Abstract:SummaryWe present the results of an investigation of surface-enhanced Raman scattering (SERS) by optical phonons in colloidal CdSe nanocrystals (NCs) homogeneously deposited on both arrays of Au nanoclusters and Au dimers using the Langmuir–Blodgett technique. The coverage of the deposited NCs was less than one monolayer, as determined by transmission and scanning electron microscopy. SERS by optical phonons in CdSe nanocrystals showed a significant enhancement that depends resonantly on the Au nanocluster and… Show more
“…NCs of ZnO, for instance, can be formed through thermal oxidation of zinc behenate films in air at a temperature of 400 °C-600 °C [51]. The LB technique was also adapted for homogeneous deposition of NC arrays of colloidal NCs [57][58][59][60][61][62][63].…”
Section: Fabrication Of Ncsmentioning
confidence: 99%
“…Anisotropy causes the splitting of the plasmonic mode polarized along and perpendicular to the long dimer axis. The splitting value increases with decreasing gap between Au nanoclusters in a dimer as shown in figure 29(b) [61,[390][391][392]. While the LSPR energy for Au nanoclusters and dimers varies gradually in the red spectral range, an array with optimal structural parameters can be chosen for SERS experiments.…”
Section: Fabrication and Characterisation Of Plasmonic Metal Nanoclus...mentioning
A review of recent applications of Raman spectroscopy as a fast, sensitive, and non-destructive technique for exploring II–VI semiconductor nanocrystals fabricated by various methods (colloidal chemistry, Langmuir–Blodgett method, diffusion-limited growth) is presented. Specific size-related features revealed in the nanocrystal Raman spectra (phonon confinement, surface phonons) are analysed, as well as more complicated size effects for ultrasmall nanocrystals (NCs) related to the activation of the phonon density of states modified by surface reconstruction. Similarities and differences of the Raman scattering in II–VI and III–V or elemental (Si) semiconductor NCs are briefly analysed. Implementation of resonant conditions and application of infrared absorption analysis, complementary to the Raman spectroscopy—resulting in the observation of phonon modes ‘silent’ in conventional Raman scattering processes—are discussed. Furthermore, Raman spectroscopy is employed for fast and efficient assessment of the composition of matrix-embedded ternary II–VI nanocrystals, as well as more complicated multimode quaternary II–VI systems. Selective probing of electronic and vibrational spectra of different parts of heterogeneous NCs (such as core–shell systems) by tuning the excitation wavelength in resonant Raman scattering is considered. The analysis of phonon spectra is applied to the quantitative estimation of strain in the core and shell, and degree of interface intermixing, as well as to checking the surface oxidation. The above approaches and phenomena are further explored in more complex compound NCs beyond II–VI, such as CuInS2/ZnS. Recent results in the field of surface- and tip-enhanced Raman spectroscopy and surface-enhanced infrared absorption are analysed showing the perspectives of Raman spectroscopy as a tool for investigation of single-nanocrystal phonon spectra.
