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

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nanoscience. This efficiency objective provides a strong motivation <strong>for</strong> a program <strong>of</strong> basic<br />

research that aims to understand and control all the factors that determine cell per<strong>for</strong>mance in<br />

nanostructured systems. Building this knowledge base will provide the plat<strong>for</strong>m from which to<br />

launch an ef<strong>for</strong>t to achieve efficiencies beyond the Shockley-Queisser limit by incorporation <strong>of</strong><br />

approaches such as multijunction cells and photon up-conversion.<br />

RESEARCH DIRECTIONS<br />

Multiple Charge Carrier Generation<br />

Calculated thermodynamic efficiency limits in single-junction solar cells (~32%) assume that<br />

absorption <strong>of</strong> an individual photon results in the <strong>for</strong>mation <strong>of</strong> a single electron-hole pair and that<br />

all photon energy in excess <strong>of</strong> the energy gap is lost as heat. This limit, however, can be<br />

surpassed via multiple exciton (electron-hole pair) generation (MEG) by single-photon<br />

absorption as was predicted (Nozik 2001; Nozik 2002) and observed optically in PbSe and PbS<br />

quantum dots (Schaller and Klimov 2004; Ellingson et al. 2005). The ability to generate multiple<br />

charge carriers upon absorption <strong>of</strong> one photon could lead to greatly enhanced photocurrent and,<br />

ultimately, to very high efficiency solar cells.<br />

Exploit the Unique Properties <strong>of</strong> Nanostructured Systems to Develop New Cells<br />

with <strong>Solar</strong> Efficiencies <strong>of</strong> 20%<br />

Current mesoporous nanocrystalline films used in dye-sensitized solar cells consist <strong>of</strong> a random<br />

nanoparticle network and a disordered pore structure. Such films are characterized by slow<br />

electron transport. Moreover, because <strong>of</strong> the wide particle distribution and disordered nature <strong>of</strong><br />

the pores, not all <strong>of</strong> the internal surface area <strong>of</strong> a film is accessible to the sensitizer. Also, it is<br />

difficult to fill the pores completely with viscous, quasi-solid, or solid ionically or electronic<br />

conductors, which serve to transfer photogenerated holes away from the sensitizers following<br />

charge separation. Development <strong>of</strong> ordered nanostructured, inorganic electrodes could lead to<br />

more effective incorporation <strong>of</strong> ionically or electronically conducting materials (ionic gels,<br />

polymers, etc.) within the pore structure and potentially to faster charge transport. Also, more<br />

uni<strong>for</strong>mly sized particles coupled with periodic order could facilitate films favoring preferred<br />

crystal faces <strong>for</strong> optimizing charge separation. Developing new stable, near-infrared absorbing<br />

molecular and quantum confined sensitizers with increased red absorbance would allow <strong>for</strong><br />

thinner TiO2 layers, which would result in lower charge recombination and higher overall<br />

efficiency. Confining photons to a high-refractive-index sensitized nanostructured oxide film is<br />

another approach to enhance the red response <strong>of</strong> the cells. For instance, a two-layer structure<br />

consisting <strong>of</strong> submicron spheres and a nanoparticulate TiO2 layer has been used to enhance light<br />

collection owing to multiple scattering. Incorporation <strong>of</strong> more advanced light management<br />

strategies, such as photonic band gaps, also <strong>of</strong>fers promise <strong>for</strong> enhancing the red response <strong>of</strong> the<br />

cell.<br />

Also, relatively unexplored are self-assembling molecular, supermolecular, and inorganic<br />

interface layers having, <strong>for</strong> example, a broad spectral response and/or the electronic capability <strong>of</strong><br />

directing the resulting energy vectorially as excitons or charges toward the nanostructure<br />

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