Jul 2 – 6, 2018
Žofín Palace
Europe/Prague timezone

P4.3002 Self-consistent simulation of hydrogen-methane plasmas for CVD diamond deposition

Jul 5, 2018, 2:00 PM
2h
Mánes

Mánes

Speaker

Khaled Hassouni

Description

See the full Abstract at http://ocs.ciemat.es/EPS2018ABS/pdf/P4.3002.pdf Self-consistent simulation of hydrogen-methane plasmas for CVD diamond deposition S. Prasanna1 , A. Michau1 , C. Rond1 , K. Hassouni1 , A. Gicquel1 1 Laboratoire des Sciences des Procédés et des Matériaux, UPR3407, CNRS, Universite Paris 13, avenue Jean-Baptiste Clément, 93430 Villetaneuse (France) MW assisted hydrogen methane plasmas have been extensively used for growth of CVD dia- 3000 mond and graphene. In this article, we discuss the T (K) 2000 results of self-consistent simulation of hydrogen- CH4 0.5% 1000 CH4 4% Hyd methane plasmas in a microwave resonating cav- 0 0.02 0.04 0.06 0.08 0.1 0.12 0.14 ity at high pressure conditions (110-200mbar) and z (m) 0.5 different concentrations of methane. Details of the 0.4 self-consistent model is provided elsewhere [1]. XH 0.3 0.2 The results indicate that the pressure, power and 0.1 concentration of methanne in the H2 −CH4 methane 0 0 0.02 0.04 0.06 0.08 0.1 0.12 0.14 z (m) affect the characteristics of the coupling between MW and plasma. Figure 1 shows the gas temper- Figure 1: Effect of methane on the tem- ature and atomic hydrogen concentration at a pres- prature and atomic hydrogen mole frac- sure of 200 mbar and power 2500 W. The results tion at 200 mbar and 2500 W at the axis are in agreement with experimental observations. It of the plasma reactor is seen that the addition of methane increases the temperature of the reactor. As a result the the dissociation of hygrogen increases with addi- tion of methane. The results are similar at 110 mbar. n general, the plasma characteristics is a function of methane concentration, pressure and MW power. References [1] S. Prasanna et al. Plasma Sources Science and Technology 26.9 (2017)

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