 
270 1 0 |m Di Napoli, S.; Departamento de Física, Fac. de Ciencias Exactas Y Naturales, Universidad de Buenos Aires, 1428 Buenos Aires, Argentina 
506 |2 openaire  |e Política editorial 
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520 3 |a Electronic, magnetic, and transport properties of the noncollinear naturally multilayered compounds LaMn2Ge2 and LaMn 2Si2 are addressed by first-principles calculations based on the density-functional theory. At low temperatures, these systems show a magnetic state with the Mn moments ordered in a conical arrangement (spin spiral) with a ferromagnetic coupling along the c axis and an in-plane antiferromagnetic coupling. The magnetic structures are studied by means of the full-potential linearized augmented-plane-wave method within both the generalized-gradient approximation and the local-density approximation. In both compounds, a conical magnetic state is obtained with energies lower than canted and collinear structures. The trends in the experimentally observed magnetic configuration when replacing Ge by Si are discussed. The origin of the experimentally observed inverse giant magnetoresistance in LaMn 2Ge2 is traced back to the presence of many noncollinear low-energy magnetic configurations.  |l eng 
536 |a Detalles de la financiación: RTN 
536 |a Detalles de la financiación: PSSBBD 0370-1972 220 , 409 ( 2000 ). 10.1002/1521-3951(200007)220:13.0.CO;2-P This work was partially funded by UBACyT-X115, the European Research Training Network (RTN) (Contract No. HPRN-CT-2000-00143), the French-Argentinian collaboration program ECOS-SETCIP A00E04, and the German-Argentinian collaboration program DAAD-Fundación Antorchas. A.M.L. belongs to Consejo Nacional de Investigaciones Científicas y Técnicas CONICET (Argentina). 
593 |a Departamento de Física, Fac. de Ciencias Exactas Y Naturales, Universidad de Buenos Aires, 1428 Buenos Aires, Argentina 
593 |a Departamento de Física, Comn. Nac. de Ener. Atómica, Avenida del Libertador 8250, 1429 Buenos Aires, Argentina 
593 |a Inst. F. Festkörperforschung, Forschungszentrum Jülich, D-52425 Jülich, Germany 
593 |a IPCMS-GEMME, UMR 7504 CNRS-ULP, 23 rue du Loess, F-67034 Strasbourg Cedex, France 
690 1 0 |a FERROMAGNETIC MATERIAL 
690 1 0 |a GERMANIUM 
690 1 0 |a LANTHANUM 
690 1 0 |a MANGANESE 
690 1 0 |a SILICON 
690 1 0 |a ARTICLE 
690 1 0 |a CALCULATION 
690 1 0 |a CHEMICAL STRUCTURE 
690 1 0 |a DENSITY FUNCTIONAL THEORY 
690 1 0 |a ELECTRONICS 
690 1 0 |a ENERGY 
690 1 0 |a FERROMAGNETISM 
690 1 0 |a MAGNET 
690 1 0 |a MAGNET STRUCTURE 
690 1 0 |a MAGNETISM 
690 1 0 |a TEMPERATURE 
700 1 |a Llois, A.M. 
700 1 |a Bihlmayer, G. 
700 1 |a Blügel, S. 
700 1 |a Alouani, M. 
700 1 |a Dreyssé, H. 
773 0 |d 2004  |g v. 70  |h pp. 1-10  |k n. 17  |p Phys. Rev. B Condens. Matter Mater. Phys.  |x 01631829  |w (AR-BaUEN)CENRE-397  |t Physical Review B - Condensed Matter and Materials Physics 
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856 4 0 |u https://doi.org/10.1103/PhysRevB.70.174418  |y DOI 
856 4 0 |u https://hdl.handle.net/20.500.12110/paper_01631829_v70_n17_p1_DiNapoli  |y Handle 
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