Hauptseite > Publikationsdatenbank > Electronic structure of Nd1−xYxMnO3 from Mn K edge absorption spectroscopy and DFT methods > print |
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005 | 20210129215625.0 | ||
024 | 7 | _ | |a 10.1016/j.ssc.2013.11.015 |2 doi |
024 | 7 | _ | |a 0038-1098 |2 ISSN |
024 | 7 | _ | |a 1879-2766 |2 ISSN |
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041 | _ | _ | |a English |
082 | _ | _ | |a 540 |
100 | 1 | _ | |a Balasubramanian, Padmanabhan |0 P:(DE-HGF)0 |b 0 |e Corresponding Author |
245 | _ | _ | |a Electronic structure of Nd1−xYxMnO3 from Mn K edge absorption spectroscopy and DFT methods |
260 | _ | _ | |a New York, NY [u.a.] |c 2014 |b Elsevier Science |
336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1433938085_12152 |2 PUB:(DE-HGF) |
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520 | _ | _ | |a The electronic structure of Nd1−xYxMnO3 (x=0–0.5) is studied using x-ray absorption near-edge structure (XANES) spectroscopy at the Mn K-edge along with the DFT-based LSDA+U and real space cluster calculations. The main edge of the spectra does not show any variation with doping. The pre-edge shows two distinct features which appear well-separated with doping. The intensity of the pre-edge decreases with doping. The theoretical XANES were calculated using real space multiple scattering methods which reproduces the entire experimental spectra at the main edge as well as the pre-edge. Density functional theory calculations are used to obtain the Mn 4p, Mn 3d and O 2p density of states. For x=0, the site-projected density of states at 1.7 eV above Fermi energy shows a singular peak of unoccupied eg (spin-up) states which is hybridized Mn 4p and O 2p states. For x=0.5, this feature develops at a higher energy and is highly delocalized and overlaps with the 3d spin-down states which changes the pre-edge intensity. The Mn 4p DOS for both compositions, show considerable difference between the individual px, py and pz states. For x=0.5, there is a considerable change in the 4p orbital polarization suggesting changes in the Jahn–Teller effect with doping. |
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