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Deutsche Tagung f ¨ur Forschung mit ... - SNI-Portal

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Materialien/Werkstoffe Poster: Do., 13:00–15:30 D-P383<br />

In situ X-Ray Diffraction Study of the Growth of the Layer-Type Semiconductor<br />

WS2<br />

Klaus Ellmer 1 , Stephan Brunken 1 , Rainald Mientus 2 , Stefan Seeger 1<br />

1 Hahn-Meitner-Institut, Abt. Solare Energetik, Glienicker Str. 100, 14109 Berlin, Germany<br />

– 2 Opto-Trans<strong>mit</strong>ter-Umweltschutz-Technologie e.V., 12555 Berlin, Köpenicker<br />

Str.325b Germany<br />

Transition metal dichalcogenides like WS2 are layer-type semiconductors with energy<br />

band gaps and absorption coefficients which make them candidates for absorber layers<br />

in thin film solar cells. In order to use the advantageous (weak) van der Waals bonding<br />

of the sulfur-terminated (001) lattice planes in these materials thin films have<br />

to be prepared with a strong (001) texture. By time-resolved energy-dispersive X-ray<br />

diffraction (EDXRD) at the beamline F3-HASYLAB, we found that the films always<br />

nucleate with the (001) planes, i.e. the van der Waals planes, parallel to the substrate<br />

surface. For high deposition rates and/or low substrate temperatures a texture crossover<br />

from the (001) to the (100) crystallite orientation occurs during the growth. High<br />

deposition rates, low substrate temperatures or low sputtering pressures lead to a significant<br />

lattice expansion of the crystallites in c direction (up to 3 %). This is most<br />

probably caused by a disturbed or turbostratic film growth induced by the energetic<br />

bombardment during film deposition. Reflected and neutralized energetic ions (Ar 0 ,<br />

S 0 ) from the tungsten target and negative ions (S − ) accelerated in the cathode dark<br />

space constitute the main sources of the energetic bombardment leading to crystallographic<br />

defects. The energy of these particles can be tailored by (i) thermalization<br />

between target and substrate in the sputtering gas or (ii) by a reduction of the discharge<br />

or target voltage, respectively, by a high frequency excitation (13 or 27 MHz) of the<br />

plasma. Another thin film preparation route, which avoids ion-bombardment-induced<br />

defects, is the crystallization of an amorphous sulfur-rich WS3+x (0

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