Optical absorption measurements and optoelectronic DFT calculations for ethanol solvated quercetin and anhydrous/hydrated quercetin crystals

UV–vis optical absorption measurements of the ethanol solvated quercetin molecule and the dihydrate triclinic quercetin crystal were performed, as well as the electronic structure of the ethanol solvated quercetin molecule and the properties of anhydrous and mono(di)hydrated quercetin crystals emplo...

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Autores:
de Paula V.F., Jr
Guedes M.I.F.
van Tilburg M.F
Vieira I.G.P.
Silva J.B.
dos Santos R.C.R.
Echeverry J.P.
Costa G
Silva B.P
Maia F.F., Jr.
Caetano E.W.S.
Freire V.N.
Tipo de recurso:
Article of investigation
Fecha de publicación:
2022
Institución:
Universidad de Ibagué
Repositorio:
Repositorio Universidad de Ibagué
Idioma:
eng
OAI Identifier:
oai:repositorio.unibague.edu.co:20.500.12313/5499
Acceso en línea:
https://hdl.handle.net/20.500.12313/5499
Palabra clave:
Mediciones de absorción optica
Cálculos DFT optoelectrónicos
Quercetina disuelta en etanol
Cristales de quercetina
Cristales moleculares hidratados
Cálculos de DFT
Propiedades estructurales
Propiedades optoelectrónicas
Estabilidad relativa
DFT calculations
Ethanol solvated quercetin
Hydrated molecular crystals
Optoelectronic properties
Quercetin crystals
Relative stability
Structural properties
Rights
openAccess
License
http://purl.org/coar/access_right/c_abf2
Description
Summary:UV–vis optical absorption measurements of the ethanol solvated quercetin molecule and the dihydrate triclinic quercetin crystal were performed, as well as the electronic structure of the ethanol solvated quercetin molecule and the properties of anhydrous and mono(di)hydrated quercetin crystals employing Density Functional Theory (DFT) calculations with a dispersion correction scheme. Unit cell geometry optimization of the anhydrous crystal has elucidated the structure of the anhydrous quercetin crystal (space group P21/a, monoclinic). Anhydrous quercetin exhibits a direct bandgap of 2.17 ​eV with large valence band dispersion, suggesting a semiconductor behavior for hole transport. Monohydrate quercetin has an indirect gap of 1.84 ​eV, while the solid dihydrate form has a Kohn-Sham indirect electronic bandgap of 2.00 ​eV, smaller than the experimental optical absorption bandgap of 2.40 ​eV. Applying the Δ-sol gap correction scheme, the bandgaps increase by about 1 ​eV. There is a significant optical anisotropy for all quercetin systems in the solid state, especially for the anhydrous form. © 2022 Elsevier Inc.