Far- and near-field properties of gold nanoshells studied by photoacoustic and surface-enhanced Raman spectroscopies.

Gold nanoshells, with a silica core and different core and shell dimensions, have been extensively investigated. Optical far-field properties, namely extinction and absorption, have been separately determined by means of spectrophotometry and photoacoustic spectroscopy, respectively, in the 440-900 nm range. The enhancement factor for surface-enhanced Raman scattering, which is related to near-field effects, has been measured from 568 to 920 nm. The absorption contribution to extinction decreases as the overall diameter increases. Moreover, absorption and scattering display different spectral distributions, the latter being red shifted. The Surface Enhanced Raman Scattering enhancement profile, measured using thiobenzoic acid as a Raman probe, is further shifted to the red. The latter result suggests that the enhancement is dominated by the presence of hot spots, which are possibly related to the surface roughness of gold nanoshell particles.

Resonance Raman spectroscopy of sensory rhodopsin II from Natronobacterium pharaonis.

Sensory rhodopsin II (pSRII), the photophobic receptor from Natronobacterium pharaonis, has been studied by time-resolved resonance Raman (RR) spectroscopy using the rotating cell technique. Upon excitation with low laser power, the RR spectra largely reflect the parent state pSRII(500) whereas an increase of the laser power leads to a substantial accumulation of long-lived intermediates contributing to the RR spectra. All RR spectra could consistently be analysed in terms of four component spectra which were assigned to the parent state pSRII(500) and the long-lived intermediates M(400), N(485) and O(535) based on the correlation between the C = C stretching frequency and the absorption maximum. The parent state and the intermediates N(485) and O(535) exhibit a protonated Schiff base. The C = N stretching frequencies and the H/D isotopic shifts indicate strong hydrogen bonding interactions of the Schiff base in pSRII(500) and O(535) whereas these interactions are most likely very weak in N(485).