Improved Ti-mask selective-area growth (SAG) by rf-plasma-assisted molecular beam epitaxy demonstrating extremely uniform GaN nanocolumn arrays

The Ti-mask selective-area growth (SAG) of GaN nanocolumns was performed at the growth temperature of 900 °C, while decreasing the supplied nitrogen flow rate ( Q N2) from 3.5 to 0.5 sccm. Highly uniform arrays of GaN nanocolumns were demonstrated. At low Q N2, both the desorption and diffusion of G...

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Veröffentlicht in:Journal of crystal growth 2009-03, Vol.311 (7), p.2063-2068
Hauptverfasser: Kishino, Katsumi, Sekiguchi, Hiroto, Kikuchi, Akihiko
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Sekiguchi, Hiroto
Kikuchi, Akihiko
description The Ti-mask selective-area growth (SAG) of GaN nanocolumns was performed at the growth temperature of 900 °C, while decreasing the supplied nitrogen flow rate ( Q N2) from 3.5 to 0.5 sccm. Highly uniform arrays of GaN nanocolumns were demonstrated. At low Q N2, both the desorption and diffusion of Ga from/on the nitrided Ti mask were accelerated, which sufficiently suppressed the crystal nucleation on the Ti-mask surface, and hence the SAG of the GaN nanocolumns was achieved even when the spacing between the nanocolumns was several hundred nm. The enhancement of Ga desorption with decreasing Q N2 brought about a reduction in the growth rate of GaN nanocolumns from 1.05 to 0.15 μm/h. The lateral growth rate of the GaN nanocolumns rapidly increased above the critical Q N2 value of 1.5 sccm and became 45 nm/h at Q N2 of 3.5 sccm. For low Q N2 values less than 1.5 sccm, the lateral growth rate became sufficiently low, approximately 8 nm/h; this contributes to well-controlled SAG of GaN, where the underlying nanomask patterns are well traced.
doi_str_mv 10.1016/j.jcrysgro.2008.11.056
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Desorption</topic><topic>A1. Growth models</topic><topic>A1. Nanostructures</topic><topic>A3. Molecular beam epitaxy</topic><topic>A3. Selective epitaxy</topic><topic>B1. Nitrides</topic><topic>Condensed matter: structure, mechanical and thermal properties</topic><topic>Cross-disciplinary physics: materials science; rheology</topic><topic>Diffusion in solids</topic><topic>Exact sciences and technology</topic><topic>Materials science</topic><topic>Methods of crystal growth; physics of crystal growth</topic><topic>Methods of deposition of films and coatings; film growth and epitaxy</topic><topic>Molecular, atomic, ion, and chemical beam epitaxy</topic><topic>Physics</topic><topic>Theory and models of crystal growth; physics of crystal growth, crystal morphology and orientation</topic><topic>Transport properties of condensed matter (nonelectronic)</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kishino, Katsumi</creatorcontrib><creatorcontrib>Sekiguchi, Hiroto</creatorcontrib><creatorcontrib>Kikuchi, Akihiko</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><jtitle>Journal of crystal growth</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kishino, Katsumi</au><au>Sekiguchi, Hiroto</au><au>Kikuchi, Akihiko</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Improved Ti-mask selective-area growth (SAG) by rf-plasma-assisted molecular beam epitaxy demonstrating extremely uniform GaN nanocolumn arrays</atitle><jtitle>Journal of crystal growth</jtitle><date>2009-03-15</date><risdate>2009</risdate><volume>311</volume><issue>7</issue><spage>2063</spage><epage>2068</epage><pages>2063-2068</pages><issn>0022-0248</issn><eissn>1873-5002</eissn><coden>JCRGAE</coden><abstract>The Ti-mask selective-area growth (SAG) of GaN nanocolumns was performed at the growth temperature of 900 °C, while decreasing the supplied nitrogen flow rate ( Q N2) from 3.5 to 0.5 sccm. Highly uniform arrays of GaN nanocolumns were demonstrated. At low Q N2, both the desorption and diffusion of Ga from/on the nitrided Ti mask were accelerated, which sufficiently suppressed the crystal nucleation on the Ti-mask surface, and hence the SAG of the GaN nanocolumns was achieved even when the spacing between the nanocolumns was several hundred nm. The enhancement of Ga desorption with decreasing Q N2 brought about a reduction in the growth rate of GaN nanocolumns from 1.05 to 0.15 μm/h. The lateral growth rate of the GaN nanocolumns rapidly increased above the critical Q N2 value of 1.5 sccm and became 45 nm/h at Q N2 of 3.5 sccm. For low Q N2 values less than 1.5 sccm, the lateral growth rate became sufficiently low, approximately 8 nm/h; this contributes to well-controlled SAG of GaN, where the underlying nanomask patterns are well traced.</abstract><cop>Amsterdam</cop><pub>Elsevier B.V</pub><doi>10.1016/j.jcrysgro.2008.11.056</doi><tpages>6</tpages></addata></record>
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subjects A1. Desorption
A1. Growth models
A1. Nanostructures
A3. Molecular beam epitaxy
A3. Selective epitaxy
B1. Nitrides
Condensed matter: structure, mechanical and thermal properties
Cross-disciplinary physics: materials science
rheology
Diffusion in solids
Exact sciences and technology
Materials science
Methods of crystal growth
physics of crystal growth
Methods of deposition of films and coatings
film growth and epitaxy
Molecular, atomic, ion, and chemical beam epitaxy
Physics
Theory and models of crystal growth
physics of crystal growth, crystal morphology and orientation
Transport properties of condensed matter (nonelectronic)
title Improved Ti-mask selective-area growth (SAG) by rf-plasma-assisted molecular beam epitaxy demonstrating extremely uniform GaN nanocolumn arrays
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