The absorption spectra of bilirubins were deconvoluted by two gaussian curves of equal widths representing the exciton bands of the non degenerate molecular system. The two bands were used to study the wavelength dependence of the (4Z,15Z)®(4Z,15E) configurational photoisomerisation quantum yield of the bichromophoric bilirubin-IXa (BR-IX), the intrinsically asymmetric bile pigment associated with jaundice and the symmetrically-substituted bilirubins (bilirubin-IIIa and mesobilirubin-XIIIa), when they are irradiated in aqueous solution bound to human serum albumin (HSA). The same study was performed for BR-IX in ammoniacal methanol solution (NH4OH/MeOH). The quantum yields of the configurational photoprocesses were fitted with a combination function of the two gaussian bands normalised to the total absorption, using the proportionality coefficients and a scaling factor as parameters. The decrease of the (4Z,15Z)® (4Z,15E) quantum yield with increasing wavelengths, which occurs for wavelengths longer than the most probable Franck-Condon transition of the molecule, did not result an unique function of the exciton absorptions. In particular we found two ranges corresponding to different exciton interactions with different proportionality coefficients and scaling factors. The wavelength dependent photoisomerisation of bilirubins was described as an abrupt change in quantum yield as soon as the excitation resulted strongly localised in each chromophores. The change was correlated to a variation of the interaction between the two chromophores when the short wavelength exciton absorption has become vanishing small. With the help of the circular dichroism (CD) spectrum of BR-IX in HSA, a small band was resolved in bilirubin absorption spectrum, delivering part of the energy required for the (4Z,15Z)®(4Z,15E) photoisomerisation of the molecule.

Analysis of Wavelenght Dependent Photoisomerisation Quantum Yields in Bilirubins by Two Exciton Absorption Bands Fitting

Mazzoni M;Agati G;
2003

Abstract

The absorption spectra of bilirubins were deconvoluted by two gaussian curves of equal widths representing the exciton bands of the non degenerate molecular system. The two bands were used to study the wavelength dependence of the (4Z,15Z)®(4Z,15E) configurational photoisomerisation quantum yield of the bichromophoric bilirubin-IXa (BR-IX), the intrinsically asymmetric bile pigment associated with jaundice and the symmetrically-substituted bilirubins (bilirubin-IIIa and mesobilirubin-XIIIa), when they are irradiated in aqueous solution bound to human serum albumin (HSA). The same study was performed for BR-IX in ammoniacal methanol solution (NH4OH/MeOH). The quantum yields of the configurational photoprocesses were fitted with a combination function of the two gaussian bands normalised to the total absorption, using the proportionality coefficients and a scaling factor as parameters. The decrease of the (4Z,15Z)® (4Z,15E) quantum yield with increasing wavelengths, which occurs for wavelengths longer than the most probable Franck-Condon transition of the molecule, did not result an unique function of the exciton absorptions. In particular we found two ranges corresponding to different exciton interactions with different proportionality coefficients and scaling factors. The wavelength dependent photoisomerisation of bilirubins was described as an abrupt change in quantum yield as soon as the excitation resulted strongly localised in each chromophores. The change was correlated to a variation of the interaction between the two chromophores when the short wavelength exciton absorption has become vanishing small. With the help of the circular dichroism (CD) spectrum of BR-IX in HSA, a small band was resolved in bilirubin absorption spectrum, delivering part of the energy required for the (4Z,15Z)®(4Z,15E) photoisomerisation of the molecule.
2003
Istituto di Fisica Applicata - IFAC
Fotoisomerizzazione
Dicroismo circolare
Eccitoni
Bilirubine
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/22390
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