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Vibronic and Cationic Features of 2-Fluorobenzonitrile and 3-Fluorobenzonitrile Studied by REMPI and MATI Spectroscopy and Franck–Condon Simulations

Fluorinated organic compounds have superior physicochemical properties than general organic compounds due to the strong C-F single bond; they are widely used in medicine, biology, pesticides, and materials science. In order to gain a deeper understanding of the physicochemical properties of fluorina...

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Detalles Bibliográficos
Autores principales: Li, Shuxian, Zhao, Yan, Jiao, Yuechun, Zhao, Jianming, Li, Changyong, Jia, Suotang
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10302412/
https://www.ncbi.nlm.nih.gov/pubmed/37375257
http://dx.doi.org/10.3390/molecules28124702
Descripción
Sumario:Fluorinated organic compounds have superior physicochemical properties than general organic compounds due to the strong C-F single bond; they are widely used in medicine, biology, pesticides, and materials science. In order to gain a deeper understanding of the physicochemical properties of fluorinated organic compounds, fluorinated aromatic compounds have been investigated by various spectroscopic techniques. 2-fluorobenzonitrile and 3-fluorobenzonitrile are important fine chemical intermediates and their excited state S(1) and cationic ground state D(0) vibrational features remain unknown. In this paper, we used two-color resonance two photon ionization (2-color REMPI) and mass analyzed threshold ionization (MATI) spectroscopy to study S(1) and D(0) state vibrational features of 2-fluorobenzonitrile and 3-fluorobenzonitrile. The precise excitation energy (band origin) and adiabatic ionization energy were determined to be 36,028 ± 2 cm(−1) and 78,650 ± 5 cm(−1) for 2-fluorobenzonitrile and 35,989 ± 2 cm(−1) and 78,873 ± 5 cm(−1) for 3-fluorobenzonitrile, respectively. The density functional theory (DFT) at the levels of RB3LYP/aug-cc-pvtz, TD-B3LYP/aug-cc-pvtz, and UB3LYP/aug-cc-pvtz were used to calculate the stable structures and vibrational frequencies for the ground state S(0), excited state S(1), and cationic ground state D(0), respectively. Franck–Condon spectral simulations for transitions of S(1) ← S(0) and D(0) ← S(1) were performed based on the above DFT calculations. The theoretical and experimental results were in good agreement. The observed vibrational features in S(1) and D(0) states were assigned according to the simulated spectra and the comparison with structurally similar molecules. Several experimental findings and molecular features were discussed in detail.