Surface optical Raman modes in GaN nanoribbons
Raman scattering studies were performed in GaN nanoribbons grown along [1 0 0]. These samples were prepared inside Na‐4 mica nanochannels by the ion‐exchange technique and subsequent annealing in NH3 ambient. Detailed morphological and structural studies including the crystalline orientation were pe...
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Veröffentlicht in: | Journal of Raman spectroscopy 2011-03, Vol.42 (3), p.429-433 |
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description | Raman scattering studies were performed in GaN nanoribbons grown along [1 0 0]. These samples were prepared inside Na‐4 mica nanochannels by the ion‐exchange technique and subsequent annealing in NH3 ambient. Detailed morphological and structural studies including the crystalline orientation were performed by analyzing the vibrational properties in these GaN nanoribbons. Pressure in the embedded structure was calculated from the blue shift of the E2(high) phonon mode of GaN. Possible red shift of optical phonon modes due to the quantum confinement is also discussed. In addition to the optical phonons allowed by symmetry, two additional Raman peaks were also observed at ∼633 and 678 cm−1 for these nanoribbons. Calculations for the wavenumbers of the surface optical (SO) phonon modes in GaN in Na‐4 mica yielded values close to those of the new Raman modes. The SO phonon modes were calculated in the slab (applicable to belt‐like nanoribbon) mode, as the wavenumber and intensity of these modes depend on the size and the shape of the nanostructures. The effect of surface‐modulation‐assisted electron–SO phonon scattering is suggested to be responsible for the pronounced appearance of SO phonon modes. A scaling factor is also estimated for the interacting surface potential influencing the observed SO Raman scattering intensities. Copyright © 2010 John Wiley & Sons, Ltd.
Raman scattering studies are performed in GaN nanoribbons prepared inside Na‐4 mica nanochannels. Calculations yield SO phonon wavenumbers close to the new Raman modes found at ∼633 and 678 cm−1 in these nanoribbons. The effect of surface‐modulation‐assisted electron–SO phonon scattering is suggested to be responsible for the pronounced appearance of SO phonon modes, invoking a scaling factor which is also estimated for the interacting surface potential. |
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Raman scattering studies are performed in GaN nanoribbons prepared inside Na‐4 mica nanochannels. Calculations yield SO phonon wavenumbers close to the new Raman modes found at ∼633 and 678 cm−1 in these nanoribbons. The effect of surface‐modulation‐assisted electron–SO phonon scattering is suggested to be responsible for the pronounced appearance of SO phonon modes, invoking a scaling factor which is also estimated for the interacting surface potential.</description><identifier>ISSN: 0377-0486</identifier><identifier>ISSN: 1097-4555</identifier><identifier>EISSN: 1097-4555</identifier><identifier>DOI: 10.1002/jrs.2704</identifier><identifier>CODEN: JRSPAF</identifier><language>eng</language><publisher>Chichester, UK: John Wiley & Sons, Ltd</publisher><subject>Gallium nitrides ; GaN ; Mathematical analysis ; Mica ; Na-4 mica ; nanobelt ; Nanocomposites ; Nanomaterials ; Nanostructure ; Phonons ; Raman scattering ; surface optical mode ; surface potential ; Wavenumber</subject><ispartof>Journal of Raman spectroscopy, 2011-03, Vol.42 (3), p.429-433</ispartof><rights>Copyright © 2010 John Wiley & Sons, Ltd.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c4304-a3a1dba232de44699a31ecf6a98f838869ddc273f4ca770080d4d51ad98a99683</citedby><cites>FETCH-LOGICAL-c4304-a3a1dba232de44699a31ecf6a98f838869ddc273f4ca770080d4d51ad98a99683</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1002%2Fjrs.2704$$EPDF$$P50$$Gwiley$$H</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1002%2Fjrs.2704$$EHTML$$P50$$Gwiley$$H</linktohtml><link.rule.ids>314,780,784,1416,27923,27924,45573,45574</link.rule.ids></links><search><creatorcontrib>Bhattacharya, Santanu</creatorcontrib><creatorcontrib>Datta, Anindya</creatorcontrib><creatorcontrib>Dhara, Sandip</creatorcontrib><creatorcontrib>Chakravorty, Dipankar</creatorcontrib><title>Surface optical Raman modes in GaN nanoribbons</title><title>Journal of Raman spectroscopy</title><addtitle>J. Raman Spectrosc</addtitle><description>Raman scattering studies were performed in GaN nanoribbons grown along [1 0 0]. These samples were prepared inside Na‐4 mica nanochannels by the ion‐exchange technique and subsequent annealing in NH3 ambient. Detailed morphological and structural studies including the crystalline orientation were performed by analyzing the vibrational properties in these GaN nanoribbons. Pressure in the embedded structure was calculated from the blue shift of the E2(high) phonon mode of GaN. Possible red shift of optical phonon modes due to the quantum confinement is also discussed. In addition to the optical phonons allowed by symmetry, two additional Raman peaks were also observed at ∼633 and 678 cm−1 for these nanoribbons. Calculations for the wavenumbers of the surface optical (SO) phonon modes in GaN in Na‐4 mica yielded values close to those of the new Raman modes. The SO phonon modes were calculated in the slab (applicable to belt‐like nanoribbon) mode, as the wavenumber and intensity of these modes depend on the size and the shape of the nanostructures. The effect of surface‐modulation‐assisted electron–SO phonon scattering is suggested to be responsible for the pronounced appearance of SO phonon modes. A scaling factor is also estimated for the interacting surface potential influencing the observed SO Raman scattering intensities. Copyright © 2010 John Wiley & Sons, Ltd.
