The epitaxial crystalline silicon-oxynitride layer on SiC(0 0 0 1): Formation of an ideal SiC–insulator interface
► Recently discovered crystalline silicon-oxynitride film of 0.6 nm-thick. ► Epitaxially grown film on 6 H-SiC(0 0 0 1) of extremely robust against air. ► Ultrathin-oxide insulator/semiconductor interface with no dangling bond. ► Band-gap at the ultrathin oxide is fully open up to a value of quartz....
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creator | Tochihara, Hiroshi Shirasawa, Tetsuroh |
description | ► Recently discovered crystalline silicon-oxynitride film of 0.6
nm-thick. ► Epitaxially grown film on 6
H-SiC(0
0
0
1) of extremely robust against air. ► Ultrathin-oxide insulator/semiconductor interface with no dangling bond. ► Band-gap at the ultrathin oxide is fully open up to a value of quartz. ► Promising seed for nanoelectronic devices.
Silicon carbide (SiC) has the potential to serve as an extremely important semiconductor material in next-generation electronics. However, a major stumbling block for its practical application has been the preparation of high-quality interfaces with insulating materials. We have discovered a way to prepare a 0.6-nm thick silicon oxynitride (SiON) layer having an epitaxial interface with the SiC(0
0
0
1) surface. This review article focuses on the atomic and electronic structures of the SiON layer. Based on various experimental techniques and theoretical studies, we understand the SiON layer to be a complex but unique hetero-double-layered structure: a topmost Si
2O
5 monolayer is connected to an interfacial Si
2N
3 monolayer via Si–O–Si linear bridge bonds. The most striking feature of the SiON structure is that there is no dangling bond in the unit cell, rendering it remarkably robust to air exposure. Stability and processes for the formation of the SiON on SiC(0
0
0
1) are discussed on the basis of the structural features obtained. Scanning tunneling spectroscopy measurements of the SiON exhibit a bulk SiO
2-like band gap of ∼9
eV as well as first-principles calculations. The remarkable band-gap opening of such a thin insulator film is investigated by the combination of element-specific soft x-ray absorption/emission spectroscopies and by first-principles calculations, revealing the Si
2N
3 and Si
2O
5 monolayers to have band gaps of corresponding bulk-like values. Promising applications of the SiON to electronic devices are discussed. |
doi_str_mv | 10.1016/j.progsurf.2011.08.003 |
format | Article |
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nm-thick. ► Epitaxially grown film on 6
H-SiC(0
0
0
1) of extremely robust against air. ► Ultrathin-oxide insulator/semiconductor interface with no dangling bond. ► Band-gap at the ultrathin oxide is fully open up to a value of quartz. ► Promising seed for nanoelectronic devices.
Silicon carbide (SiC) has the potential to serve as an extremely important semiconductor material in next-generation electronics. However, a major stumbling block for its practical application has been the preparation of high-quality interfaces with insulating materials. We have discovered a way to prepare a 0.6-nm thick silicon oxynitride (SiON) layer having an epitaxial interface with the SiC(0
0
0
1) surface. This review article focuses on the atomic and electronic structures of the SiON layer. Based on various experimental techniques and theoretical studies, we understand the SiON layer to be a complex but unique hetero-double-layered structure: a topmost Si
2O
5 monolayer is connected to an interfacial Si
2N
3 monolayer via Si–O–Si linear bridge bonds. The most striking feature of the SiON structure is that there is no dangling bond in the unit cell, rendering it remarkably robust to air exposure. Stability and processes for the formation of the SiON on SiC(0
0
0
1) are discussed on the basis of the structural features obtained. Scanning tunneling spectroscopy measurements of the SiON exhibit a bulk SiO
2-like band gap of ∼9
