Effects of microwave power on the structural and emission properties of hydrogenated amorphous silicon carbide deposited by electron cyclotron resonance chemical vapor deposition

Citation
Sf. Cui, J",rusli,"yoon et al., Effects of microwave power on the structural and emission properties of hydrogenated amorphous silicon carbide deposited by electron cyclotron resonance chemical vapor deposition, J APPL PHYS, 89(5), 2001, pp. 2699-2705
Citations number
54
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
JOURNAL OF APPLIED PHYSICS
ISSN journal
00218979 → ACNP
Volume
89
Issue
5
Year of publication
2001
Pages
2699 - 2705
Database
ISI
SICI code
0021-8979(20010301)89:5<2699:EOMPOT>2.0.ZU;2-S
Abstract
Hydrogenated amorphous silicon carbide (a-Si1-xCx:H) films have been deposi ted using an electron cyclotron resonance chemical vapor deposition system. The effects of varying the microwave power from 100 to 1000 W on the depos ition rate, optical band gap, film composition, and disorder were studied u sing various techniques such as Rutherford backscattering spectrometry, spe ctrophotometry, Fourier-transform infrared absorption, and Raman scattering . Samples deposited at 100 W are found to have a carbon fraction (x) of 0.4 9 which is close to that of stoichiometric SiC, whereas samples deposited a t higher microwave powers are carbon rich with x which are nearly independe nt of the microwave power. The optical gaps of the films deposited at highe r microwave powers were noted to be related to the strength of the C-H-n bo nd in the films. The photoluminescence (PL) peak emission energy and bandwi dth of these films were investigated at different excitation energies (E-ex ) and correlated to their optical band gaps and Urbach tail widths. Using a n E-ex of 3.41 eV, the PL peak energy was found to range from 2.44 to 2.79 eV, with the lowest value corresponded to an intermediate microwave power o f 600 W. At increasing optical gap, the PL peak energy was found to be blue shifted, accompanied by a narrowing of the bandwidth. Similar blueshift was also observed at increasing E-ex, but in this case accompanied by a broade ning of the bandwidth. These results can be explained using a PL model for amorphous semiconductors based on tail-to-tail states radiative recombinati on. A linear relation between the full width at half maximum of the PL spec tra and the Urbach energy was also observed, suggesting the broadening of t he band tail states as the main factor that contributes to the shape of the PL spectra observed. (C) 2001 American Institute of Physics.