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Atomic surface structure of MOVPE-prepared GaP(1 1 1)B

Controlling the surface formation of the group-V face of (1 1 1)-oriented III-V semiconductors is crucial for subsequent successful growth of III-V nanowires for electronic and optoelectronic applications. With a view to preparing GaP/Si(1 1 1) virtual substrates, we investigate the atomic structure...

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Autores principales: Kleinschmidt, P, Mutombo, P, Berthold, T, Paszuk, A, Steidl, M, Ecke, G, Nägelein, A, Koppka, C, Supplie, O, Krischok, S, Romanyuk, O, Himmerlich, M, Hannappel, T
Lenguaje:eng
Publicado: 2020
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.apsusc.2020.147346
http://cds.cern.ch/record/2800446
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author Kleinschmidt, P
Mutombo, P
Berthold, T
Paszuk, A
Steidl, M
Ecke, G
Nägelein, A
Koppka, C
Supplie, O
Krischok, S
Romanyuk, O
Himmerlich, M
Hannappel, T
author_facet Kleinschmidt, P
Mutombo, P
Berthold, T
Paszuk, A
Steidl, M
Ecke, G
Nägelein, A
Koppka, C
Supplie, O
Krischok, S
Romanyuk, O
Himmerlich, M
Hannappel, T
author_sort Kleinschmidt, P
collection CERN
description Controlling the surface formation of the group-V face of (1 1 1)-oriented III-V semiconductors is crucial for subsequent successful growth of III-V nanowires for electronic and optoelectronic applications. With a view to preparing GaP/Si(1 1 1) virtual substrates, we investigate the atomic structure of the MOVPE (metalorganic vapor phase epitaxy)-prepared GaP(1 1 1)B surface (phosphorus face). We find that upon high-temperature annealing in the H2-based MOVPE process ambience, the surface is phosphorus-depleted, as evidenced by X-ray photoemission spectroscopy (XPS). However, a combination of density functional theory calculations and scanning tunneling microscopy (STM) suggests the formation of a partially H-terminated phosphorus surface, where the STM contrast is due to electrons tunneling from non-terminated dangling bonds of the phosphorus face. Atomic force microscopy (AFM) reveals that a high proportion of the surface is covered by islands, which are confirmed as Ga-rich by Auger electron spectroscopy (AES). We conclude that the STM images of the samples after high-temperature annealing only reflect the flat regions of the partially H-terminated phosphorus face, whereas an increasing coverage with Ga-rich islands, as detected by AFM and AES, forms upon annealing and underlies the higher proportion of Ga in the XPS measurements.
id cern-2800446
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2020
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spelling cern-28004462022-01-26T22:36:34Zdoi:10.1016/j.apsusc.2020.147346http://cds.cern.ch/record/2800446engKleinschmidt, PMutombo, PBerthold, TPaszuk, ASteidl, MEcke, GNägelein, AKoppka, CSupplie, OKrischok, SRomanyuk, OHimmerlich, MHannappel, TAtomic surface structure of MOVPE-prepared GaP(1 1 1)BDetectors and Experimental TechniquesControlling the surface formation of the group-V face of (1 1 1)-oriented III-V semiconductors is crucial for subsequent successful growth of III-V nanowires for electronic and optoelectronic applications. With a view to preparing GaP/Si(1 1 1) virtual substrates, we investigate the atomic structure of the MOVPE (metalorganic vapor phase epitaxy)-prepared GaP(1 1 1)B surface (phosphorus face). We find that upon high-temperature annealing in the H2-based MOVPE process ambience, the surface is phosphorus-depleted, as evidenced by X-ray photoemission spectroscopy (XPS). However, a combination of density functional theory calculations and scanning tunneling microscopy (STM) suggests the formation of a partially H-terminated phosphorus surface, where the STM contrast is due to electrons tunneling from non-terminated dangling bonds of the phosphorus face. Atomic force microscopy (AFM) reveals that a high proportion of the surface is covered by islands, which are confirmed as Ga-rich by Auger electron spectroscopy (AES). We conclude that the STM images of the samples after high-temperature annealing only reflect the flat regions of the partially H-terminated phosphorus face, whereas an increasing coverage with Ga-rich islands, as detected by AFM and AES, forms upon annealing and underlies the higher proportion of Ga in the XPS measurements.oai:cds.cern.ch:28004462020
spellingShingle Detectors and Experimental Techniques
Kleinschmidt, P
Mutombo, P
Berthold, T
Paszuk, A
Steidl, M
Ecke, G
Nägelein, A
Koppka, C
Supplie, O
Krischok, S
Romanyuk, O
Himmerlich, M
Hannappel, T
Atomic surface structure of MOVPE-prepared GaP(1 1 1)B
title Atomic surface structure of MOVPE-prepared GaP(1 1 1)B
title_full Atomic surface structure of MOVPE-prepared GaP(1 1 1)B
title_fullStr Atomic surface structure of MOVPE-prepared GaP(1 1 1)B
title_full_unstemmed Atomic surface structure of MOVPE-prepared GaP(1 1 1)B
title_short Atomic surface structure of MOVPE-prepared GaP(1 1 1)B
title_sort atomic surface structure of movpe-prepared gap(1 1 1)b
topic Detectors and Experimental Techniques
url https://dx.doi.org/10.1016/j.apsusc.2020.147346
http://cds.cern.ch/record/2800446
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