Combined experimental and modeling studies of microwave activated CH4/H2/Ar plasmas for microcrystalline, nanocrystalline, and ultrananocrystalline diamond deposition

被引:37
作者
Richley, James C. [1 ]
Fox, Oliver J. L. [1 ]
Ashfold, Michael N. R. [1 ]
Mankelevich, Yuri A. [2 ]
机构
[1] Univ Bristol, Sch Chem, Bristol BS8 1TS, Avon, England
[2] Moscow MV Lomonosov State Univ, Skobeltsyn Inst Nucl Phys, Moscow 119991, Russia
基金
英国工程与自然科学研究理事会;
关键词
GAS-PHASE CHEMISTRY; R-MATRIX METHOD; DISSOCIATIVE RECOMBINATION; THIN-FILMS; GROWTH; SPECTROSCOPY; MIXTURES; IONS; C-2; DENSITIES;
D O I
10.1063/1.3562185
中图分类号
O59 [应用物理学];
学科分类号
摘要
A comprehensive study of microwave (MW) activated CH4/H-2/Ar plasmas used for diamond chemical vapor deposition is reported, focusing particularly on the effects of gross variations in the H-2/Ar ratio in the input gas mixture (from H-2/Ar mole fraction ratios of > 10:1, through to similar to 1:99). Absolute column densities of C-2(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, H-2, 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, C-2, and C-3 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 H-2 by Ar (at constant p and P) leads to an expanded plasma volume. Under H-2-rich conditions, > 90% of the input MW power is absorbed through rovibrational excitation of H-2. Reducing the H-2 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 H-2-rich plasma operating at the same p and P. Progressive replacement of H-2 by Ar is shown also to result in an increased electron temperature, an increased [H]/[H-2] number density ratio, but little change in the maximum gas temperature in the plasma core (which is consistently similar to 3000 K). Given the increased [ H]/[ H-2] ratio, the fast H-shifting (CyHx + H <-> CyHx-1 + H-2; y=1-3) reactions ensure that the core of Ar-rich plasma contains much higher relative abundances of "product" species like C atoms, and C-2, and C-3 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. (C) 2011 American Institute of Physics. [doi:10.1063/1.3562185]
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页数:14
相关论文
共 51 条
[1]   Interpretation of the Raman spectra of ultrananocrystalline diamond [J].
Birrell, J ;
Gerbi, JE ;
Auciello, O ;
Gibson, JM ;
Johnson, J ;
Carlisle, JA .
DIAMOND AND RELATED MATERIALS, 2005, 14 (01) :86-92
[2]   Understanding the chemical vapor deposition of diamond: recent progress [J].
Butler, J. E. ;
Mankelevich, Y. A. ;
Cheesman, A. ;
Ma, Jie ;
Ashfold, M. N. R. .
JOURNAL OF PHYSICS-CONDENSED MATTER, 2009, 21 (36)
[3]   Investigation of the combined effect of argon addition and substrate bias on the growth of ultrananocrystalline diamond layers [J].
Csikvari, P. ;
Somogyi, A. ;
Veres, M. ;
Hars, Gy. ;
Toth, A. .
DIAMOND AND RELATED MATERIALS, 2009, 18 (12) :1459-1465
[4]   ON THE FORMATION OF THE FULLERENES [J].
CURL, RF .
PHILOSOPHICAL TRANSACTIONS OF THE ROYAL SOCIETY OF LONDON SERIES A-MATHEMATICAL PHYSICAL AND ENGINEERING SCIENCES, 1993, 343 (1667) :19-32
[5]   The role of inert gas in MW-enhanced plasmas for the deposition of nanocrystalline diamond thin films [J].
Fox, O. J. L. ;
Ma, J. ;
May, P. W. ;
Ashfold, M. N. R. ;
Mankelevich, Yu. A. .
DIAMOND AND RELATED MATERIALS, 2009, 18 (5-8) :750-758
[6]   Validation of actinometry for estimating relative hydrogen atom densities and electron energy evolution in plasma assisted diamond deposition reactors [J].
Gicquel, A ;
Chenevier, M ;
Hassouni, K ;
Tserepi, A ;
Dubus, M .
JOURNAL OF APPLIED PHYSICS, 1998, 83 (12) :7504-7521
[7]   SPECTROSCOPIC ANALYSIS AND CHEMICAL-KINETICS MODELING OF A DIAMOND DEPOSITION PLASMA REACTOR [J].
GICQUEL, A ;
HASSOUNI, K ;
FARHAT, S ;
BRETON, Y ;
SCOTT, CD ;
LEFEBVRE, M ;
PEALAT, M .
DIAMOND AND RELATED MATERIALS, 1994, 3 (4-6) :581-586
[8]  
Goodwin D.G., 1998, HANBOOK IND DIAMONDS, P527
[9]   A quasianalytic kinetic model for nonequilibrium C2H2(1%)/H2/Ar RF plasmas of interest in nanocrystalline diamond growth [J].
Gordillo-Vázquez, FJ ;
Albella, JM .
PLASMA SOURCES SCIENCE & TECHNOLOGY, 2002, 11 (04) :498-512
[10]   Spectroscopic determination of carbon dimer densities in Ar-H2-CH4 and Ar-H2-C60 plasmas [J].
Goyette, AN ;
Lawler, JE ;
Anderson, LW ;
Gruen, DM ;
McCauley, TG ;
Zhou, D ;
Krauss, AR .
JOURNAL OF PHYSICS D-APPLIED PHYSICS, 1998, 31 (16) :1975-1986