eV as well as first-principles calculations. The remarkable band-gap opening of such a thin insulator film is investigated by the combination of element-specific soft x-ray absorption/emission spectroscopies and by first-principles calculations, revealing the Si
2N
3 and Si
2O
5 monolayers to have band gaps of corresponding bulk-like values. Promising applications of the SiON to electronic devices are discussed.</description><identifier>ISSN: 0079-6816</identifier><identifier>EISSN: 1878-4240</identifier><identifier>DOI: 10.1016/j.progsurf.2011.08.003</identifier><identifier>CODEN: PSSFBP</identifier><language>eng</language><publisher>Oxford: Elsevier Ltd</publisher><subject>Atomic structure ; Band spectra ; Condensed matter: electronic structure, electrical, magnetic, and optical properties ; Condensed matter: structure, mechanical and thermal properties ; Cross-disciplinary physics: materials science; rheology ; Electron diffraction and scattering ; Electronic structure and electrical properties of surfaces, interfaces, thin films and low-dimensional structures ; Energy gaps (solid state) ; Epitaxy ; Exact sciences and technology ; Low-energy electron diffraction (leed) and reflection high-energy electron diffraction (rheed) ; Materials science ; Mathematical analysis ; Methods of deposition of films and coatings; film growth and epitaxy ; Monolayers ; New surface material ; Physics ; Semiconductor/oxide interface ; Silicon carbide ; Silicon oxynitride ; Structure of solids and liquids; crystallography ; Surface and interface electron states ; Surface states, band structure, electron density of states ; Ultrathin epitaxial film ; Vapor phase epitaxy; growth from vapor phase</subject><ispartof>Progress in surface science, 2011-12, Vol.86 (11), p.295-327</ispartof><rights>2011 Elsevier Ltd</rights><rights>2015 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c441t-42cb519e1ca61d154d5f1af1a7bbb4c5610b5179dd7ebb8296257e371b1624853</citedby><cites>FETCH-LOGICAL-c441t-42cb519e1ca61d154d5f1af1a7bbb4c5610b5179dd7ebb8296257e371b1624853</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.progsurf.2011.08.003$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,780,784,3550,27924,27925,45995</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=25286538$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Tochihara, Hiroshi</creatorcontrib><creatorcontrib>Shirasawa, Tetsuroh</creatorcontrib><title>The epitaxial crystalline silicon-oxynitride layer on SiC(0 0 0 1): Formation of an ideal SiC–insulator interface</title><title>Progress in surface science</title><description>► Recently discovered crystalline silicon-oxynitride film of 0.6
nm-thick. ► Epitaxially grown film on 6
H-SiC(0
0
0
1) of extremely robust against air. ► Ultrathin-oxide insulator/semiconductor interface with no dangling bond. ► Band-gap at the ultrathin oxide is fully open up to a value of quartz. ► Promising seed for nanoelectronic devices.
Silicon carbide (SiC) has the potential to serve as an extremely important semiconductor material in next-generation electronics. However, a major stumbling block for its practical application has been the preparation of high-quality interfaces with insulating materials. We have discovered a way to prepare a 0.6-nm thick silicon oxynitride (SiON) layer having an epitaxial interface with the SiC(0
0
0
1) surface. This review article focuses on the atomic and electronic structures of the SiON layer. Based on various experimental techniques and theoretical studies, we understand the SiON layer to be a complex but unique hetero-double-layered structure: a topmost Si
2O
5 monolayer is connected to an interfacial Si
2N
3 monolayer via Si–O–Si linear bridge bonds. The most striking feature of the SiON structure is that there is no dangling bond in the unit cell, rendering it remarkably robust to air exposure. Stability and processes for the formation of the SiON on SiC(0
0
0
1) are discussed on the basis of the structural features obtained. Scanning tunneling spectroscopy measurements of the SiON exhibit a bulk SiO
2-like band gap of ∼9
