The Resonance Raman Spectrum of the Metalloprotein Ovotransferrin

1974 ◽  
Vol 52 (4) ◽  
pp. 273-280 ◽  
Author(s):  
Paul R. Carey ◽  
N. Martin Young

Using ovotransferrin it is shown that amino-acid side chains forming the metal binding site in coloured metalloproteins can be identified and monitored by resonance Raman spectroscopy. All major features above 800 cm−1 in the resonance Raman spectrum of iron–bicarbonate ovotransferrin could be assigned to histidine or tyrosine vibrational modes, by comparison with Raman and infrared data for these amino acids and related compounds. Comparison of the features due to ring modes of imidazole ligated to Fe3+ in ovotransferrin with those of aqueous histidine at pH 8.0 suggests that rearrangement of the ring π electrons takes place upon ligation. Although iron–bicarbonate and iron–oxalate ovotransferrin have similar visible absorption spectra, differences in their resonance Raman spectra are clearly distinguishable, but no evidence was found for the direct binding of bicarbonate or oxalate to the iron. Differences between the geometries of the two sites at which iron is bound in iron–bicarbonate ovotransferrin appeared to be small compared with the perturbation caused to these sites by replacing bicarbonate with oxalate.

1994 ◽  
Vol 48 (7) ◽  
pp. 822-826 ◽  
Author(s):  
Catherine A. Butler ◽  
Ralph P. Cooney ◽  
William A. Denny

The binding of amsacrine [4′-(9-acridinylamino)methanesulfon- m-anisidide] to calf thymus DNA was studied by UV-visible and resonance Raman spectroscopy. A shift of the UV-visible absorption band of amsacrine at 434 to 442 nm together with a decrease in the intensity of this band is observed upon amsacrine-DNA binding. The resonance Raman spectrum of DNA-bound amsacrine shows a general slight decrease in intensity relative to the spectrum of the free species. The significant decrease in intensity of the bands at 1165, 1265, and 1380 cm−1 upon binding to DNA is attributed to the formation of a single amsacrine-DNA species. The assignment of these bands (1165, 1265, and 1380 cm−1), which was based upon a previous normal coordinate analysis (NCA) and molecular neglect of diatomic overlap (MNDO) calculation, and the observed lack of shift in the band positions upon binding are consistent with intercalation being the major binding mode of amsacrine, as inferred previously by other techniques.


1981 ◽  
Vol 59 (6) ◽  
pp. 964-967 ◽  
Author(s):  
S. Sunder ◽  
H. J. Bernstein

Resonance Raman spectra have been obtained for a deuterated crystal violet [p(CH3)2N•C6D4]3C+Cl−, as a dilute aqueous solution. The assignment of some of the strong features seen in the spectra of crystal violet and deuterated crystal violet is discussed.


1979 ◽  
Vol 34 (9) ◽  
pp. 1240-1242 ◽  
Author(s):  
W. Preetz ◽  
G. Peters ◽  
L. Rudzik

Abstract Irradiation of [(n-C4H9)4N]2[Re2l8] at 80 K with exciting laser lines, which approximately coincide with the electronic band maximum at 520 nm, exhibits resonance Raman spectra. Overtone progressions of ν1(Re-Re) and ν2(Re-I), both A1g, and many combination tones are observed. The spectroscopic constants are calculated to be ω1 =258,5 cm -1 , x11 = - 0,42 cm-1 ; ω2 -153,0 cm-1 , x12 = - 0,32 cm-1.


1970 ◽  
Vol 25 (10) ◽  
pp. 1394-1400 ◽  
Author(s):  
W. Krasser ◽  
H. W. Nürnberg

Abstract The thiocyanates of the transition metals iron, cobalt, copper as well as of rhenium and of tech-netium appear in solution as strongly coloured complexes. The resonance raman bands in the sol-vent acetonitrile are investigated. To achieve an unambiguous identification the infrared spectra were recorded too. The change in position and structure of the acetonitrile bands indicates strong complexation of iron, cobalt and copper with acetonitrile, thus indicating the existence of mixed acetonitrile-thiocyanate complexes. The resonance raman spectra of the rhenium-and technetium-thiocyanates present as tetramethyl ammonium salts show however no raman-and infrared-bands of complexed acetonitrile molecules.In the raman spectrum of the thiocyanates of iron, cobalt and copper mainly the totally sym-metric C≡N, S-C, Me-S and Me-N valence vibrations are observed, among which the S-C vibration shows a remarkably high intensity. Besides, a series of bands is obtained which is inter-preted partly as caused by decay products, and partly as bands of complexed acetonitrile. The thiocyanates of rhenium and of technetium show the three possible valence vibrations only. The high frequency of the S-C valence indicates the N-coordination of the thiocyanate group.


1996 ◽  
Vol 248 (5-6) ◽  
pp. 353-360 ◽  
Author(s):  
Sean H. Gallagher ◽  
Robert S. Armstrong ◽  
Peter A. Lay ◽  
Christopher A. Reed

1977 ◽  
Vol 6 (6) ◽  
pp. 267-272 ◽  
Author(s):  
S. Sufrà ◽  
G. Dellepiane ◽  
G. Masetti ◽  
G. Zerbi

1977 ◽  
Vol 55 (9) ◽  
pp. 1444-1453 ◽  
Author(s):  
Kamal Kumar ◽  
P. R. Carey

The resonance Raman spectra of three pharmacologically important sulfonamides, 4-sulfamyl-4′-dimethylaminoazobenzene (1), 4-sulfamyl-4′-hydroxyazobenzene (2), and 4-sulfamyl-4′-aminoazobenzene (3), are compared with those of analogues lacking the sulfonamide group. The —SO2NH2 moiety does not directly contribute intense or moderately intense bands to the resonance Raman spectra of 1, 2, and 3. However, —SO2NH2 ionization is reflected by frequency changes in a band near 1140 cm−1 and intensity changes in the 1420 cm−1 region. The normal Raman spectrum of 2 confirms that the intensity changes reflect —SO2NH2 ionization rather than unrelated changes in vibronic coupling. The effect of —OH ionization on the resonance Raman spectrum of 2 emphasizes that caution must be exercised when relating spectral perturbations to changes in contributions from valence bond type structures. Resonance Raman excitation profiles for the 1138, 1387, and 1416 cm−1 bands of 2 show that these bands gain intensity by coupling with the electronic transitions in the 240 to 450 nm region and that, more than 1000 cm−1 to the red of λmax, the wavelength dependence can be closely reproduced by the FB type terms of Albrecht and Hutley. The excitation profile for each band shows evidence for structure in the 470 nm region, although lack of sufficient excitation wavelengths prevents accurate estimation of the spacing. Under conditions of rigorous resonance the intense Raman lines all occur in the 1400 cm−1 region, i.e. they are 'bunched' in the region known to contain the —N=N— stretching vibration.


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