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Basic Research Needs for Solar Energy Utilization - Office of ...

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Efficient Photoinduced Charge Separation<br />

Both theory and experiment show that there is an optimal free<br />

energy <strong>of</strong> reaction <strong>for</strong> achieving the maximum electron transfer<br />

rate (right, top). Moreover, an important prediction <strong>of</strong> theory is<br />

that the rate <strong>of</strong> an electron transfer reaction slows down when the<br />

free energy <strong>of</strong> reaction becomes very large. The key to observing<br />

this so-called “inverted region” in donor-acceptor molecules is<br />

maintaining a fixed distance between the donor and the acceptor<br />

as the free energy <strong>of</strong> the reaction is changed. The use <strong>of</strong> large<br />

free energies <strong>for</strong> charge recombination to slow these energywasting<br />

reactions is critical to achieving the long charge<br />

separation times essential <strong>for</strong> driving catalysts <strong>for</strong> fuel <strong>for</strong>mation.<br />

As the distance between the donor and the acceptor increases,<br />

the electron transfer rate usually decreases exponentially (right,<br />

upper middle). The largest ratios <strong>of</strong> <strong>for</strong>ward-to-back electron<br />

transfer rates achieved in a molecule having a single donor and<br />

acceptor are about 1,000 to 1 (right, lower middle).<br />

Multi-Step Electron Transfer Provides Long-lived<br />

Charge Separation and Storage<br />

Drawing on inspiration from natural photosynthesis, the initial<br />

photo-induced electron transfer can be followed by one or more<br />

thermal electron (or hole) transfer steps. If each <strong>of</strong> these steps is<br />

optimized with regard to reaction free energy, as indicated above,<br />

and the charges move further apart, long-lived charge separation<br />

at high quantum efficiencies can be achieved (left, bottom). This<br />

has been demonstrated in molecular triads that achieve charge<br />

separation quantum efficiencies in excess <strong>of</strong> 80%, with lifetimes<br />

approaching seconds (right, bottom).<br />

Donor Acceptor (1)<br />

e- Donor Acceptor (1) Acceptor (2)<br />

Fast !<br />

e<br />

Very Slow!<br />

-<br />

Donor Acceptor (1) Acceptor (2)<br />

Fast !<br />

Very Slow!<br />

+<br />

-<br />

Donor Acceptor (1)<br />

+<br />

Donor Acceptor (1)<br />

DESIGNING AN ARTIFICIAL REACTION CENTER<br />

e- e- Acceptor (2)<br />

Acceptor (2)<br />

Fast !<br />

-<br />

Acceptor (2)<br />

42<br />

Rate Constant s -1<br />

Rate Constant (s -1 )<br />

Electron Transfer Rate vs. Free <strong>Energy</strong> <strong>of</strong> Reaction<br />

10 12<br />

10 11<br />

10 10<br />

10 9<br />

Normal Region<br />

Optimal Rate<br />

Inverted Region<br />

10<br />

0.0 0.5 1.0 1.5 2.0<br />

8<br />

-ΔG (eV)<br />

10 12<br />

10 11<br />

10 10<br />

10 9<br />

10 8<br />

0 2 4 6 8 10<br />

Donor-Acceptor Distance (Å)<br />

Donor Acceptor<br />

Donor Acceptor<br />

e- Donor Acceptor<br />

e- +<br />

Fast ! Slow<br />

-<br />

Donor Acceptor<br />

Carotene-Porphyrin-Fullerene Triad<br />

H<br />

N C<br />

O<br />

N N<br />

H<br />

N N<br />

H<br />

N<br />

CH3

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