eV as well as first-principles calculations. The remarkable band-gap opening of such a thin insulator film is investigated by the combination of element-specific soft x-ray absorption/emission spectroscopies and by first-principles calculations, revealing the Si
2N
3 and Si
2O
5 monolayers to have band gaps of corresponding bulk-like values. Promising applications of the SiON to electronic devices are discussed.</description><subject>Atomic structure</subject><subject>Band spectra</subject><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Cross-disciplinary physics: materials science; rheology</subject><subject>Electron diffraction and scattering</subject><subject>Electronic structure and electrical properties of surfaces, interfaces, thin films and low-dimensional structures</subject><subject>Energy gaps (solid state)</subject><subject>Epitaxy</subject><subject>Exact sciences and technology</subject><subject>Low-energy electron diffraction (leed) and reflection high-energy electron diffraction (rheed)</subject><subject>Materials science</subject><subject>Mathematical analysis</subject><subject>Methods of deposition of films and coatings; film growth and epitaxy</subject><subject>Monolayers</subject><subject>New surface material</subject><subject>Physics</subject><subject>Semiconductor/oxide interface</subject><subject>Silicon carbide</subject><subject>Silicon oxynitride</subject><subject>Structure of solids and liquids; crystallography</subject><subject>Surface and interface electron states</subject><subject>Surface states, band structure, electron density of states</subject><subject>Ultrathin epitaxial film</subject><subject>Vapor phase epitaxy; growth from vapor phase</subject><issn>0079-6816</issn><issn>1878-4240</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNqFkMtqGzEUQEVpoW7aXyjaFNLFTKTx6OGsUkxeEOgiyVpoNHeSa2TJleQS7_oP_cN8SWScdhskEFyd-zqEfOWs5YzLk1W7SfEhb9PUdozzlumWsfk7MuNa6abvevaezBhTi0ZqLj-STzmvGGNCaTEj-e4RKGyw2Ce0nrq0y8V6jwFoRo8uhiY-7QKWhCNQb3eQaAz0FpfHjO4P_35KL2Ja24I1HidqA61orVWZ5z9_MeSttyUmiqFAmqyDz-TDZH2GL6_vEbm_OL9bXjU3Py-vlz9uGtf3vNTJ3SD4Arizko9c9KOYuK1XDcPQOyE5q_9qMY4KhkF3C9kJBXPFBy67Xov5ETk-1K1-fm0hF7PG7MB7GyBus6n2mFZdr_aoPKAuxZwTTGaTcG3TrkJ7TpqV-WfZ7C0bpk21XBO_vfaw2Vk_JRsc5v_Znei0FHNdubMDB3Xh3wjJZIcQHIyYwBUzRnyr1Qt-NJcx</recordid><startdate>201112</startdate><enddate>201112</enddate><creator>Tochihara, Hiroshi</creator><creator>Shirasawa, Tetsuroh</creator><general>Elsevier Ltd</general><general>Elsevier</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>201112</creationdate><title>The epitaxial crystalline silicon-oxynitride layer on SiC(0 0 0 1): Formation of an ideal SiC–insulator interface</title><author>Tochihara, Hiroshi ; Shirasawa, Tetsuroh</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c441t-42cb519e1ca61d154d5f1af1a7bbb4c5610b5179dd7ebb8296257e371b1624853</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Atomic structure</topic><topic>Band spectra</topic><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>Condensed matter: structure, mechanical and thermal properties</topic><topic>Cross-disciplinary physics: materials science; rheology</topic><topic>Electron diffraction and scattering</topic><topic>Electronic structure and electrical properties of surfaces, interfaces, thin films and low-dimensional structures</topic><topic>Energy gaps (solid state)</topic><topic>Epitaxy</topic><topic>Exact sciences and technology</topic><topic>Low-energy electron diffraction (leed) and reflection high-energy electron diffraction (rheed)</topic><topic>Materials science</topic><topic>Mathematical analysis</topic><topic>Methods of deposition of films and coatings; film growth and epitaxy</topic><topic>Monolayers</topic><topic>New surface material</topic><topic>Physics</topic><topic>Semiconductor/oxide interface</topic><topic>Silicon carbide</topic><topic>Silicon oxynitride</topic><topic>Structure of solids and liquids; crystallography</topic><topic>Surface and interface electron states</topic><topic>Surface states, band structure, electron density of states</topic><topic>Ultrathin epitaxial film</topic><topic>Vapor phase