Density functional
theory and its time-dependent extension are
employed to investigate the intermolecular hydrogen-bonding- (Inter-HB-)
induced fluorescence enhancement of benzaldehydes. The fluorescence
quenching mechanism of benzaldehydes in chloroform is attributed to
the low energy gap between the lowest ππ* and nπ*
states at Franck–Condon (FC) point and conical interaction
between ππ* and nπ* states. The Inter-HB between
the aldehyde group of benzaldehydes and methanol can considerably
increase the energy gap between ππ* and nπ* states
at the FC point, and this type of hydrogen bond is strengthened in
the excited ππ* state, thereby precluding the nonradiative
transition from nπ* state and enhancing fluorescence. The Inter-HB
between the hydroxy group of benzaldehydes and methanol is considerably
stronger than that between the aldehyde group of benzaldehydes and
methanol; which has a little effect on the energy gap of ππ*
and nπ* states. Therefore, if Inter-HB exists between the hydroxy
group of benzaldehydes and methanol, then it will play an important
role in ground and excited ππ* states, and fluorescence
enhancement by Inter-HB between the aldehyde group of benzaldehydes
and methanol will be absent. Our proposed mechanism can explain the
experimental observations and differs from that of “proximity
effects”.
Heteroatom substitution of gold nanoclusters enables precise tuning of their physicochemical properties at single-atom level, which has importance impact on the applications related to excited states including photovoltaic, photocatalysis and...
To achieve efficient conversion and avoid loss of solar energy, ultrafast charge separation and slow electron−hole recombination are desired. Combining timedependent density functional theory (TD-DFT) with nonadiabatic molecular dynamics, Au 9 (PH 3 ) 8 /MoS 2 , as a prototype for zero-dimensional/two-dimensional (0D/2D) heterojunction, has been demonstrated to present excellent light absorption capacity and effective charge separation characteristics. In the heterojunction, photoexcitation of the Au 9 (PH 3 ) 8 nanocluster drives an ultrafast electron transfer from Au 9 (PH 3 ) 8 to MoS 2 within 20 fs, whereas photoexcitation of the MoS 2 nanosheet leads to hole transfer from MoS 2 to Au 9 (PH 3 ) 8 within 680 fs. The strong nonadiabatic coupling and prominent density overlap are responsible for the faster electron separation relative to hole separation. In competition with the charge separation, electron−hole recombination requires 205 ns, ensuring an effective carrier separation. Our atomistic TD-DFT simulation provides valuable insights into the photocarrier dynamics at the Au 9 (PH 3 ) 8 /MoS 2 interface, which would stimulate the exploration of 0D/2D hybrid materials for photovoltaic and optoelectronic devices.
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