2009
DOI: 10.1016/j.chemphys.2008.11.008
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Conformations and vibrational properties of disulfide bridges: Potential energy distribution in the model system diethyl disulfide

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Cited by 23 publications
(20 citation statements)
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“…Raman spectroscopy (Figure b) provides significant structural insight into the materials, both in the pristine state and at different states of charge. The pristine disulfide powder displays a strong disulfide peak at 480 cm −1 , assigned from previous literature . Also seen is a strong aromatic C−S mode at 1050 cm −1 , as well as an aromatic C−C mode at 1450 cm −1 (Figure b).…”
Section: Methodssupporting
confidence: 62%
“…Raman spectroscopy (Figure b) provides significant structural insight into the materials, both in the pristine state and at different states of charge. The pristine disulfide powder displays a strong disulfide peak at 480 cm −1 , assigned from previous literature . Also seen is a strong aromatic C−S mode at 1050 cm −1 , as well as an aromatic C−C mode at 1450 cm −1 (Figure b).…”
Section: Methodssupporting
confidence: 62%
“…Because of its extreme simplicity, this Raman‐based conformational rule has received a great attention, not only for analyzing the disulfide markers of simple model compounds but also in the structural analysis of disulfide linkages in peptides and proteins . Meanwhile, the increasing progress in quantum chemistry calculations could bring the proof of reliability for the aforementioned simple rule by means of the Hartree–Fock and density functional theory data obtained basically from diethyl disulfide (Scheme (c)). Nevertheless, despite the fact that diethyl disulfide represents quite well the close vicinity of a disulfide bridge, simply by the presence of ‐S‐C‐ bonds, it completely fails to mimic a correct environment for the two α ‐carbon atoms included in a cystine (Cys‐Cys) unit (Scheme (a)).…”
Section: Introductionmentioning
confidence: 96%
“…Peaks at 510 ± 5, 525 ± 5, and 540 ± 5 cm −1 were assigned to SS stretching vibrations of gauche‐gauche‐gauche (g‐g‐g), gauche‐gauche‐trans (g‐g‐t), and trans‐gauche‐trans (t‐g‐t) conformers, respectively . Among the three conformers, g‐g‐g conformer was energetically most stable . As shown in Figure , the SS region of 485–570 cm −1 for wool keratin before HTP was dominated by the most stable g‐g‐g conformer.…”
Section: Resultsmentioning
confidence: 99%
“…Table summarizes the assignments of some Raman vibration bands for wool keratin. Peaks at 510 ± 5, 525 ± 5, and 540 ± 5 cm −1 were assigned to SS stretching vibrations of gauche‐gauche‐gauche (g‐g‐g), gauche‐gauche‐trans (g‐g‐t), and trans‐gauche‐trans (t‐g‐t) conformers, respectively . Among the three conformers, g‐g‐g conformer was energetically most stable .…”
Section: Resultsmentioning
confidence: 99%