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  <title><![CDATA[Unexpected Electronic Transport Phenomena in Composite Amorphous/nanocrystalline Thin Films]]></title>
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<h4><strong>School of Physics Hard Condensed Matter Seminar, Taylor Distinguished Professor, James Kakalios, University of Minnesota</strong></h4>

<p>Composite materials consisting of nanocrystalline semiconductors embedded within a bulk amorphous semiconductor or an insulator have attracted interest for applications ranging from photovoltaics, thermoelectrics, thin film transistors, particle detectors and electroluminescent devices.&nbsp;</p>

<p>These materials combine the best of both worlds &ndash; the thin film large area advantages of disordered semiconductors with the superior opto-electronic properties of crystals, and often display electronic properties not observed in either material separately.</p>

<p>In undoped nc-Si within hydrogenated amorphous silicon (a-Si:H) (a/nc-Si:H), the dark conductivity increases with crystal fraction, with the largest enhancement of several orders of magnitude observed when the nanocrystalline density corresponds to a crystalline fraction of 2 &ndash; 4%, but decreases for higher nanocrystal content.</p>

<p>The dark conductivity of n-type doped a/nc-Si:H films displays three distinct conduction mechanisms: thermally activated conduction, multi-phonon hopping and Mott variable range hopping, as the crystal fraction and temperature of these films is varied.</p>

<p>Studies of the thermopower of composite films of a-Si:H containing germanium nanocrystals find that transport changes from n-type to p-type as the nc-Ge concentration is increased, with a transition sharper than expected from a standard two-channel model for charge transport. Finally, the conductivity in the nc-Ge/a-Si:H films is described by an anomalous hopping expression, ~ exp[(T<sub>o</sub>/T)<sup>k</sup>] where k = &frac34;, suggesting an entirely new conduction mechanism.</p>

<p>This research done in collaboration with Uwe Kortshagen, C. Blackwell, Y. Adjallah, L. Wienkes, K. Bodurtha, C. Anderson and J. Trask.</p>

<p>This work was partially supported by NSF grants NER-DMI-0403887, DMR-0705675, the NINN Characterization Facility, the Xcel Energy grant under RDF contract #RD3-25, NREL XEA-9-99012-01 and the University of Minnesota.</p>
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