Tian Zhao (341370)Jeremy W. Jarrett (1640359)JeffreyS. Johnson (1661566)Kyoungweon Park (1289037)Richard A. Vaia (1289031)Kenneth L. Knappenberger (1281822)
We report the polarization-dependent\nand time-resolved photoluminescence\n(PL) properties of gold nanorods (AuNRs). AuNRs corresponding to three\ndifferent length-to-diameter aspect ratios (AR)1.86, 2.91,\nand 3.90were examined using single-nanorod spectroscopy and\nimaging; the nanorod volume was approximately constant over the three\nsample types. For each AuNR, an aspect ratio-independent transverse\nplasmon resonance (TSPR) was detected at 2.41 eV. Aspect-ratio-dependent\nlongitudinal surface plasmon resonances (LSPRs) were observed at 2.08\n± 0.19 eV, 1.76 ± 0.12 eV, and 1.53 ± 0.15 eV for the\n1.86-AR, 2.91-AR, and 3.90-AR samples, respectively. On the basis\nof both excitation and emission polarization-resolved two-photon photoluminescence\n(TPPL) measurements, AuNR PL emission proceeded by plasmon-mediated\nradiative electron–hole recombination. The resonant LSPR mode\nfrequencies of the nanorods were determined from interferometrically\ndetected TPPL signals. For these measurements, the interpulse time\ndelays of a spectrally broad laser pulse (1.48–1.65 eV) were\nchanged systematically with attosecond time resolution, and the TPPL\nsignal amplitude was recorded. The 1.86-AR AuNR did not support a\nplasmon mode that was resonant within the laser bandwidth, whereas\nthe 2.91-AR and 3.90-AR samples had LSPR frequencies that overlapped\nthe high- and low-energy components of the excitation pulse. The LSPR\nfrequencies were obtained by Fourier transformation of the time-domain\nTPPL data and compared to dark-field scattering spectra. The accuracy\nof the interferometric TPPL measurement for recovering plasmon resonance\nfrequencies was confirmed by polarization-dependent measurements;\nalignment of the laser electric field parallel to the nanorod major\naxis was LSPR resonant, whereas projection of the laser pulse into\nan orthogonal plane was not. Finally, dephasing times (<i>T</i><sub>2</sub>) for resonant plasmon modes were extracted from analysis\nof interferometric TPPL and second harmonic generation data. These\nresults showed that the dephasing time increased from 22 ± 4\nto 31 ± 9 fs as the LSPR resonance energy decreased from 1.76\nto 1.53 eV, as a result of less efficient plasmon dephasing due to\ninterband scattering for lower energy resonances. These results demonstrate\nthe capability of interferometric nonlinear optical imaging with single-nanostructure\nsensitivity for determining structure-specific dephasing times, which\ninfluence the efficiency of metal nanoparticle light-harvesting applications.\nTherefore, interferometric nonlinear optical (NLO) imaging is likely\nto make a significant impact on the rational design of photonic nanostructures.
Tian ZhaoJeremy W. JarrettJeffrey S. JohnsonKyoungweon ParkRichard A. VaiaKenneth L. Knappenberger
Yoshio NishiyamaKeisuke ImaedaKohei ImuraHiromi Okamoto
Yoshio Nishiyama (1487083)Keisuke Imaeda (1567273)Kohei Imura (1487086)Hiromi Okamoto (1336890)
Matthew PeltonMingzhao LiuHee Young KimGlenna SmithPhilippe Guyot‐SionnestNorbert F. Scherer
Matthew PeltonMingzhao LiuHee Young KimGlenna SmithPhilippe Guyot‐SionnestNorbert F. Scherer