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

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Control over Nucleation and Growth <strong>for</strong> Producing High-quality Thin Films<br />

The growth <strong>of</strong> a thin semiconductor layer on an inexpensive substrate usually results in a<br />

polycrystalline material. The properties <strong>of</strong> polycrystalline materials are challenging to study<br />

because each individual grain is likely to have a different size, orientation, shape, surface<br />

termination, structural quality, and impurity content. A variation in any <strong>of</strong> these attributes can<br />

translate into variations in device per<strong>for</strong>mance, and thus an associated reduction in<br />

manufacturing yield.<br />

The challenge <strong>of</strong> characterizing, modeling, and controlling polycrystalline film properties is<br />

<strong>for</strong>midable. Figure 26 illustrates how control over the nucleation and growth can yield control<br />

over grain size, orientation, and shape, and, there<strong>for</strong>e, material quality. The remarkable advances<br />

in nanostructure synthesis over the past decade provide scientists with tremendous opportunities<br />

<strong>for</strong> controlling the structure <strong>of</strong> thin polycrystalline films. Similar advances in materials<br />

characterization tools provide new opportunities <strong>for</strong> quantifying and thus eventually controlling<br />

grain boundaries, defect states, etc. Understanding and controlling thin-film nucleation and<br />

growth are key <strong>for</strong> both achieving high-per<strong>for</strong>mance photovoltaics and <strong>for</strong> achieving practical<br />

success in the manufacturing environment.<br />

Large oriented grains<br />

Misaligned grains<br />

Sparse, oriented<br />

uni<strong>for</strong>m nuclei Non-uni<strong>for</strong>m, nonoriented<br />

nuclei<br />

Film Nucleation<br />

Figure 26 Controlling nucleation and growth<br />

97<br />

Growth<br />

Improve Understanding <strong>of</strong> Carrier Dynamics at Interfaces<br />

Interfaces between different materials are necessary ingredients <strong>of</strong> every type <strong>of</strong> solar cell. Their<br />

number increases with the number <strong>of</strong> different materials and with the complexity <strong>of</strong> the solar cell<br />

structure. Electronic interface states can fall within the band gap but show up also as resonances<br />

isoenergetic with the electronic bulk states. Recent advances in experimental and theoretical<br />

techniques now give access to real-time measurements and modeling <strong>of</strong> the underlying<br />

interfacial charge carrier dynamics on the relevant time scales. The latter range from a few<br />

femtoseconds to milliseconds. The actual energy distribution <strong>of</strong> hot charge carriers in<br />

semiconductors under solar irradiation with up to a thousand-fold concentration can remain nonthermalized<br />

and thus cannot be characterized by the lattice temperature. A realistic description <strong>of</strong><br />

interfacial loss processes requires (a) a model <strong>for</strong> the respective charge carrier dynamics that is<br />

based on the detailed atomic and electronic structure <strong>of</strong> bulk interface and (b) a sufficiently<br />

detailed time-dependent model calculation that comprises all the relevant electronic levels and all

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