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H 2 Raman‐shifted YAG laser ultraviolet Raman spectrometer operating at wavelengths down to 184 nm
Author(s) -
Fodor Stephen P. A.,
Rava Richard P.,
Copeland Robert A.,
Spiro Thomas G.
Publication year - 1986
Publication title -
journal of raman spectroscopy
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.748
H-Index - 110
eISSN - 1097-4555
pISSN - 0377-0486
DOI - 10.1002/jrs.1250170609
Subject(s) - raman spectroscopy , monochromator , laser , optics , chemistry , materials science , raman scattering , analytical chemistry (journal) , coherent anti stokes raman spectroscopy , wavelength , optoelectronics , physics , chromatography
Apparatus is described for the acquisition of Raman spectra with excitation at wavelengths as short as 184 nm. The H 2 Raman‐shifted output of an Nd:YAG laser is directed on to a free‐flowing sample, and the Raman photons are collected and dispersed by a scanning 1.26 m single monochromator equipped with a 2400 groove holographic grating and a solar blind phototube with integrating electronics, or by a 0.5 m spectrograph with an 1800 groove holographic grating and a reticon multi‐channel detector. Data for air‐sensitive samples are obtained by enclosing the sample jet in an inert gas purged shroud equipped with a UV‐transparent optical window. Raman spectra are reported for phenylalanine at a series of excitation wavelengths down to 184 nm. They show a sharp transition between 200 and 192 nm from vibronic to Franck–Condon scattering. At 200 nm, the intensities of the vibronically induced ν 8a and ν 8b modes, at 1606 and 1586 cm −1 , are nearly the same as that of the 1000 cm −1 ν 1 ring breathing mode, whereas at 192 nm the relative intensities of the former bands are dramatically dimished. In contrast, the ν 8a and ν 8b modes of tyrosine continue to show enhancement comparable to the ring breathing modes at 192 nm, the maximum of the strong 1 B α, b tyrosine absorption. The spectrum of insulin at 192 nm shows comparable contributions from tyrosine, phenylalanine and amide vibrations, whereas at 200 and 218 nm excitation the aromatic contributions are dominant.

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