Raman scattering studies are performed in GaN nanoribbons prepared inside Na‐4 mica nanochannels. Calculations yield SO phonon wavenumbers close to the new Raman modes found at ∼633 and 678 cm−1 in these nanoribbons. The effect of surface‐modulation‐assisted electron–SO phonon scattering is suggested to be responsible for the pronounced appearance of SO phonon modes, invoking a scaling factor which is also estimated for the interacting surface potential.</description><subject>Gallium nitrides</subject><subject>GaN</subject><subject>Mathematical analysis</subject><subject>Mica</subject><subject>Na-4 mica</subject><subject>nanobelt</subject><subject>Nanocomposites</subject><subject>Nanomaterials</subject><subject>Nanostructure</subject><subject>Phonons</subject><subject>Raman scattering</subject><subject>surface optical mode</subject><subject>surface potential</subject><subject>Wavenumber</subject><issn>0377-0486</issn><issn>1097-4555</issn><issn>1097-4555</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNp10M9LwzAcBfAgCs4p-CcUvHjpzM8mOcrQqYwJ22SwS_guTaGzbWayovvv7ZgoCp7e5cPj8RC6JHhAMKY36xAHVGJ-hHoEa5lyIcQx6mEmZYq5yk7RWYxrjLHWGemhwawNBViX-M22tFAlU6ihSWqfu5iUTTKCSdJA40O5WvkmnqOTAqroLr6yj17u7-bDh3T8PHoc3o5TyxnmKTAg-Qooo7njPNMaGHG2yECrQjGlMp3nlkpWcAtSYqxwznNBINcKul2K9dH1oXcT_Fvr4tbUZbSuqqBxvo2GYEpVRgURHb36Q9e-DU23zhBBJNNCSv1TaIOPMbjCbEJZQ9h1VWZ_nOmOM_vjOpoe6HtZud2_zjxNZ799Gbfu49tDeDWZZFKYxWRk5moh6XS5NEv2CWSTe6Q</recordid><startdate>201103</startdate><enddate>201103</enddate><creator>Bhattacharya, Santanu</creator><creator>Datta, Anindya</creator><creator>Dhara, Sandip</creator><creator>Chakravorty, Dipankar</creator><general>John Wiley & Sons, Ltd</general><general>Wiley Subscription Services, Inc</general><scope>BSCLL</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7QF</scope><scope>7QO</scope><scope>7QQ</scope><scope>7SC</scope><scope>7SE</scope><scope>7SP</scope><scope>7SR</scope><scope>7TA</scope><scope>7TB</scope><scope>7U5</scope><scope>7U9</scope><scope>8BQ</scope><scope>8FD</scope><scope>F28</scope><scope>FR3</scope><scope>H8D</scope><scope>H8G</scope><scope>H94</scope><scope>JG9</scope><scope>JQ2</scope><scope>KR7</scope><scope>L7M</scope><scope>L~C</scope><scope>L~D</scope><scope>P64</scope><scope>RC3</scope></search><sort><creationdate>201103</creationdate><title>Surface optical Raman modes in GaN nanoribbons</title><author>Bhattacharya, Santanu ; Datta, Anindya ; Dhara, Sandip ; Chakravorty, Dipankar</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c4304-a3a1dba232de44699a31ecf6a98f838869ddc273f4ca770080d4d51ad98a99683</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Gallium nitrides</topic><topic>GaN</topic><topic>Mathematical analysis</topic><topic>Mica</topic><topic>Na-4 mica</topic><topic>nanobelt</topic><topic>Nanocomposites</topic><topic>Nanomaterials</topic><topic>Nanostructure</topic><topic>Phonons</topic><topic>Raman scattering</topic><topic>surface optical mode</topic><topic>surface potential</topic><topic>Wavenumber</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bhattacharya, Santanu</creatorcontrib><creatorcontrib>Datta, Anindya</creatorcontrib><creatorcontrib>Dhara, Sandip</creatorcontrib><creatorcontrib>Chakravorty, Dipankar</creatorcontrib><collection>Istex</collection><collection>CrossRef</collection><collection>Aluminium Industry Abstracts</collection><collection>Biotechnology Research Abstracts</collection><collection>Ceramic Abstracts</collection><collection>Computer and Information Systems Abstracts</collection><collection>Corrosion Abstracts</collection><collection>Electronics & Communications Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>Materials