FN Archimer Export Format
PT J
TI Surface enhanced Raman scattering optimization of gold nanocylinder arrays: Influence of the localized surface plasmon resonance and excitation wavelength
BT 
AF GUILLOT, N.
   SHEN, H.
   FREMAUX, B.
   PERON, Olivier
   RINNERT, Emmanuel
   TOURY, T.
   DE LA CHAPELLE, M. Lamy
AS 1:1;2:2;3:1;4:3;5:3;6:2;7:1;
FF 1:;2:;3:;4:PDG-DOP-DCB-RDT-IC;5:PDG-DOP-DCB-RDT-IC;6:;7:;
C1 Univ Paris 13, Lab CSPBAT FRE 3043, UFR SMBH, Equipe LBPS, F-93017 Bobigny, France.
   Univ Technol Troyes, Inst Charles Delaunay, LNIO, UMR CNRS 6279, F-10010 Troyes, France.
   IFREMER, Dept Rech & Dev Technol Serv Interfaces & Capteur, F-29280 Plouzane, France.
C2 UNIV PARIS 13, FRANCE
   UNIV TROYES, FRANCE
   IFREMER, FRANCE
SI BREST
SE PDG-DOP-DCB-RDT-IC
IN WOS Ifremer jusqu'en 2018
   copubli-france
   copubli-univ-france
IF 3.841
TC 95
UR https://archimer.ifremer.fr/doc/00011/12240/8970.pdf
LA English
DT Article
DE ;gradient index optics;lenses;metamaterials;microwave photonics;optical design techniques;optical fabrication;particle size
AB We here emphasize that the surface enhanced Raman scattering (SERS) intensity has to be optimized by choosing the appropriate gold nanoparticles size for two excitation wavelengths; 632.8 and 785 nm. We discuss the role of the position and of the order of the localized surface plasmon resonance (LSPR) in such optimization for both wavelengths. At 632.8 nm, the best SERS intensity is reached for a LSPR located between the excitation and Raman wavelengths whereas at 785 nm, the LSPR should be placed outside this range. The third order of LSPR is shown to have no influence on the SERS intensity. (C) 2010 American Institute of Physics. [doi:10.1063/1.3462068]
PY 2010
PD JUN
SO Applied Physics Letters
SN 0003-6951
PU American Institut of Physics
VL 97
IS 2
UT 000279999800063
DI 10.1063/1.3462068
ID 12240
ER

EF