epitaxy; growth from vapor phase</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Tochihara, Hiroshi</creatorcontrib><creatorcontrib>Shirasawa, Tetsuroh</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Progress in surface science</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Tochihara, Hiroshi</au><au>Shirasawa, Tetsuroh</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The epitaxial crystalline silicon-oxynitride layer on SiC(0 0 0 1): Formation of an ideal SiC–insulator interface</atitle><jtitle>Progress in surface science</jtitle><date>2011-12</date><risdate>2011</risdate><volume>86</volume><issue>11</issue><spage>295</spage><epage>327</epage><pages>295-327</pages><issn>0079-6816</issn><eissn>1878-4240</eissn><coden>PSSFBP</coden><abstract>► Recently discovered crystalline silicon-oxynitride film of 0.6
nm-thick. ► Epitaxially grown film on 6
H-SiC(0
0
0
1) of extremely robust against air. ► Ultrathin-oxide insulator/semiconductor interface with no dangling bond. ► Band-gap at the ultrathin oxide is fully open up to a value of quartz. ► Promising seed for nanoelectronic devices.
Silicon carbide (SiC) has the potential to serve as an extremely important semiconductor material in next-generation electronics. However, a major stumbling block for its practical application has been the preparation of high-quality interfaces with insulating materials. We have discovered a way to prepare a 0.6-nm thick silicon oxynitride (SiON) layer having an epitaxial interface with the SiC(0
0
0
1) surface. This review article focuses on the atomic and electronic structures of the SiON layer. Based on various experimental techniques and theoretical studies, we understand the SiON layer to be a complex but unique hetero-double-layered structure: a topmost Si
2O
5 monolayer is connected to an interfacial Si
2N
3 monolayer via Si–O–Si linear bridge bonds. The most striking feature of the SiON structure is that there is no dangling bond in the unit cell, rendering it remarkably robust to air exposure. Stability and processes for the formation of the SiON on SiC(0
0
0
1) are discussed on the basis of the structural features obtained. Scanning tunneling spectroscopy measurements of the SiON exhibit a bulk SiO
2-like band gap of ∼9
eV as well as first-principles calculations. The remarkable band-gap opening of such a thin insulator film is investigated by the combination of element-specific soft x-ray absorption/emission spectroscopies and by first-principles calculations, revealing the Si
2N
3 and Si
2O
5 monolayers to have band gaps of corresponding bulk-like values. Promising applications of the SiON to electronic devices are discussed.</abstract><cop>Oxford</cop><pub>Elsevier Ltd</pub><doi>10.1016/j.progsurf.2011.08.003</doi><tpages>33</tpages></addata></record> |
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source | Elsevier ScienceDirect Journals Complete |
subjects | Atomic structure Band spectra Condensed matter: electronic structure, electrical, magnetic, and optical properties Condensed matter: structure, mechanical and thermal properties Cross-disciplinary physics: materials science rheology Electron diffraction and scattering Electronic structure and electrical properties of surfaces, interfaces, thin films and low-dimensional structures Energy gaps (solid state) Epitaxy Exact sciences and technology Low-energy electron diffraction (leed) and reflection high-energy electron diffraction (rheed) Materials science Mathematical analysis Methods of deposition of films and coatings film growth and epitaxy Monolayers New surface material Physics Semiconductor/oxide interface Silicon carbide Silicon oxynitride Structure of solids and liquids crystallography Surface and interface electron states Surface states, band structure, electron density of states Ultrathin epitaxial film Vapor phase epitaxy growth from vapor phase |
title | The epitaxial crystalline silicon-oxynitride layer on SiC(0 0 0 1): Formation of an ideal SiC–insulator interface |
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