“…NCs of ZnO, for instance, can be formed through thermal oxidation of zinc behenate films in air at a temperature of 400 °C-600 °C [51]. The LB technique was also adapted for homogeneous deposition of NC arrays of colloidal NCs [57][58][59][60][61][62][63].…”
Section: Fabrication Of Ncsmentioning
confidence: 99%
“…Anisotropy causes the splitting of the plasmonic mode polarized along and perpendicular to the long dimer axis. The splitting value increases with decreasing gap between Au nanoclusters in a dimer as shown in figure 29(b) [61,[390][391][392]. While the LSPR energy for Au nanoclusters and dimers varies gradually in the red spectral range, an array with optimal structural parameters can be chosen for SERS experiments.…”
Section: Fabrication and Characterisation Of Plasmonic Metal Nanoclus...mentioning
A review of recent applications of Raman spectroscopy as a fast, sensitive, and non-destructive technique for exploring II–VI semiconductor nanocrystals fabricated by various methods (colloidal chemistry, Langmuir–Blodgett method, diffusion-limited growth) is presented. Specific size-related features revealed in the nanocrystal Raman spectra (phonon confinement, surface phonons) are analysed, as well as more complicated size effects for ultrasmall nanocrystals (NCs) related to the activation of the phonon density of states modified by surface reconstruction. Similarities and differences of the Raman scattering in II–VI and III–V or elemental (Si) semiconductor NCs are briefly analysed. Implementation of resonant conditions and application of infrared absorption analysis, complementary to the Raman spectroscopy—resulting in the observation of phonon modes ‘silent’ in conventional Raman scattering processes—are discussed. Furthermore, Raman spectroscopy is employed for fast and efficient assessment of the composition of matrix-embedded ternary II–VI nanocrystals, as well as more complicated multimode quaternary II–VI systems. Selective probing of electronic and vibrational spectra of different parts of heterogeneous NCs (such as core–shell systems) by tuning the excitation wavelength in resonant Raman scattering is considered. The analysis of phonon spectra is applied to the quantitative estimation of strain in the core and shell, and degree of interface intermixing, as well as to checking the surface oxidation. The above approaches and phenomena are further explored in more complex compound NCs beyond II–VI, such as CuInS2/ZnS. Recent results in the field of surface- and tip-enhanced Raman spectroscopy and surface-enhanced infrared absorption are analysed showing the perspectives of Raman spectroscopy as a tool for investigation of single-nanocrystal phonon spectra.
“…Monolayers of colloidal CdSe NCs with a size of (5.0 ± 0.3) nm purchased from Lumidot were homogeneously deposited on specially prepared plasmonic substrates by means of the modified LB technique as described in ref . LB is a well-proven technique for fabricating both highly ordered organic films and NCs with controlled areal density , on solid substrates.…”
Section: Methodsmentioning
confidence: 99%
“…Monolayers of colloidal CdSe NCs with a size of (5.0 ± 0.3) nm purchased from Lumidot were homogeneously deposited on specially prepared plasmonic substrates by means of the modified LB technique as described in ref 21. LB is a well-proven technique for fabricating both highly ordered organic films 29 and NCs with controlled areal density 20,21 on solid substrates. The size, shape, and areal density of CdSe NCs, as well as structural parameters of nanoantennas (length, width, period) were determined by SEM using the same Raith-150 system at 10 kV acceleration voltage, 30 μm aperture, and 6 mm working distance.…”
Section: ■ Experimental Sectionmentioning
confidence: 99%
“…SERS by confined and surface optical phonons in semiconductor nanostructures including CdS, ,, CdSe, ,,− Cu x S, ,− and ZnO , NCs and GaN, AlN, and ZnO , nanorods was observed and investigated by different groups. A strong SERS enhancement by surface optical (SO) modes with the gain factor up to 10 4 was reported for ZnO nanostructures. , The vibrational response from localized optical phonons in CdSe NC arrays of a low areal density down to a few NCs per square micrometer was also probed by SERS. , …”
We report on a study
of surface-enhanced infrared absorption (SEIRA)
by optical phonons in monolayers (MLs) of CdSe, CdS, and PbS nanocrystals
(NCs) deposited on arrays of linear nanoantennas the optimized structural
parameters of which allow coupling between the localized surface plasmon
resonance (LSPR) and diffraction modes in the far-infrared spectral
region. The Langmuir–Blodgett technique was used for homogeneous
deposition of the NCs. The structural parameters of the arrays and
the NC MLs were determined by scanning electron microscopy. According
to the three-dimensional electrodynamic simulations of the electromagnetic
field distribution around the antennas, the maximal SEIRA enhancement
is realized for an array period of about 15 μm when the energy
of a diffraction mode coincides with that of the LSPR mode. SEIRA
experimental results are in perfect quantitative agreement with the
simulation. The maximal SEIRA enhancement is observed for the nanoantenna
length and transverse periodicity predicted by the simulations. The
frequency positions of the absorption features indicate that only
the NC surface optical phonons are activated in the SEIRA spectra.
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