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

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Multiple Exciton Generation <strong>Solar</strong> Cells<br />

A central limitation <strong>of</strong> existing solar cell approaches is the one-to-one relationship between an<br />

absorbed photon and a generated electron-hole pair. The process <strong>of</strong> impact ionization, known <strong>for</strong><br />

decades in bulk semiconductor crystals, allows the conversion <strong>of</strong> single high-energy photons to<br />

multiple electron-hole pairs (Kolodinski et al. 1993), but with relatively low efficiency. Recent<br />

experimental reports <strong>of</strong> multiple exciton generation (MEG) in nano-sized (quantum dot)<br />

semiconductors indicate much more efficient generation <strong>of</strong> multiple electron-hole pairs<br />

compared to bulk materials (see Figure 22). For example, semiconductor quantum dots <strong>of</strong> PbSe<br />

and PbS have demonstrated high efficiencies <strong>of</strong> multiple exciton generation, producing as many<br />

as three excitons per absorbed photon (Schaller and Klimov 2004; Ellingson et al. 2005). While<br />

the basic physical phenomenon has been demonstrated, additional challenges remain, including<br />

efficient transfer and extraction <strong>of</strong> the generated charges from the nano-structured materials.<br />

Figure 22 Multiple exciton generation in quantum dots. Because <strong>of</strong> quantum<br />

confinement in the small nanoscale semiconductor QD particle, the energy levels <strong>for</strong><br />

electrons and holes are discrete. This slows hot exciton cooling and enhances multiple<br />

exciton <strong>for</strong>mation. A single absorbed photon that has an energy at least 3 times the<br />

energy difference between the first energy levels <strong>for</strong> electrons and holes in the QD can<br />

create 3 excitons. The bandgap <strong>of</strong> the bulk semiconductor is indicated as Eg.<br />

93

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