Spectroscopy and nonlinear microscopy of Au nanoparticle arrays: Experiment and theory

被引:66
作者
Hohenau, A [1 ]
Krenn, JR
Beermann, J
Bozhevolnyi, SI
Rodrigo, SG
Martin-Moreno, L
Garcia-Vidal, F
机构
[1] Karl Franzens Univ Graz, A-8010 Graz, Austria
[2] Erwin Schrodinger Inst Nanoscale Res, A-8010 Graz, Austria
[3] Univ Aalborg, Dept Phys & Nanotechnol, DK-9220 Aalborg, Denmark
[4] Univ Zaragoza, Fac Ciencias, E-50009 Zaragoza, Spain
[5] Univ Autonoma Madrid, Madrid, Spain
来源
PHYSICAL REVIEW B | 2006年 / 73卷 / 15期
关键词
D O I
10.1103/PhysRevB.73.155404
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Regular arrays of rectangular gold nanoparticles on glass substrates are characterized by using linear extinction spectroscopy (in the wavelength range of 450-950 nm) and nonlinear scanning optical microscopy, in which two-photon photoluminescence (TPL) excited with a strongly focused laser beam (in the wavelength range of 720-800 nm) is detected. The dimensions of the nanoparticles (similar to 150x150x50 nm(3)) are chosen to realize the localized-surface-plasmon (LSP) resonance at the wavelength of similar to 750 nm, which is clearly seen on the obtained extinction spectra as well as with the recorded TPL images. Extinction spectra are modeled using a finite-difference time-domain approach with the dielectric function of gold approximated by a Drude-Lorentz formula, showing rather good agreement between the experimental and theoretical spectra simulated for the nominal geometrical parameters of gold nanoparticles. The developed modeling tool is further used to evaluate the field intensity enhancement at the particles, which is then compared to the intensity enhancement estimated from the TPL images. We find good agreement between the intensity enhancement levels and indications that the LSP resonance wavelengths seen in the extinction spectra might differ from those deduced from the intensity enhancement spectra. The implications of the results obtained are discussed.
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页数:7
相关论文
共 17 条
[1]  
[Anonymous], 2011, RECENT PAT BIOTECHNO
[2]  
Azoulay J, 1999, J MICROSC-OXFORD, V194, P486, DOI 10.1046/j.1365-2818.1999.00558.x
[3]   Two-photon luminescence microscopy of field enhancement at gold nanoparticles [J].
Beermann, J ;
Bozhevolnyi, SI .
Physica Status Solidi C - Conferences and Critical Reviews, Vol 2 , No 12, 2005, 2 (12) :3983-3987
[4]   High-resolution second-harmonic microscopy of poled silica waveguides [J].
Beermann, J ;
Bozhevolnyi, SI ;
Pedersen, K ;
Fage-Pedersen, J .
OPTICS COMMUNICATIONS, 2003, 221 (4-6) :295-300
[5]   LOCAL-FIELD ENHANCEMENT ON ROUGH SURFACES OF METALS, SEMIMETALS, AND SEMICONDUCTORS WITH THE USE OF OPTICAL 2ND-HARMONIC GENERATION [J].
BOYD, GT ;
RASING, T ;
LEITE, JRR ;
SHEN, YR .
PHYSICAL REVIEW B, 1984, 30 (02) :519-526
[6]   Enhanced substrate-induced coupling in two-dimensional gold nanoparticle arrays -: art. no. 245407 [J].
Félidj, N ;
Aubard, J ;
Lévi, G ;
Krenn, JR ;
Schider, G ;
Leitner, A ;
Aussenegg, FR .
PHYSICAL REVIEW B, 2002, 66 (24) :1-7
[7]   Gap-dependent optical coupling of single "Bowtie" nanoantennas resonant in the visible [J].
Fromm, DP ;
Sundaramurthy, A ;
Schuck, PJ ;
Kino, G ;
Moerner, WE .
NANO LETTERS, 2004, 4 (05) :957-961
[8]   Metal nanoparticle gratings: Influence of dipolar particle interaction on the plasmon resonance [J].
Lamprecht, B ;
Schider, G ;
Lechner, RT ;
Ditlbacher, H ;
Krenn, JR ;
Leitner, A ;
Aussenegg, FR .
PHYSICAL REVIEW LETTERS, 2000, 84 (20) :4721-4724
[9]   FDTD FOR NTH-ORDER DISPERSIVE MEDIA [J].
LUEBBERS, RJ ;
HUNSBERGER, F .
IEEE TRANSACTIONS ON ANTENNAS AND PROPAGATION, 1992, 40 (11) :1297-1301
[10]  
McCord M., 1997, HDB MICROLITHOGRAPHY, V1