Abstract:In the present work, density functional theory (DFT) and time‐dependent density functional theory (TDDFT) methods have been performed to explore the ground‐state and excited‐state intramolecular hydrogen bonding interactions for 2‐(4‐(diphenylamino)phenyl)‐3‐hydroxy‐4H‐chromen‐4‐one (2‐DHC) system. We demonstrate that the intramolecular hydrogen bond formed in the ground state should be strengthened in the first single excited state by comparing the bond parameters and infrared (IR) vibrational spectra, which … Show more
“…In other words, via an experimental manner, most of the excited state behaviors are inferred without the most correct explanations. [38][39][40][41][42][43][44][45][46][47][48][49][50] In fact, if the novel functions of the HNIBT molecule are to be developed and applied reasonably in the future, the correct and reasonable explanations of excited-state processes and dynamics should be essential. Therefore, in this work, we intent to elaborate the elementary aspects for the HNIBT system theoretically (i.e., based on density functional theory (DFT) and time-dependent density functional theory (TDDFT) methods).…”
In this work, we devote to explore excited‐state intramolecular proton transfer (ESIPT) behavior for a novel fluorescent molecule naphthalimide‐based 2‐(2‐hydroxyphenyl)‐benzothiazole (HNIBT) [New J. Chem. 2019, 43, 9152.] in toluene and methanol (MeOH) solvents. Exploring weak interactions, stable HNIBT‐enol, and HNIBT‐MeOH‐enol complex can be found in S0 state via TDDFT/B3LYP/6‐311+G(d,p) level. Given photoexcitation, intramolecular hydrogen bond O1H2···N3 of HNIBT‐enol and HNIBT‐MeOH‐enol is dramatically enhanced, which offers impetus for facilitates ESIPT reaction. After repeated comparisons, we verify the unavailability of intermolecular hydrogen bonding effects between HNIBT‐enol and MeOH molecules. In view of excitation, HOMO (π) → LUMO (π*) transition and the changes of electronical densities indeed impulse ESIPT tendency. Via constructing potential energy curves (PECs), for both HNIBT‐enol and HNIBT‐MeOH‐enol complex, the ESIPT could only occur along with intramolecular hydrogen bond O1H2···N3. Through comparison, the potential barrier falls from 4.124 kcal/mol (HNIBT‐enol) to 2.132 kcal/mol (HNIBT‐MeOH‐enol). Therefore, we confirm that the ESIPT of the HNIBT system happens more easily in the MeOH solvent compared with the toluene solvent.
“…In other words, via an experimental manner, most of the excited state behaviors are inferred without the most correct explanations. [38][39][40][41][42][43][44][45][46][47][48][49][50] In fact, if the novel functions of the HNIBT molecule are to be developed and applied reasonably in the future, the correct and reasonable explanations of excited-state processes and dynamics should be essential. Therefore, in this work, we intent to elaborate the elementary aspects for the HNIBT system theoretically (i.e., based on density functional theory (DFT) and time-dependent density functional theory (TDDFT) methods).…”
In this work, we devote to explore excited‐state intramolecular proton transfer (ESIPT) behavior for a novel fluorescent molecule naphthalimide‐based 2‐(2‐hydroxyphenyl)‐benzothiazole (HNIBT) [New J. Chem. 2019, 43, 9152.] in toluene and methanol (MeOH) solvents. Exploring weak interactions, stable HNIBT‐enol, and HNIBT‐MeOH‐enol complex can be found in S0 state via TDDFT/B3LYP/6‐311+G(d,p) level. Given photoexcitation, intramolecular hydrogen bond O1H2···N3 of HNIBT‐enol and HNIBT‐MeOH‐enol is dramatically enhanced, which offers impetus for facilitates ESIPT reaction. After repeated comparisons, we verify the unavailability of intermolecular hydrogen bonding effects between HNIBT‐enol and MeOH molecules. In view of excitation, HOMO (π) → LUMO (π*) transition and the changes of electronical densities indeed impulse ESIPT tendency. Via constructing potential energy curves (PECs), for both HNIBT‐enol and HNIBT‐MeOH‐enol complex, the ESIPT could only occur along with intramolecular hydrogen bond O1H2···N3. Through comparison, the potential barrier falls from 4.124 kcal/mol (HNIBT‐enol) to 2.132 kcal/mol (HNIBT‐MeOH‐enol). Therefore, we confirm that the ESIPT of the HNIBT system happens more easily in the MeOH solvent compared with the toluene solvent.
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