A SURFACE-ENHANCED HYPER-RAMAN AND SURFACE-ENHANCED RAMAN-SCATTERING STUDY OF TRANS-1,2-BIS(4-PYRIDYL)ETHYLENE ADSORBED ONTO SILVER FILM OVER NANOSPHERE ELECTRODES - VIBRATIONAL ASSIGNMENTS - EXPERIMENT AND THEORY

Citation
Wh. Yang et al., A SURFACE-ENHANCED HYPER-RAMAN AND SURFACE-ENHANCED RAMAN-SCATTERING STUDY OF TRANS-1,2-BIS(4-PYRIDYL)ETHYLENE ADSORBED ONTO SILVER FILM OVER NANOSPHERE ELECTRODES - VIBRATIONAL ASSIGNMENTS - EXPERIMENT AND THEORY, The Journal of chemical physics, 104(11), 1996, pp. 4313-4323
Citations number
31
Categorie Soggetti
Physics, Atomic, Molecular & Chemical
ISSN journal
00219606
Volume
104
Issue
11
Year of publication
1996
Pages
4313 - 4323
Database
ISI
SICI code
0021-9606(1996)104:11<4313:ASHASR>2.0.ZU;2-L
Abstract
We present theoretical and experimental studies of the infrared (LR) s pectroscopy, normal Raman spectroscopy (NRS), surface-enhanced Raman s pectroscopy (SERS), and surface-enhanced hyper-Raman (SEHRS) spectrosc opy of trans-1,2-bis(4-pyridyl)ethylene (BPE). This centrosymmetric mo lecule is expected to have no common Raman and hyper-Raman lines provi ded that it is not strongly perturbed by adsorption on the surface. Th e measured SERS spectrum, obtained under electrochemical conditions on Ag film over nanosphere (AgFON) electrode's, shows a well defined C d ouble bond C stretch band that is not seen in the SEHRS spectrum, but many of the other bands overlap closely. We use ab initio calculations for isolated BPE to assign the spectra, and find excellent agreement between the calculated and measured IR and SERS spectra, and good agre ement between the calculated and measured SEHRS spectrum. We find that the apparently overlapping IR, SERS, and SEHRS bands are in fact due to modes that have similar vibrational characteristics but different s ymmetry. Our results indicate that SEHRS spectra are consistent with t he expected (three photon) selection rules and intensities. This rules out an alternative mechanism in which the observed spectrum arises fr om surface second harmonic generation (SHG) followed by SERS excited a t the second harmonic frequency. (C) 1996 American Institute of Physic s.