Theoretical Routes for c-BN Thin Film Growth

Cubic boron nitride (c-BN) has been in focus for several years due to its interesting properties. The possibility for large area chemical vapor deposition (CVD) is a requirement for the realization of these different properties in various applications. Unfortunately, there are at present severe prob...

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Main Author: Karlsson, Johan
Format: Doctoral Thesis
Language:English
Published: Uppsala universitet, Oorganisk kemi 2013
Subjects:
Online Access:http://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-204234
http://nbn-resolving.de/urn:isbn:978-91-554-8705-8
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spelling ndltd-UPSALLA1-oai-DiVA.org-uu-2042342014-01-08T04:59:01ZTheoretical Routes for c-BN Thin Film GrowthengKarlsson, JohanUppsala universitet, Oorganisk kemiUppsala2013cubic boron nitridechemical vapor depositiondensity functional theoryCubic boron nitride (c-BN) has been in focus for several years due to its interesting properties. The possibility for large area chemical vapor deposition (CVD) is a requirement for the realization of these different properties in various applications. Unfortunately, there are at present severe problems in the CVD growth of c-BN. The purpose with this research project has been to theoretically investigate, using density functional theory (DFT) calculations, the possibility for a layer-by-layer CVD growth of c-BN.  The results, in addition with experimental work by Zhang et al.57,  indicate that plasma-enhanced atomic layer deposition (PEALD), using a BF3-H2-NH3-F2 pulse cycle and a diamond substrate, is a promising method for deposition of c-BN films. The gaseous species will decompose in the plasma and form BFx, H, NHx, and F species (x = 0, 1, 2, 3). The H and F radicals will uphold the cubic structure by completely hydrogenate, or fluorinate, the growing surface. Surface radical sites will appear during the growth process as a result of atomic H, or F, abstraction reactions. However, introduction of energy (e.g., ionic bombardment) is probably necessary to promote removal of H from the surface. The addition of NHx growth species (x = 0, 1, 2) to the B radical sites, and BFx growth species (x = 0, 1, 2) to N radical sites, will then result in a continuous growth of c-BN. Doctoral thesis, comprehensive summaryinfo:eu-repo/semantics/doctoralThesistexthttp://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-204234urn:isbn:978-91-554-8705-8Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology, 1651-6214 ; 1055application/pdfinfo:eu-repo/semantics/openAccess
collection NDLTD
language English
format Doctoral Thesis
sources NDLTD
topic cubic boron nitride
chemical vapor deposition
density functional theory
spellingShingle cubic boron nitride
chemical vapor deposition
density functional theory
Karlsson, Johan
Theoretical Routes for c-BN Thin Film Growth
description Cubic boron nitride (c-BN) has been in focus for several years due to its interesting properties. The possibility for large area chemical vapor deposition (CVD) is a requirement for the realization of these different properties in various applications. Unfortunately, there are at present severe problems in the CVD growth of c-BN. The purpose with this research project has been to theoretically investigate, using density functional theory (DFT) calculations, the possibility for a layer-by-layer CVD growth of c-BN.  The results, in addition with experimental work by Zhang et al.57,  indicate that plasma-enhanced atomic layer deposition (PEALD), using a BF3-H2-NH3-F2 pulse cycle and a diamond substrate, is a promising method for deposition of c-BN films. The gaseous species will decompose in the plasma and form BFx, H, NHx, and F species (x = 0, 1, 2, 3). The H and F radicals will uphold the cubic structure by completely hydrogenate, or fluorinate, the growing surface. Surface radical sites will appear during the growth process as a result of atomic H, or F, abstraction reactions. However, introduction of energy (e.g., ionic bombardment) is probably necessary to promote removal of H from the surface. The addition of NHx growth species (x = 0, 1, 2) to the B radical sites, and BFx growth species (x = 0, 1, 2) to N radical sites, will then result in a continuous growth of c-BN.
author Karlsson, Johan
author_facet Karlsson, Johan
author_sort Karlsson, Johan
title Theoretical Routes for c-BN Thin Film Growth
title_short Theoretical Routes for c-BN Thin Film Growth
title_full Theoretical Routes for c-BN Thin Film Growth
title_fullStr Theoretical Routes for c-BN Thin Film Growth
title_full_unstemmed Theoretical Routes for c-BN Thin Film Growth
title_sort theoretical routes for c-bn thin film growth
publisher Uppsala universitet, Oorganisk kemi
publishDate 2013
url http://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-204234
http://nbn-resolving.de/urn:isbn:978-91-554-8705-8
work_keys_str_mv AT karlssonjohan theoreticalroutesforcbnthinfilmgrowth
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