Direct measurement of the Raman enhancement factor of rhodamine 6G on graphene under resonant excitation
Graphene substrates have recently been found to generate Raman enhancement. Systematic studies using different Raman probes have been implemented, but one of the most commonly used Raman probes, rhodamine 6G (R6G), has yielded controversial results for the enhancement effect on graphene. Indeed, the...
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description | Graphene substrates have recently been found to generate Raman enhancement. Systematic studies using different Raman probes have been implemented, but one of the most commonly used Raman probes, rhodamine 6G (R6G), has yielded controversial results for the enhancement effect on graphene. Indeed, the Raman enhancement factor of R6G induced by graphene has never been measured directly under resonant excitation because of the presence of intense fluorescence backgrounds. In this study, a polarization-difference technique is used to suppress the fluorescence background by subtracting two spectra collected using different excitation laser polarizations. As a result, enhancement factors are obtained ranging between 1.7 and 5.6 for the four Raman modes of R6G at 611, 1,183, 1,361, and 1,647 cm-~ under resonant excitation by a 514.5 nm laser. By comparing these results with the results obtained under non-resonant excitation (632.8 nm) and pre-resonant excitation (593 nm), the enhancement can be attributed to static chemical enhancement (CHEM) and tuning of the molecular resonance. Density functional theory simulations reveal that the orbital energies and densities for R6G are modified bv ~raphene dots. |
doi_str_mv | 10.1007/s12274-014-0490-3 |
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Systematic studies using different Raman probes have been implemented, but one of the most commonly used Raman probes, rhodamine 6G (R6G), has yielded controversial results for the enhancement effect on graphene. Indeed, the Raman enhancement factor of R6G induced by graphene has never been measured directly under resonant excitation because of the presence of intense fluorescence backgrounds. In this study, a polarization-difference technique is used to suppress the fluorescence background by subtracting two spectra collected using different excitation laser polarizations. As a result, enhancement factors are obtained ranging between 1.7 and 5.6 for the four Raman modes of R6G at 611, 1,183, 1,361, and 1,647 cm-~ under resonant excitation by a 514.5 nm laser. By comparing these results with the results obtained under non-resonant excitation (632.8 nm) and pre-resonant excitation (593 nm), the enhancement can be attributed to static chemical enhancement (CHEM) and tuning of the molecular resonance. Density functional theory simulations reveal that the orbital energies and densities for R6G are modified bv ~raphene dots.</description><identifier>ISSN: 1998-0124</identifier><identifier>EISSN: 1998-0000</identifier><identifier>DOI: 10.1007/s12274-014-0490-3</identifier><language>eng</language><publisher>Heidelberg: Tsinghua University Press</publisher><subject>Atomic/Molecular Structure and Spectra ; Biomedicine ; Biotechnology ; Chemistry ; Chemistry and Materials Science ; Computer engineering ; Condensed Matter Physics ; Density ; Excitation ; Fluorescence ; Graphene ; Laboratories ; Lasers ; Materials Science ; Nanotechnology ; Probes ; Research Article ; Rhodamine 6G ; Spectra ; Tuning ; 共振激发 ; 化学增强 ; 增强因子 ; 拉曼 ; 探头系统 ; 直接测量 ; 石墨 ; 罗丹明6G</subject><ispartof>Nano research, 2014-09, Vol.7 (9), p.1271-1279</ispartof><rights>Tsinghua University Press and Springer-Verlag Berlin Heidelberg 2014</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c452t-775bef5f7a78f17b51f6a2145528d3321b51d1b9cb480e3aecaf60e283f8aa3f3</citedby><cites>FETCH-LOGICAL-c452t-775bef5f7a78f17b51f6a2145528d3321b51d1b9cb480e3aecaf60e283f8aa3f3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Uhttp://image.cqvip.com/vip1000/qk/71233X/71233X.jpg</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s12274-014-0490-3$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s12274-014-0490-3$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,776,780,27901,27902,41464,42533,51294</link.rule.ids></links><search><creatorcontrib>Deng, Shibin</creatorcontrib><creatorcontrib>Xu, Weigao</creatorcontrib><creatorcontrib>Wang, Jinying</creatorcontrib><creatorcontrib>Ling, Xi</creatorcontrib><creatorcontrib>Wu, Juanxia</creatorcontrib><creatorcontrib>Xie, Liming</creatorcontrib><creatorcontrib>Kong, Jing</creatorcontrib><creatorcontrib>Dresselhaus, Mildred S.