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...

Descripción completa

Detalles Bibliográficos
Autores principales: 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
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