2019
DOI: 10.1039/c9cp02230a
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Electronic spectra of flavin in different redox and protonation states: a computational perspective on the effect of the electrostatic environment

Abstract: This study discusses how UV/vis absorption spectra of flavin in different redox and protonation states are shifted by the nearby electrostatic microenvironment.

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Cited by 46 publications
(87 citation statements)
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References 99 publications
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“…44 , here, and also in the accompanying article 56 ). Potentially negatively charged amino acids also do not produce a substantial blue shift, contrary to what might have been expected from the electrostatic tuning maps 42,72 . Evidently, Glu148 and Asp148 either do not interact with FMN, or interact with it in the protonated form (hydrogen-bonded conformation in Figure 4E).…”
Section: Discussioncontrasting
confidence: 65%
“…44 , here, and also in the accompanying article 56 ). Potentially negatively charged amino acids also do not produce a substantial blue shift, contrary to what might have been expected from the electrostatic tuning maps 42,72 . Evidently, Glu148 and Asp148 either do not interact with FMN, or interact with it in the protonated form (hydrogen-bonded conformation in Figure 4E).…”
Section: Discussioncontrasting
confidence: 65%
“…4 A physically more appealing alternative for modeling the band broadening is to take vibronic effects into account by explicitly calculating the coupling between vibrational motion and electronic transitions. [2][3][4][12][13][14][15][16][17][18][19][20][21][22] Since the molecular structure of the excited state differs from the molecular structure of the ground-state, the absorption intensity depends on Franck-Condon factors, 23 which are according to the Franck-Condon principle in the first approximation proportional to the square of the overlap of the vibrational wave functions of the ground and excited electronic states. Since the molecular structures of the two states are different, the normal coordinates of the vibrational modes are also different leading to the Duschinsky effect.…”
Section: Introductionmentioning
confidence: 99%
“…Both N286A (results not shown) and Q258A‐N286A, for reasons which are obvious in model F of Figure 1, fail to produce the WT LOV spectrum exhibited in Figure 2. A small peak around 415 nm though matches neutral hydroquinone state of flavin in time‐dependent density functional theory calculations, 28 presence of doublet at 360 and 378 nm makes the spectrum difficult to explain. However, the spectral characteristics in the visible region do not completely match with neutral hydroquinone state of protein‐bound flavin 31 .…”
Section: Resultsmentioning
confidence: 96%
“…Such dark‐state contacts are necessary for the depiction of discrete vibronic structures with an absorption maximum at 447 nm. A recent study considered “Electrostatic Spectral Tuning Maps (ESTM)” 28 for simulating UV‐vis spectrum of the flavin chromophore. It is depicted that the nonpolar environment surrounding flavin is primarily responsible for the generation of triple vibronic structures.…”
Section: Resultsmentioning
confidence: 99%