</creatorcontrib><creatorcontrib>Zhang, Jin</creatorcontrib><title>Direct measurement of the Raman enhancement factor of rhodamine 6G on graphene under resonant excitation</title><title>Nano research</title><addtitle>Nano Res</addtitle><addtitle>Nano Research</addtitle><description>Graphene substrates have recently been found to generate Raman enhancement. Systematic studies using different Raman probes have been implemented, but one of the most commonly used Raman probes, rhodamine 6G (R6G), has yielded controversial results for the enhancement effect on graphene. Indeed, the Raman enhancement factor of R6G induced by graphene has never been measured directly under resonant excitation because of the presence of intense fluorescence backgrounds. In this study, a polarization-difference technique is used to suppress the fluorescence background by subtracting two spectra collected using different excitation laser polarizations. As a result, enhancement factors are obtained ranging between 1.7 and 5.6 for the four Raman modes of R6G at 611, 1,183, 1,361, and 1,647 cm-~ under resonant excitation by a 514.5 nm laser. By comparing these results with the results obtained under non-resonant excitation (632.8 nm) and pre-resonant excitation (593 nm), the enhancement can be attributed to static chemical enhancement (CHEM) and tuning of the molecular resonance. Density functional theory simulations reveal that the orbital energies and densities for R6G are modified bv ~raphene dots.</description><subject>Atomic/Molecular Structure and Spectra</subject><subject>Biomedicine</subject><subject>Biotechnology</subject><subject>Chemistry</subject><subject>Chemistry and Materials Science</subject><subject>Computer engineering</subject><subject>Condensed Matter Physics</subject><subject>Density</subject><subject>Excitation</subject><subject>Fluorescence</subject><subject>Graphene</subject><subject>Laboratories</subject><subject>Lasers</subject><subject>Materials Science</subject><subject>Nanotechnology</subject><subject>Probes</subject><subject>Research Article</subject><subject>Rhodamine 6G</subject><subject>Spectra</subject><subject>Tuning</subject><subject>共振激发</subject><subject>化学增强</subject><subject>增强因子</subject><subject>拉曼</subject><subject>探头系统</subject><subject>直接测量</subject><subject>石墨</subject><subject>罗丹明6G</subject><issn>1998-0124</issn><issn>1998-0000</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><sourceid>BENPR</sourceid><recordid>eNqFkV9rHCEUxYfQQtK0H6Bv0r7kZVqvOuo-lqRNC4FASJ7lrnvdmbCjG52B5tvHZdJS8pAK4p_7O-cqp2k-Av8CnJuvBYQwquVQp1rxVh41J7Ba2ZbX8ebPHoQ6bt6Vcs-5FqDsSdNfDJn8xEbCMmcaKU4sBTb1xG5wxMgo9hj9Ugjop5QP9dynDY5DJKYvWYpsm3HfUz3OcUOZZSopYlXQbz9MOA0pvm_eBtwV-vC8njZ3P77fnv9sr64vf51_u2q96sTUGtOtKXTBoLEBzLqDoLE-teuE3UgpoN5sYL3ya2U5SSSPQXMSVgaLKIM8bc4W331ODzOVyY1D8bTbYaQ0FwfGarBGCP1_VAsOXBmjKvr5BXqf5hzrRxx01U9wKaFSsFA-p1IyBbfPw4j50QF3h5jcEpOrMblDTE5WjVg0pbJxS_kf51dEn54b9SluH6rubyetRcdBSiWfAL0joBw</recordid><startdate>20140901</startdate><enddate>20140901</enddate><creator>Deng, 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Mildred S.</au><au>Zhang, Jin</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Direct measurement of the Raman enhancement factor of rhodamine 6G on graphene under resonant excitation</atitle><jtitle>Nano research</jtitle><stitle>Nano Res</stitle><addtitle>Nano Research</addtitle><date>2014-09-01</date><risdate>2014</risdate><volume>7</volume><issue>9</issue><spage>1271</spage><epage>1279</epage><pages>1271-1279</pages><issn>1998-0124</issn><eissn>1998-0000</eissn><abstract>Graphene substrates have recently been found to generate Raman enhancement. Systematic studies using different Raman probes have been implemented, but one of the most commonly used Raman probes, rhodamine 6G (R6G), has yielded controversial results for the enhancement effect on graphene. Indeed, the Raman enhancement factor of R6G induced by graphene has never been measured directly under resonant excitation because of the presence of intense fluorescence backgrounds. In this study, a polarization-difference technique is used to suppress the fluorescence background by subtracting two spectra collected using different excitation laser polarizations. As a result, enhancement factors are obtained ranging between 1.7 and 5.6 for the four Raman modes of R6G at 611, 1,183, 1,361, and 1,647 cm-~ under resonant excitation by a 514.5 nm laser. By comparing these results with the results obtained under non-resonant excitation (632.8 nm) and pre-resonant excitation (593 nm), the enhancement can be attributed to static chemical enhancement (CHEM) and tuning of the molecular resonance. Density functional theory simulations reveal that the orbital energies and densities for R6G are modified bv ~raphene dots.</abstract><cop>Heidelberg</cop><pub>Tsinghua University Press</pub><doi>10.1007/s12274-014-0490-3</doi><tpages>9</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Atomic/Molecular Structure and Spectra Biomedicine Biotechnology Chemistry Chemistry and Materials Science Computer engineering Condensed Matter Physics Density Excitation Fluorescence Graphene Laboratories Lasers Materials Science Nanotechnology Probes Research Article Rhodamine 6G Spectra Tuning 共振激发 化学增强 增强因子 拉曼 探头系统 直接测量 石墨 罗丹明6G |
title | Direct measurement of the Raman enhancement factor of rhodamine 6G on graphene under resonant excitation |
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