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

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process <strong>of</strong> charge carrier recombination. Transport <strong>of</strong> the resulting charged carriers away from<br />

the interface so as not to <strong>for</strong>m bound interface states is an equally important process to control,<br />

but both these processes are poorly understood. The role <strong>of</strong> interfacial energy <strong>of</strong>f-sets, dipole<br />

layers, exciton binding energy, and spin states must be understood, and their relationships to the<br />

electronic structure <strong>of</strong> the interface are important issues to address.<br />

Semiconductor quantum dots, metal nanoparticles, and carbon nanotubes are all examples <strong>of</strong><br />

species that can be incorporated in an organic host to promote exciton dissociation and/or<br />

additional charge carrier generation and transport. Similarly, photoexcited semiconductor<br />

nanoparticles can undergo charge transfer upon contact with metal nanoclusters (such as gold<br />

and silver). Such charge redistribution can influence the energetics <strong>of</strong> the composite by shifting<br />

the Fermi level. A better understanding <strong>of</strong> the mediating role <strong>of</strong> metal nanoclusters, including<br />

their size and shape dependence on the storage and transport <strong>of</strong> electrons, is needed to design the<br />

next generation <strong>of</strong> hybrid systems. Metal nanoparticles have potential as components <strong>of</strong> the<br />

interconnecting junction in a tandem solar cell, where they act as recombination centers, but they<br />

can also dramatically influence the optical properties <strong>of</strong> the surrounding medium.<br />

Third-generation OPV<br />

To achieve a device with efficiency that approaches 50% will<br />

require the development <strong>of</strong> organic species and device<br />

architectures that can extract more energy from the solar<br />

spectrum than can a single-junction device. The two basic<br />

methods <strong>for</strong> achieving this goal are the development <strong>of</strong><br />

efficient structures <strong>for</strong> up- and down-conversion <strong>of</strong> solar<br />

photons to match an existing, single-junction device; or the<br />

construction <strong>of</strong> multiple, stacked single-junction devices that<br />

are optimized <strong>for</strong> specific wavelengths <strong>of</strong> light within the solar<br />

spectrum (Figure 31).<br />

To achieve these objectives, research into the relationship<br />

between the excited-state properties <strong>of</strong> organic molecules and<br />

their structure is needed. For photons absorbed above the<br />

optical bandgap, such a strategy can lead to systems with the<br />

ability to either down-convert the initial excited excitons into<br />

multiple ground-state excitons and ultimately into multiple<br />

charge carriers, or systems that can facilitate the up-conversion<br />

<strong>of</strong> sub-optical bandgap solar photons into excitons.<br />

The progress made in the direction <strong>of</strong> stacked (tandem) solar<br />

cells will be facilitated by the development <strong>of</strong> new deposition<br />

procedures that can be adapted to provide the required<br />

structures. Such issues as layer thickness and the creation <strong>of</strong><br />

multiple interfaces are nontrivial aspects <strong>of</strong> the problem that<br />

are far from optimized and require attention. Furthermore, the<br />

need <strong>for</strong> materials that can act as interconnectors <strong>for</strong> balanced<br />

105<br />

Figure 31 Schematic <strong>of</strong> a<br />

multi-layered, tandem organic<br />

solar cell with three stacked<br />

solar cells designed to absorb<br />

different solar photons that<br />

enter through the substrate.<br />

Balanced charge transport in<br />

each cell is indicated with<br />

efficient recombination at the<br />

two interconnectors.

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