2020
DOI: 10.1021/acs.jpca.0c03396
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Optical Emission Imaging and Modeling Investigations of Microwave-Activated SiH4/H2 and SiH4/CH4/H2 Plasmas

Abstract: Silicon is a known trace contaminant in diamond grown by chemical vapor deposition (CVD) methods.Deliberately Si-doped diamond is currently attracting great interest because of the attractive optical properties of the negatively charged silicon-vacancy (SiV − ) defect. This work reports in-depth studies of microwave activated H2 plasmas containing trace (10-100 ppm) amounts of SiH4, with and without a few % of CH4, operating at pressures and powers relevant for contemporary diamond CVD, using a combination of … Show more

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Cited by 10 publications
(17 citation statements)
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References 97 publications
(307 reference statements)
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“…At yet higher CH4 additions (X0(CH4) >2%), ion production by EII of neutral CxHy species (mainly C2H2) is predicted to start exceeding the sum of that from EII of H and H2, resulting in a slow and progressive decline in Te. Such trends upon CH4 addition were also noted and discussed in [41].…”
Section: Response Of Plasma Parameters Upon Adding N2 To Ch4/h2 Mixturessupporting
confidence: 54%
“…At yet higher CH4 additions (X0(CH4) >2%), ion production by EII of neutral CxHy species (mainly C2H2) is predicted to start exceeding the sum of that from EII of H and H2, resulting in a slow and progressive decline in Te. Such trends upon CH4 addition were also noted and discussed in [41].…”
Section: Response Of Plasma Parameters Upon Adding N2 To Ch4/h2 Mixturessupporting
confidence: 54%
“…The H-atom number density in the plasma core is predicted to barely change. Such minor variations in these key parameters can be understood by recognizing the X 0 (CH 4 )-dependent balances between the ionization (i.e., associative ionization (AI) reactions between H­( n ≥ 2) atoms and H 2 and electron impact ionization (EII) of C 2 H 2 , H 2 , and H) and electron–ion recombination processes (whereby H 3 + ions interchange with C x H y + ions), as recently discussed in detail for the more complex case of dilute MW activated Si/C/H plasmas . The predicted insensitivity of these key plasma parameters to changes in X 0 (CH 4 ) is reflected in the near constancy of the (predicted) {C 2 (C)}/{C 2 (d)} and (observed) R (C/d) versus z plots shown in Figure (b).…”
Section: Resultsmentioning
confidence: 97%
“…Such minor variations in these key parameters can be understood by recognizing the X 0 (CH 4 )- + ions), as recently discussed in detail for the more complex case of dilute MW activated Si/C/H plasmas. 21 The predicted insensitivity of these key plasma parameters to changes in X 0 (CH 4 ) is reflected in the near constancy of the (predicted) {C 3.4. Higher Pressure Effects and Plasma Shrinkage.…”
Section: The Journal Ofmentioning
confidence: 97%
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“…After the cleaning process, the residual level of silicon in the reactor was estimated from the ratio of the emission intensities of the silicon line at a wavelength of 288.16 nm to the dissociative continuum for a discharge in pure hydrogen. It is known that the addition of methane to a hydrogen plasma with a low content of silane leads to a significant decrease of the emission intensity of silicon lines in the plasma; [ 8,24 ] therefore, the residual level was estimated in pure hydrogen. To calibrate the residual level, a small flow of silane was added to the hydrogen plasma.…”
Section: Methodsmentioning
confidence: 99%