Abstract

Curcumin, the main yellow bioactive component of turmeric, has recently acquired attention by chemists due its wide range of potential biological applications as an antioxidant, an anti-inflammatory, and an anti-carcinogenic agent. This molecule fluoresces weakly and poorly soluble in water. In this detailed study of curcumin in thirteen different solvents, both the absorption and fluorescence spectra of curcumin was found to be broad, however, a narrower and simple synchronous fluorescence spectrum of curcumin was obtained at Δ λ = 10–20 nm. Lippert–Mataga plot of curcumin in different solvents illustrated two sets of linearity which is consistent with the plot of Stokes’ shift vs. the E T30. When Stokes's shift in wavenumber scale was replaced by synchronous fluorescence maximum in nanometer scale, the solvent polarity dependency measured by λ SFS max vs. Lippert–Mataga plot or E T30 values offered similar trends as measured via Stokes’ shift for protic and aprotic solvents for curcumin. Better linear correlation of λ SFS max vs. π* scale of solvent polarity was found compared to λ abs max or λ em max or Stokes’ shift measurements. In Stokes’ shift measurement both absorption/excitation as well as emission (fluorescence) spectra are required to compute the Stokes’ shift in wavenumber scale, but measurement could be done in a very fast and simple way by taking a single scan of SFS avoiding calculation and obtain information about polarity of the solvent. Curcumin decay properties in all the solvents could be fitted well to a double-exponential decay function.

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