Phys. Chem. Chem. Phys., 2004, 6 | |
Additions and corrections Vibrational study of the S0 and S1 states of 2-naphthyl-1-ethanol/(water)2 and 2-naphthyl-1-ethanol/(methanol)2 complexes by IR/UV double resonance spectroscopy |
N. Seurre, J. Sepio, F. Lahmani, A. Zehnacker-Rentien and K. Le Barbu-Debus
Phys. Chem. Chem. Phys., 2004, 6, DOI: 10.1039/b405276e. Amendment published 26th August 2004
In the captions for Figs. 3 and 4 the words "cyclic" and "bridged" should be swapped: the bridged structure is associated with the solid lines and the cyclic with the broken lines.
Fig. 3 IR absorption spectra of the
NapOH/water 1:2 complex measured by fluorescence dip IR/UV double
resonance techniques. The UV probe is fixed on the band at –30
cm–1 from the 0–0 transition of NapOH. The
S0 and S1 IR spectra
are resolved by adjusting spatially the relative position of the beams in
the interaction zone of the jet. (a) IR and UV beams are superimposed; (b)
UV beam is shifted upstream from IR; (c) IR beam is set upstream from UV;
the stick diagram shows the computed spectra (DFT B3LYP/6-31G**) obtained
by applying a scaling factor of 0.96 to the calculated harmonic
frequencies for the bridged structure and /// for the cyclic one.
Fig. 4 IR absorption spectra of the
NapOH/methanol 1:2 complex measured by fluorescence dip IR/UV double
resonance techniques. The UV probe is fixed on the band
IIR at –55 cm–1 from
the 0–0 transition of NapOH. The S0 and
S1 IR spectra are resolved by adjusting
spatially the relative position of the beams in the interaction zone of
the jet. (a) IR and UV beams are superimposed; (b) UV beam is shifted
upstream from IR; (c) IR beam is set upstream from UV; the stick diagram
shows the computed spectra (DFT B3LYP/6-31G**) obtained by applying a
scaling factor of 0.96 to the calculated harmonic frequencies for the
bridged structure and /// for the cyclic
one.
The Royal Society of Chemistry apologises for these errors and any consequent inconvenience to authors and readers.