Hydrogen-surface reactions during the growth of hydrogenated amorphous silicon by reactive magnetron sputtering: A real time kinetic study by in situ infrared absorption
- 15 June 1995
- journal article
- research article
- Published by AIP Publishing in Journal of Applied Physics
- Vol. 77 (12) , 6247-6256
- https://doi.org/10.1063/1.359156
Abstract
This article experimentally identifies the hydrogen incorporation and release processes which control the final hydrogen content of hydrogenated amorphous silicon films (a‐Si:H). We deposit films using reactive magnetron sputtering of a silicon target in an Ar and H2 atmosphere. Hydrogen incorporation or loss is measured using real time infrared reflectance spectroscopy. An optical cavity substrate increases the sensitivity, allowing us to observe Si–H bonding in layers ≥5 Å thick via the stretching mode absorption (1800–2300 cm−1). We observe a narrow component at ∼2100 cm−1 corresponding to all SiHx bonds on the physical surface; the line width allows us to distinguish this contribution from the broader bulk modes. Various combinations of growth flux (isotope labeling, hydrogen partial pressure between 0.1 and 2.0 mTorr) and substrate material (on SiO2, a‐Si, or a‐Si:D) at substrate temperatures between 120 and 350 °C are used to distinguish various mechanisms. From the deposition of a‐Si:H films on SiO2, we quantify the H surface coverage at the end of the nucleation stage (10 Å of growth) to be 1.2±0.3×1015 cm−2, essentially independent of growth conditions. From the evolution of Si–H bonding during the initial growth (≤25 Å), we infer a reduction of the surface area (smoothening) during nucleation and coalescence. During a‐Si:H growth on unhydrogenated a‐Si, we observe H implantation up to a depth of 40 Å, and derive the total flux of arriving H as a function of hydrogen partial pressure. For the exposure of a‐Si:H to atomic deuterium and of a‐Si:D to atomic H, we observe a loss/gain of surface H due to abstraction or exchange reactions. When a‐Si:D or a‐Si films are deposited on a‐Si:H films, we observe H loss from the bulk of the film due to fast particle bombardment at the growing surface. Based on the experimental evidence, we discuss the dependence of various H incorporation and release processes on the incident H flux, substrate temperature, and deposition rate.This publication has 36 references indexed in Scilit:
- Deposition of device quality a-Si:H films with the hot-wire techniqueJournal of Non-Crystalline Solids, 1993
- Deposition of a-Si:H with the hot-wire techniqueJournal of Non-Crystalline Solids, 1993
- Towards high deposition rates of a-Si:H: The limiting factorsJournal of Non-Crystalline Solids, 1993
- Plasma deposition of hydrogenated amorphous silicon: Studies of the growth surfaceApplied Physics A, 1993
- Defect density and hydrogen bonding in hydrogenated amorphous silicon as functions of substrate temperature and deposition ratePhilosophical Magazine Part B, 1992
- Deposition of device quality, low H content amorphous siliconJournal of Applied Physics, 1991
- Role of Atomic Hydrogen During Growth of Hydrogenated Amorphous Silicon in the “Chemical Annealing”Japanese Journal of Applied Physics, 1991
- Energetic particle fluxes in magnetron sputter deposition of a-Si:HJournal of Non-Crystalline Solids, 1991
- In Situ Measurements of Hydrogen Flux, Surface Coverage, Incorporation and Desorption During Magnetron Sputter-Deposition of A-SI:H.MRS Proceedings, 1991
- Hydrogenated microvoids and light-induced degradation of amorphous-silicon solar cellsApplied Physics A, 1986