Cargando…
Electronic Properties of Fully Strained La(1–x)Sr(x)MnO(3) Thin Films Grown by Molecular Beam Epitaxy (0.15 ≤ x ≤ 0.45)
[Image: see text] The structural, electronic, and magnetic properties of Sr-hole-doped epitaxial La(1–x)Sr(x)MnO(3) (0.15 ≤ x ≤ 0.45) thin films deposited using the molecular beam epitaxy technique on 4° vicinal STO (001) substrates are probed by the combination of X-ray diffraction and various sync...
Autores principales: | , , , , , , , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2022
|
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9088787/ https://www.ncbi.nlm.nih.gov/pubmed/35557663 http://dx.doi.org/10.1021/acsomega.1c06529 |
_version_ | 1784704383489933312 |
---|---|
author | Chaluvadi, Sandeep Kumar Polewczyk, Vincent Petrov, Aleksandr Yu Vinai, Giovanni Braglia, Luca Diez, Jose Manuel Pierron, Victor Perna, Paolo Mechin, Laurence Torelli, Piero Orgiani, Pasquale |
author_facet | Chaluvadi, Sandeep Kumar Polewczyk, Vincent Petrov, Aleksandr Yu Vinai, Giovanni Braglia, Luca Diez, Jose Manuel Pierron, Victor Perna, Paolo Mechin, Laurence Torelli, Piero Orgiani, Pasquale |
author_sort | Chaluvadi, Sandeep Kumar |
collection | PubMed |
description | [Image: see text] The structural, electronic, and magnetic properties of Sr-hole-doped epitaxial La(1–x)Sr(x)MnO(3) (0.15 ≤ x ≤ 0.45) thin films deposited using the molecular beam epitaxy technique on 4° vicinal STO (001) substrates are probed by the combination of X-ray diffraction and various synchrotron-based spectroscopy techniques. The structural characterizations evidence a significant shift in the LSMO (002) peak to the higher diffraction angles owing to the increase in Sr doping concentrations in thin films. The nature of the LSMO Mn mixed-valence state was estimated from X-ray photoemission spectroscopy together with the relative changes in the Mn L(2,3) edges observed in X-ray absorption spectroscopy (XAS), both strongly affected by doping. CTM4XAS simulations at the XAS Mn L(2,3) edges reveal the combination of epitaxial strain, and different MnO(6) crystal field splitting give rise to a peak at ∼641 eV. The observed changes in the occupancy of the e(g) and the t(2g) orbitals as well as their binding energy positions toward the Fermi level with hole doping are discussed. The room-temperature magnetic properties were probed at the end by circular dichroism. |
format | Online Article Text |
id | pubmed-9088787 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-90887872022-05-11 Electronic Properties of Fully Strained La(1–x)Sr(x)MnO(3) Thin Films Grown by Molecular Beam Epitaxy (0.15 ≤ x ≤ 0.45) Chaluvadi, Sandeep Kumar Polewczyk, Vincent Petrov, Aleksandr Yu Vinai, Giovanni Braglia, Luca Diez, Jose Manuel Pierron, Victor Perna, Paolo Mechin, Laurence Torelli, Piero Orgiani, Pasquale ACS Omega [Image: see text] The structural, electronic, and magnetic properties of Sr-hole-doped epitaxial La(1–x)Sr(x)MnO(3) (0.15 ≤ x ≤ 0.45) thin films deposited using the molecular beam epitaxy technique on 4° vicinal STO (001) substrates are probed by the combination of X-ray diffraction and various synchrotron-based spectroscopy techniques. The structural characterizations evidence a significant shift in the LSMO (002) peak to the higher diffraction angles owing to the increase in Sr doping concentrations in thin films. The nature of the LSMO Mn mixed-valence state was estimated from X-ray photoemission spectroscopy together with the relative