The Raman and surface-enhanced Raman spectra (SERS) of flavone and three of its hydroxy derivatives, 3-hydroxyflavone (3-HF) and 5-hydroxyflavone (5-HF) and quercetin (3,5,7,3 ,4 pentahydroxyflavone) have been obtained. The normal Raman (NR) spectra were taken in the powder form. The SERS spectra were obtained both on Ag colloids and Ag electrode substrates. Assignments of the spectrally observed normal modes were aided by density functional theory (DFT) calculations using the B3LYP functional and the 6-31+G * basis, a split valence polarized basis set with diffuse functions. Excellent fits were obtained for the observed spectra with little or no scaling. The most intense lines of the NR spectra are those in the C O stretching region (near 1600 cm −1 ). These lines are often weakened by proximity to the surface, while other lines at lower wavenumbers, due to in-plane ring stretches, tend to be strongly enhanced. The SERS spectrum of flavone is weak both on the colloid and on the electrode, indicating weak attachment to the surface. In contrast, the SERS spectra of the hydroxy derivatives of flavone are intense, indicating the assistance of OH groups in attachment to the surface. The spectra of the various species are compared, and a case study of application to detection of a textile dye (Persian berries), which contains quercetin, is presented.
Normal Raman (NR) and surface enhanced Raman scattering (SERS) spectra of 3-hydroxyflavone (3-HF)
have been measured. The SERS spectra are obtained both on an electrode surface and on Ag colloid. Spectral
bands are assigned using DFT calculations for the NR, SERS, and FTIR spectra. The IR, normal Raman, and
SERS results are compared and in conjunction with a DFT calculation are used to interpret the low-frequency
carbonyl stretching vibration in 3-HF. The experimental results support the DFT geometry calculations, which
show that an adatom site at the vertex of Ag20 cluster binding with the 3-HF molecular plane tilted at an
angle of about 53° to the surface is a low-energy structure. This is consistent with the enhancement of in-plane vibrational modes.
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