Thickness-Dependent Band Gap Modification in BaBiO<sub>3</sub>

The material BaBiO<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> is known for its insulat...

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Main Authors: Rosa Luca Bouwmeester, Alexander Brinkman, Kai Sotthewes
Format: Article
Language:English
Published: MDPI AG 2021-03-01
Series:Nanomaterials
Subjects:
Online Access:https://www.mdpi.com/2079-4991/11/4/882
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author Rosa Luca Bouwmeester
Alexander Brinkman
Kai Sotthewes
author_facet Rosa Luca Bouwmeester
Alexander Brinkman
Kai Sotthewes
author_sort Rosa Luca Bouwmeester
collection DOAJ
description The material BaBiO<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> is known for its insulating character. However, for thin films, in the ultra-thin limit, metallicity is expected because the oxygen octahedra breathing mode will be suppressed as reported recently. Here, we confirm the influence of the oxygen breathing mode on the size of the band gap. The electronic properties of a BaBiO<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> thickness series are studied using in-situ scanning tunneling microscopy. We observe a wide-gap (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>E</mi><mi mathvariant="normal">G</mi></msub></semantics></math></inline-formula> > 1.2 V) to small-gap (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>E</mi><mi mathvariant="normal">G</mi></msub></semantics></math></inline-formula> ≈ 0.07 eV) semiconductor transition as a function of a decreasing BaBiO<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> film thickness. However, even for an ultra-thin BaBiO<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> film, no metallic state is present. The dependence of the band gap size is found to be coinciding with the intensity of the Raman response of the breathing phonon mode as a function of thickness.
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spelling doaj.art-45ca9ef41c94478ea66c4887371802af2023-11-21T13:27:09ZengMDPI AGNanomaterials2079-49912021-03-0111488210.3390/nano11040882Thickness-Dependent Band Gap Modification in BaBiO<sub>3</sub>Rosa Luca Bouwmeester0Alexander Brinkman1Kai Sotthewes2MESA+ Institute for Nanotechnology, University of Twente, 7500 AE Enschede, The NetherlandsMESA+ Institute for Nanotechnology, University of Twente, 7500 AE Enschede, The NetherlandsMESA+ Institute for Nanotechnology, University of Twente, 7500 AE Enschede, The NetherlandsThe material BaBiO<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> is known for its insulating character. However, for thin films, in the ultra-thin limit, metallicity is expected because the oxygen octahedra breathing mode will be suppressed as reported recently. Here, we confirm the influence of the oxygen breathing mode on the size of the band gap. The electronic properties of a BaBiO<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> thickness series are studied using in-situ scanning tunneling microscopy. We observe a wide-gap (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>E</mi><mi mathvariant="normal">G</mi></msub></semantics></math></inline-formula> > 1.2 V) to small-gap (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>E</mi><mi mathvariant="normal">G</mi></msub></semantics></math></inline-formula> ≈ 0.07 eV) semiconductor transition as a function of a decreasing BaBiO<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> film thickness. However, even for an ultra-thin BaBiO<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mrow></mrow><mn>3</mn></msub></semantics></math></inline-formula> film, no metallic state is present. The dependence of the band gap size is found to be coinciding with the intensity of the Raman response of the breathing phonon mode as a function of thickness.https://www.mdpi.com/2079-4991/11/4/882BaBiO<sub>3</sub>scanning tunneling miscroscopyspectroscopypulsed laser depositionperovskitecomplex oxide
spellingShingle Rosa Luca Bouwmeester
Alexander Brinkman
Kai Sotthewes
Thickness-Dependent Band Gap Modification in BaBiO<sub>3</sub>
Nanomaterials
BaBiO<sub>3</sub>
scanning tunneling miscroscopy
spectroscopy
pulsed laser deposition
perovskite
complex oxide
title Thickness-Dependent Band Gap Modification in BaBiO<sub>3</sub>
title_full Thickness-Dependent Band Gap Modification in BaBiO<sub>3</sub>
title_fullStr Thickness-Dependent Band Gap Modification in BaBiO<sub>3</sub>
title_full_unstemmed Thickness-Dependent Band Gap Modification in BaBiO<sub>3</sub>
title_short Thickness-Dependent Band Gap Modification in BaBiO<sub>3</sub>
title_sort thickness dependent band gap modification in babio sub 3 sub
topic BaBiO<sub>3</sub>
scanning tunneling miscroscopy
spectroscopy
pulsed laser deposition
perovskite
complex oxide
url https://www.mdpi.com/2079-4991/11/4/882
work_keys_str_mv AT rosalucabouwmeester thicknessdependentbandgapmodificationinbabiosub3sub
AT alexanderbrinkman thicknessdependentbandgapmodificationinbabiosub3sub
AT kaisotthewes thicknessdependentbandgapmodificationinbabiosub3sub