Business File</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Virology and AIDS Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Copper Technical Reference Library</collection><collection>AIDS and Cancer Research Abstracts</collection><collection>Materials Research Database</collection><collection>ProQuest Computer Science Collection</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Computer and Information Systems Abstracts Academic</collection><collection>Computer and Information Systems Abstracts Professional</collection><collection>Biotechnology and BioEngineering Abstracts</collection><collection>Genetics Abstracts</collection><jtitle>Journal of Raman spectroscopy</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bhattacharya, Santanu</au><au>Datta, Anindya</au><au>Dhara, Sandip</au><au>Chakravorty, Dipankar</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Surface optical Raman modes in GaN nanoribbons</atitle><jtitle>Journal of Raman spectroscopy</jtitle><addtitle>J. Raman Spectrosc</addtitle><date>2011-03</date><risdate>2011</risdate><volume>42</volume><issue>3</issue><spage>429</spage><epage>433</epage><pages>429-433</pages><issn>0377-0486</issn><issn>1097-4555</issn><eissn>1097-4555</eissn><coden>JRSPAF</coden><abstract>Raman scattering studies were performed in GaN nanoribbons grown along [1 0 0]. These samples were prepared inside Na‐4 mica nanochannels by the ion‐exchange technique and subsequent annealing in NH3 ambient. Detailed morphological and structural studies including the crystalline orientation were performed by analyzing the vibrational properties in these GaN nanoribbons. Pressure in the embedded structure was calculated from the blue shift of the E2(high) phonon mode of GaN. Possible red shift of optical phonon modes due to the quantum confinement is also discussed. In addition to the optical phonons allowed by symmetry, two additional Raman peaks were also observed at ∼633 and 678 cm−1 for these nanoribbons. Calculations for the wavenumbers of the surface optical (SO) phonon modes in GaN in Na‐4 mica yielded values close to those of the new Raman modes. The SO phonon modes were calculated in the slab (applicable to belt‐like nanoribbon) mode, as the wavenumber and intensity of these modes depend on the size and the shape of the nanostructures. The effect of surface‐modulation‐assisted electron–SO phonon scattering is suggested to be responsible for the pronounced appearance of SO phonon modes. A scaling factor is also estimated for the interacting surface potential influencing the observed SO Raman scattering intensities. Copyright © 2010 John Wiley & Sons, Ltd.
Raman scattering studies are performed in GaN nanoribbons prepared inside Na‐4 mica nanochannels. Calculations yield SO phonon wavenumbers close to the new Raman modes found at ∼633 and 678 cm−1 in these nanoribbons. The effect of surface‐modulation‐assisted electron–SO phonon scattering is suggested to be responsible for the pronounced appearance of SO phonon modes, invoking a scaling factor which is also estimated for the interacting surface potential.</abstract><cop>Chichester, UK</cop><pub>John Wiley & Sons, Ltd</pub><doi>10.1002/jrs.2704</doi><tpages>5</tpages></addata></record> |
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subjects | Gallium nitrides GaN Mathematical analysis Mica Na-4 mica nanobelt Nanocomposites Nanomaterials Nanostructure Phonons Raman scattering surface optical mode surface potential Wavenumber |
title | Surface optical Raman modes in GaN nanoribbons |
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