Ekaterina E. Rodyakina

Combination of surface- and interference-enhanced Raman scattering by CuS nanocrystals on nanopatterned Au structures

Summary We present the results of a Raman study of optical phonons in CuS nanocrystals (NCs) with a low areal density fabricated through the Langmuir–Blodgett technology on nanopatterned Au nanocluster arrays using a combination of surface- and interference-enhanced Raman scattering (SERS and IERS, respectively). Micro-Raman spectra of one monolayer of CuS NCs deposited on a bare Si substrate reveal only features corresponding to crystalline Si. However, a new relatively strong peak occurs in the Raman spectrum of CuS NCs on Au nanocluster arrays at 474 cm−1. This feature is related to the optical phonon mode in CuS NCs and manifests the SERS effect. For CuS NCs deposited on a SiO2 layer this phonon mode is also observed due to the IERS effect. Its intensity changes periodically with increasing SiO2 layer thickness for different laser excitation lines and is enhanced by a factor of about 30. CuS NCs formed on Au nanocluster arrays fabricated on IERS substrates combine the advantages of SERS and IERS and demonstrate stronger SERS enhancement allowing for the observation of Raman signals from CuS NCs with an ultra-low areal density.

Surface-enhanced Raman scattering and gap-mode tip-enhanced Raman scattering investigations of phthalocyanine molecules on gold nanostructured substrates

This study reports the use of surface-enhanced Raman scattering (SERS) and tip-enhanced Raman scattering (TERS), both independent and in combination, to investigate Raman enhancement of films under different confinement geometries. The experiments are performed on ultrathin cobalt phthalocyanine (CoPc) films deposited on specially designed SERS structures. The SERS structures are fabricated by electron-beam lithography and contain nanostructured gold films and gold dimer arrays with controlled size and internanocluster distance. Such structures allow investigation of the effects of nanocluster size and internanocluster distance, excitation wavelength, and polarization of light upon the electromagnetic SERS enhancement. Significant enhancement of the Raman scattering by CoPc is observed under 632.8 nm excitation because of the double resonance originating from the energy match between the laser excitation and the localized surface plasmon and electronic transitions in CoPc. The SERS signal of CoPc is further enhanced by decreasing the internanocluster distance. Maximum SERS enhancement occurs when the polarization of the incident light is perpendicular to the dimer axis. Under 514.5 nm excitation, nanostructured gold films give greater enhancement than any of the nanocluster arrays, with the highest enhancement realized using the so-called “gap-mode TERS” wherein the SERS structures are probed in the TERS condition. The TERS experiment is performed using a customized TERS setup and all-metal atomic force microscopy tips custom fabricated. In terms of obtaining the ultimate sensitivity in Raman spectroscopy, further enhancement is achieved by confining the electromagnetic field in a gap between two metallic nanostructures either by using SERS or by combining SERS and TERS.This study reports the use of surface-enhanced Raman scattering (SERS) and tip-enhanced Raman scattering (TERS), both independent and in combination, to investigate Raman enhancement of films under different confinement geometries. The experiments are performed on ultrathin cobalt phthalocyanine (CoPc) films deposited on specially designed SERS structures. The SERS structures are fabricated by electron-beam lithography and contain nanostructured gold films and gold dimer arrays with controlled size and internanocluster distance. Such structures allow investigation of the effects of nanocluster size and internanocluster distance, excitation wavelength, and polarization of light upon the electromagnetic SERS enhancement. Significant enhancement of the Raman scattering by CoPc is observed under 632.8 nm excitation because of the double resonance originating from the energy match between the laser excitation and the localized surface plasmon and electronic transitions in CoPc. The SERS signal of CoPc is furth...

Surface-enhanced Raman scattering by colloidal CdSe nanocrystal submonolayers fabricated by the Langmuir–Blodgett technique

Summary We 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 dimer size, and thus on the localized surface plasmon resonance (LSPR) energy. The deposition of CdSe nanocrystals on the Au dimer nanocluster arrays enabled us to study the polarization dependence of SERS. The maximal SERS signal was observed for light polarization parallel to the dimer axis. The polarization ratio of the SERS signal parallel and perpendicular to the dimer axis was 20. The SERS signal intensity was also investigated as a function of the distance between nanoclusters in a dimer. Here the maximal SERS enhancement was observed for the minimal distance studied (about 10 nm), confirming the formation of SERS “hot spots”.

Localized surface plasmons in structures with linear Au nanoantennas on a SiO2/Si surface

The study of infrared absorption by linear gold nanoantennas fabricated on a Si surface with underlying SiO2 layers of various thicknesses allowed the penetration depth of localized surface plasmons into SiO2 to be determined. The value of the penetration depth derived experimentally (20 ± 10 nm) corresponds to that obtained from electromagnetic simulations (12.9–30.0 nm). Coupling between plasmonic excitations of gold nanoantennas and optical phonons in SiO2 leads to the appearance of new plasmon–phonon modes observed in the infrared transmission spectra the frequencies of which are well predicted by the simulations.

Nanoantenna structures for the detection of phonons in nanocrystals

We report a study of the infrared response by localized surface plasmon resonance (LSPR) modes in gold micro- and nanoantenna arrays with various morphologies and surface-enhanced infrared absorption (SEIRA) by optical phonons of semiconductor nanocrystals (NCs) deposited on the arrays. The arrays of nano- and microantennas fabricated with nano- and photolithography reveal infrared-active LSPR modes of energy ranging from the mid to far-infrared that allow the IR response from very low concentrations of organic and inorganic materials deposited onto the arrays to be analyzed. The Langmuir–Blodgett technology was used for homogeneous deposition of CdSe, CdS, and PbS NC monolayers on the antenna arrays. The structural parameters of the arrays were confirmed by scanning electron microscopy. 3D full-wave electromagnetic simulations of the electromagnetic field distribution around the micro- and nanoantennas were employed to realize the maximal SEIRA enhancement for structural parameters of the arrays whereby the LSPR and the NC optical phonon energies coincide. The SEIRA experiments quantitatively confirmed the computational results. The maximum SEIRA enhancement was observed for linear nanoantennas with optimized structural parameters determined from the electromagnetic simulations. The frequency position of the feature’s absorption seen in the SEIRA response evidences that the NC surface and transverse optical phonons are activated in the infrared spectra.

Raman scattering for probing semiconductor nanostructures: From nanocrystal arrays towards a single nanocrystal

We present a study of resonant and surface enhanced Raman scattering (SERS) by arrays of CdS, CuS, ZnO, and PbSe nanocrystals (NCs) with various areal density. Resonant Raman scattering by optical phonons and their overtones up to 9th order was observed for ZnO NC arrays by adjusting the laser energy to that of the interband transitions. The resonance enhancement allowed a Raman response from arrays of NCs with a low areal density (down to 10 PbSe NCs per 1 μm2) to be measured. An enhancement of Raman scattering by LO modes in CdS NC arrays by a factor of about 730 due to the resonant SERS effect was demonstrated. SERS effect by optical phonons in CuS NCs with ultra-low areal density formed on laterally ordered arrays of Au nanoclusters was observed.