Combined experimental and modeling studies of microwave activated CH4/H2/Ar plasmas for microcrystalline, nanocrystalline, and ultrananocrystalline diamond deposition
- 1. School of Chemistry, University of Bristol, Bristol, BS8 1TS (United Kingdom)
- 2. Skobel'tsyn Institute of Nuclear Physics, Moscow State University, Leninskie gory, Moscow, 119991 (Russian Federation)
Description
A comprehensive study of microwave (MW) activated CH4/H2/Ar plasmas used for diamond chemical vapor deposition is reported, focusing particularly on the effects of gross variations in the H2/Ar ratio in the input gas mixture (from H2/Ar mole fraction ratios of > 10:1, through to ∼1:99). Absolute column densities of C2(a) and CH(X) radicals and of H(n = 2) atoms have been determined by cavity ringdown spectroscopy, as functions of height (z) above a substrate and of process conditions (CH4, H2, and Ar input mole fractions, total pressure, p, and input microwave power, P). Optical emission spectroscopy has also been used to explore the relative densities of electronically excited H atoms, and CH, C2, and C3 radicals, as functions of these same process conditions. These experimental data are complemented by extensive 2D (r, z) modeling of the plasma chemistry, which provides a quantitative rationale for all of the experimental observations. Progressive replacement of H2 by Ar (at constant p and P) leads to an expanded plasma volume. Under H2-rich conditions, > 90% of the input MW power is absorbed through rovibrational excitation of H2. Reducing the H2 content (as in an Ar-rich plasma) leads to a reduction in the absorbed power density; the plasma necessarily expands in order to accommodate a given input power. The average power density in an Ar-rich plasma is much lower than that in an H2-rich plasma operating at the same p and P. Progressive replacement of H2 by Ar is shown also to result in an increased electron temperature, an increased [H]/[H2] number density ratio, but little change in the maximum gas temperature in the plasma core (which is consistently ∼3000 K). Given the increased [H]/[H2] ratio, the fast H-shifting (CyHx + H ↔ CyHx-1 + H2; y = 1-3) reactions ensure that the core of Ar-rich plasma contains much higher relative abundances of ''product'' species like C atoms, and C2, and C3 radicals. The effects of Ar dilution on the absorbed power dissipation pathways and the various species concentrations just above the growing diamond film are also investigated and discussed.
Additional details
Identifiers
- DOI
- 10.1063/1.3562185;
Publishing Information
- Journal Title
- Journal of Applied Physics
- Journal Volume
- 109
- Journal Issue
- 6
- Journal Page Range
- p. 063307-063307.14
- ISSN
- 0021-8979
- CODEN
- JAPIAU
INIS
- Country of Publication
- United States
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 43017173
- Subject category
- S36: MATERIALS SCIENCE; S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
- Descriptors DEI
- ARGON; CHEMICAL VAPOR DEPOSITION; CRYSTALS; DENSITY; DIAMONDS; ELECTRON TEMPERATURE; EMISSION SPECTROSCOPY; EXCITATION; FLUORESCENCE; HYDROGEN; METHANE; MICROWAVE RADIATION; MIXTURES; NANOSTRUCTURES; PLASMA; POWER DENSITY; SIMULATION; SUBSTRATES; SYNTHESIS
- Descriptors DEC
- ALKANES; CARBON; CHEMICAL COATING; DEPOSITION; DISPERSIONS; ELECTROMAGNETIC RADIATION; ELEMENTS; EMISSION; ENERGY-LEVEL TRANSITIONS; FLUIDS; GASES; HYDROCARBONS; LUMINESCENCE; MINERALS; NONMETALS; ORGANIC COMPOUNDS; PHOTON EMISSION; PHYSICAL PROPERTIES; RADIATIONS; RARE GASES; SPECTROSCOPY; SURFACE COATING
Optional Information
- Notes
- (c) 2011 American Institute of Physics