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46807-G4
Controlled Electron Transfer in Hydrogen Bonded Systems
Ksenija D. Glusac, Bowling Green State University
The aim of our
research is to improve the effectiveness of photoinduced charge-separation
between donors and acceptors. Since the efficiency of this process is tightly correlated
with the performance of solar cells, we expect this work to provide a basic
knowledge for the improvement of photovoltaic devices. In this specific
project, we investigated hydrogen-bonded naphthalimide-pyridine (NI-PYR)
systems, with a goal to learn how to take advantage of H-bond dynamics to
control the electron flow in molecular systems. The NI-PYR derivatives were
designed in such a way so that the initial photoinduced electron transfer from
NI to PYR triggers a proton motion along an H-bonded surface. This in turn is
expected to make the charge recombination thermodynamically and/or kinetically
inefficient. In other words, the H-bonded surface could act as a unidirectional
gate for the electron flow.
To obtain a good
understanding of the chromophore used in our donor-acceptor system, we started
out with the investigation of excited state properties of five NI derivatives.1
The study involved synthesis and solvent-dependent absorption and emission
spectra. Furthermore, the excited state dynamics of these compounds were
analyzed using femtosecond optical and mid-IR pump-probe spectroscopy. While
the optical pump-probe setup has already been available as a part of our shared
laser facility here at BGSU, my group has built a transient absorption setup
that can probe in the mid-IR range. To obtain a better understanding of our
experimental results, we started collaboration with Prof. Christopher Hadad, who
characterized the excited state behavior of NI derivatives using DFT.
One of the main
findings of our work is that the excited state properties of NI derivatives are
characterized by a competition between n,p* and p,p*
excited states. As an example, the figure above presents the transient
absorption spectra of SMe-NI derivative obtained at different time delays after
the excitation pulse. We can see that the initially produced excited state can
be characterized by an excited state absorption with a maximum at ~480 nm. We assign
this state to the S2 excited state of SMe-NI. Over the course of 40
ps, S2 excited state converts to another state that exhibits a
stimulated emission signal at ~500 nm, which we assign to S1 excited
state of SMe-NI.
The information about the
character of these two states was obtained from DFT calculations. The above
figure presents difference density plots of S2 and S1
states in SMe-NI. In the case of S2 excited state, electronic charge
is depleted from lone electron pairs of imide oxygen atoms and a charge is
accumulated at the aromatic rings. This sort of difference density plot is characteristic
of an n,p*
excited state, which is additionally supported by the small oscillator strength
for this transition (f=0.0001). The transition density for the S1
excited state is characteristic of p,p* excited state. In addition, the charge is depleted
from SMe-group, which is indicative of a charge-transfer state.
We further studied
electron transfer dynamics from excited SMe-NI to NO2,CN-PYR.2
The donor-acceptor system was chosen in such a way to enable: (i) photoinduced
electron transfer from NI to PYR and (ii) proton transfer from NI radical
cation to PYR radical anion that are produced upon electron transfer. The main
finding of our work is that the fast deactivation of the excited state occurs
in the H-bonded complex. This effect can be best observed from the figure above,
which presents the dynamics of bleach recovery of the SMe-NI carbonyl-group at
1695 cm-1. As the concentration of the PYR is increased, less
excited state absorption is observed at t=0, suggesting that the deactivation
of the NI excited state in H-bonded complex is faster than the time-resolution
of our instrument (~300 fs).
Unfortunately,
the fast thermal deactivation of the SMe-NI excited state in H-bonded complex
made it impossible to study electron transfer dynamics in NI-PYR systems. To
overcome this problem, we initiated a preparation of covalently bound donor-acceptor
system presented in the scheme above. We are currently in the last step of
synthesis, and we expect this model compound to be better for electron transfer
studies.
Reference:
(1) Pavel
Kucheryavy, G. L., Shubham Vyas, Christopher Hadad, Ksenija D. Glusac,
"Excited State Properties of 4-Substituted Naphthalimides", In Preparation.
(2) Pavel Kucheryavy, G. L., Shubham Vyas,
Christopher Hadad, Ksenija D. Glusac, "Ultrafast Excited State
Deactivation in Hydrogen-Bonded Naphthalimide-Pyridine Donor-Acceptor
Systems", In Preparation.
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