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Effect of pulse laser frequency on PLD growth of LuFeO(3) explained by kinetic simulations of in-situ diffracted intensities
Atomistic processes during pulsed-laser deposition (PLD) growth influence the physical properties of the resulting films. We investigated the PLD of epitaxial layers of hexagonal LuFeO[Formula: see text] by measuring the X-ray diffraction intensity in the quasiforbidden reflection 0003 in situ durin...
Autores principales: | , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8983772/ https://www.ncbi.nlm.nih.gov/pubmed/35383221 http://dx.doi.org/10.1038/s41598-022-09414-3 |
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author | Gabriel, Vít Kocán, Pavel Bauer, Sondes Nergis, Berkin Rodrigues, Adriana Horák, Lukáš Jin, Xiaowei Schneider, Reinhard Baumbach, Tilo Holý, Václav |
author_facet | Gabriel, Vít Kocán, Pavel Bauer, Sondes Nergis, Berkin Rodrigues, Adriana Horák, Lukáš Jin, Xiaowei Schneider, Reinhard Baumbach, Tilo Holý, Václav |
author_sort | Gabriel, Vít |
collection | PubMed |
description | Atomistic processes during pulsed-laser deposition (PLD) growth influence the physical properties of the resulting films. We investigated the PLD of epitaxial layers of hexagonal LuFeO[Formula: see text] by measuring the X-ray diffraction intensity in the quasiforbidden reflection 0003 in situ during deposition. From measured X-ray diffraction intensities we determined coverages of each layer and studied their time evolution which is described by scaling exponent [Formula: see text] directly connected to the surface roughness. Subsequently we modelled the growth using kinetic Monte Carlo simulations. While the experimentally obtained scaling exponent [Formula: see text] decreases with the laser frequency, the simulations provided the opposite behaviour. We demonstrate that the increase of the surface temperature caused by impinging ablated particles satisfactorily explains the recorded decrease in the scaling exponent with the laser frequency. This phenomena is often overlooked during the PLD growth. |
format | Online Article Text |
id | pubmed-8983772 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-89837722022-04-06 Effect of pulse laser frequency on PLD growth of LuFeO(3) explained by kinetic simulations of in-situ diffracted intensities Gabriel, Vít Kocán, Pavel Bauer, Sondes Nergis, Berkin Rodrigues, Adriana Horák, Lukáš Jin, Xiaowei Schneider, Reinhard Baumbach, Tilo Holý, Václav Sci Rep Article Atomistic processes during pulsed-laser deposition (PLD) growth influence the physical properties of the resulting films. We investigated the PLD of epitaxial layers of hexagonal LuFeO[Formula: see text] by measuring the X-ray diffraction intensity in the quasiforbidden reflection 0003 in situ during deposition. From measured X-ray diffraction intensities we determined coverages of each layer and studied their time evolution which is described by scaling exponent [Formula: see text] directly connected to the surface roughness. Subsequently we modelled the growth using kinetic Monte Carlo simulations. While the experimentally obtained scaling exponent [Formula: see text] decreases with the laser frequency, the simulations provided the opposite behaviour. We demonstrate that the increase of the surface temperature caused by impinging ablated particles satisfactorily explains the recorded decrease in the scaling exponent with the laser frequency. This phenomena is often overlooked during the PLD growth. Nature Publishing Group UK 2022-04-05 /pmc/articles/PMC8983772/ /pubmed/35383221 http://dx.doi.org/10.1038/s41598-022-09414-3 Text en © The Author(s) 2022 https://creativecommons.org/licenses/by/4.0/Open AccessThis article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) . |
spellingShingle | Article Gabriel, Vít Kocán, Pavel Bauer, Sondes Nergis, Berkin Rodrigues, Adriana Horák, Lukáš Jin, Xiaowei Schneider, Reinhard Baumbach, Tilo Holý, Václav Effect of pulse laser frequency on PLD growth of LuFeO(3) explained by kinetic simulations of in-situ diffracted intensities |
title | Effect of pulse laser frequency on PLD growth of LuFeO(3) explained by kinetic simulations of in-situ diffracted intensities |
title_full | Effect of pulse laser frequency on PLD growth of LuFeO(3) explained by kinetic simulations of in-situ diffracted intensities |
title_fullStr | Effect of pulse laser frequency on PLD growth of LuFeO(3) explained by kinetic simulations of in-situ diffracted intensities |
title_full_unstemmed | Effect of pulse laser frequency on PLD growth of LuFeO(3) explained by kinetic simulations of in-situ diffracted intensities |
title_short | Effect of pulse laser frequency on PLD growth of LuFeO(3) explained by kinetic simulations of in-situ diffracted intensities |
title_sort | effect of pulse laser frequency on pld growth of lufeo(3) explained by kinetic simulations of in-situ diffracted intensities |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8983772/ https://www.ncbi.nlm.nih.gov/pubmed/35383221 http://dx.doi.org/10.1038/s41598-022-09414-3 |
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