changes in the Mn L(2,3) edges observed in X-ray absorption spectroscopy (XAS), both strongly affected by doping. CTM4XAS simulations at the XAS Mn L(2,3) edges reveal the combination of epitaxial strain, and different MnO(6) crystal field splitting give rise to a peak at ∼641 eV. The observed changes in the occupancy of the e(g) and the t(2g) orbitals as well as their binding energy positions toward the Fermi level with hole doping are discussed. The room-temperature magnetic properties were probed at the end by circular dichroism. American Chemical Society 2022-04-20 /pmc/articles/PMC9088787/ /pubmed/35557663 http://dx.doi.org/10.1021/acsomega.1c06529 Text en © 2022 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by-nc-nd/4.0/Permits non-commercial access and re-use, provided that author attribution and integrity are maintained; but does not permit creation of adaptations or other derivative works (https://creativecommons.org/licenses/by-nc-nd/4.0/). |
spellingShingle | Chaluvadi, Sandeep Kumar Polewczyk, Vincent Petrov, Aleksandr Yu Vinai, Giovanni Braglia, Luca Diez, Jose Manuel Pierron, Victor Perna, Paolo Mechin, Laurence Torelli, Piero Orgiani, Pasquale Electronic Properties of Fully Strained La(1–x)Sr(x)MnO(3) Thin Films Grown by Molecular Beam Epitaxy (0.15 ≤ x ≤ 0.45) |
title | Electronic Properties of Fully Strained La(1–x)Sr(x)MnO(3) Thin
Films Grown by Molecular Beam Epitaxy (0.15 ≤ x ≤ 0.45) |
title_full | Electronic Properties of Fully Strained La(1–x)Sr(x)MnO(3) Thin
Films Grown by Molecular Beam Epitaxy (0.15 ≤ x ≤ 0.45) |
title_fullStr | Electronic Properties of Fully Strained La(1–x)Sr(x)MnO(3) Thin
Films Grown by Molecular Beam Epitaxy (0.15 ≤ x ≤ 0.45) |
title_full_unstemmed | Electronic Properties of Fully Strained La(1–x)Sr(x)MnO(3) Thin
Films Grown by Molecular Beam Epitaxy (0.15 ≤ x ≤ 0.45) |
title_short | Electronic Properties of Fully Strained La(1–x)Sr(x)MnO(3) Thin
Films Grown by Molecular Beam Epitaxy (0.15 ≤ x ≤ 0.45) |
title_sort | electronic properties of fully strained la(1–x)sr(x)mno(3) thin
films grown by molecular beam epitaxy (0.15 ≤ x ≤ 0.45) |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9088787/ https://www.ncbi.nlm.nih.gov/pubmed/35557663 http://dx.doi.org/10.1021/acsomega.1c06529 |
work_keys_str_mv | AT chaluvadisandeepkumar electronicpropertiesoffullystrainedla1xsrxmno3thinfilmsgrownbymolecularbeamepitaxy015x045 AT polewczykvincent electronicpropertiesoffullystrainedla1xsrxmno3thinfilmsgrownbymolecularbeamepitaxy015x045 AT petrovaleksandryu electronicpropertiesoffullystrainedla1xsrxmno3thinfilmsgrownbymolecularbeamepitaxy015x045 AT vinaigiovanni electronicpropertiesoffullystrainedla1xsrxmno3thinfilmsgrownbymolecularbeamepitaxy015x045 AT braglialuca electronicpropertiesoffullystrainedla1xsrxmno3thinfilmsgrownbymolecularbeamepitaxy015x045 AT diezjosemanuel electronicpropertiesoffullystrainedla1xsrxmno3thinfilmsgrownbymolecularbeamepitaxy015x045 AT pierronvictor electronicpropertiesoffullystrainedla1xsrxmno3thinfilmsgrownbymolecularbeamepitaxy015x045 AT pernapaolo electronicpropertiesoffullystrainedla1xsrxmno3thinfilmsgrownbymolecularbeamepitaxy015x045 AT mechinlaurence electronicpropertiesoffullystrainedla1xsrxmno3thinfilmsgrownbymolecularbeamepitaxy015x045 AT torellipiero electronicpropertiesoffullystrainedla1xsrxmno3thinfilmsgrownbymolecularbeamepitaxy015x045 AT orgianipasquale electronicpropertiesoffullystrainedla1xsrxmno3thinfilmsgrownbymolecularbeamepitaxy015x045 |