STRUCTURAL, OPTICAL, AND ELECTRICAL-PROPERTIES OF NANOCRYSTALLINE SILICON FILMS DEPOSITED BY HYDROGEN PLASMA SPUTTERING

Citation
B. Garrido et al., STRUCTURAL, OPTICAL, AND ELECTRICAL-PROPERTIES OF NANOCRYSTALLINE SILICON FILMS DEPOSITED BY HYDROGEN PLASMA SPUTTERING, Journal of vacuum science & technology. B, Microelectronics and nanometer structures processing, measurement and phenomena, 16(4), 1998, pp. 1851-1859
Citations number
33
Categorie Soggetti
Physics, Applied","Engineering, Eletrical & Electronic
ISSN journal
10711023
Volume
16
Issue
4
Year of publication
1998
Pages
1851 - 1859
Database
ISI
SICI code
1071-1023(1998)16:4<1851:SOAEON>2.0.ZU;2-9
Abstract
Nanocrystalline silicon films were deposited by radio frequency sputte ring in a pure H-2 plasma on glass and monocrystalline [100] silicon a t various substrate temperatures, T-s. The detailed structural, optica l, and electrical analysis of the films has been performed by transmis sion electron microscopy, Raman scattering, infrared spectroscopy, x-r ay diffraction, optical absorption, photoluminescence and electrical m easurements. The data obtained show that, to a significant extent, con trol of the structure and hence of the optical and electrical properti es of the films can be achieved by changing T-s. Increasing T-s from 5 0 to 250 degrees C leads to an increase of the average grain size (fro m a few nm to a few tens of nm) and crystalline fraction (from 37% to 74%) and the optical band gap decreases from 2.40 to 1.95 eV. Hydrogen incorporation, together with T-s, are thought to be at the origin of the resulting microstructure and consequently determine the optical an d transport properties, Moreover, hydrogen content was found to be ass ociated with void formation which induces structure relaxation with ve ry low residual stress. Finally, electrical conductivity in the layers increases by more than six orders of magnitude with T-s. The high dar k conductivity measured from the sample deposited at the highest T-s ( >10(-3) Omega(-1) cm(-1)) and its low activation energy (0.13 eV) are in agreement with the high crystalline fraction of this layer, where t unneling of carriers between the crystallites likely occurs. (C) 1998 American Vacuum Society.