Shedding Light on the Extinction-Enhancement Duality in Gold Nanostar-Enhanced Raman Spectroscopy

Surface‐enhanced Raman spectroscopy (SERS) has evolved from an esoteric physical phenomenon to a robust and effective analytical method recently. The need of addressing both the field enhancement and the extinction of nanoparticle suspensions, however, has been underappreciated despite its substanti...

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Published inAngewandte Chemie (International ed.) Vol. 53; no. 51; pp. 14115 - 14119
Main Authors Li, Ming, Kang, Jeon Woong, Dasari, Ramachandra Rao, Barman, Ishan
Format Journal Article
LanguageEnglish
Published Weinheim WILEY-VCH Verlag 15.12.2014
WILEY‐VCH Verlag
Wiley Subscription Services, Inc
EditionInternational ed. in English
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Summary:Surface‐enhanced Raman spectroscopy (SERS) has evolved from an esoteric physical phenomenon to a robust and effective analytical method recently. The need of addressing both the field enhancement and the extinction of nanoparticle suspensions, however, has been underappreciated despite its substantive impact on the sensing performance. A systematic experimental investigation of SERS enhancement and attenuation is performed in suspensions of gold nanostars, which exhibit a markedly different behavior in relation to conventional nanoparticles. The relationship is elucidated between the SERS enhancement and the localized surface plasmon resonance band, and the effect of the concentration of the gold nanostars on the signal propagation is investigated. It is shown that an optimal concentration of gold nanostars exists to maximize the enhancement factor (EF), and the maximum EF occurs when the LSPR band is blue‐shifted from the excitation wavelength rather than at the on‐resonance position. Gold nanostars: The relationship between the enhancement by surface‐enhanced Raman spectroscopy (SERS) and the localized surface plasmon resonance (LSPR) band is investigated (see picture). The competition between the field enhancement and the optical extinction causes the maximum enhancement factor occurring at a blue‐shifted LSPR band from the excitation wavelength rather than at the on‐resonance position.
Bibliography:JHU Whiting School of Engineering Startup Funds
National Science Foundation - No. DMR-08-19762
NIH - No. 9P41EB015871-27
This research was supported by the JHU Whiting School of Engineering Startup Funds, NIH NIBIB (grant number 9P41EB015871-27) and the MIT SkolTech initiative. This work made use of the MRSEC shared experimental facilities at MIT, supported by the National Science Foundation under award number DMR-08-19762.
ArticleID:ANIE201409314
ark:/67375/WNG-WF9P6PW9-C
MIT SkolTech
istex:9506C64B65E8C5314015406CE452CFB5D2BF3029
This research was supported by the JHU Whiting School of Engineering Startup Funds, NIH NIBIB (grant number 9P41EB015871‐27) and the MIT SkolTech initiative. This work made use of the MRSEC shared experimental facilities at MIT, supported by the National Science Foundation under award number DMR‐08‐19762.
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ISSN:1433-7851
1521-3773
DOI:10.1002/anie.201409314