Effect of central gas flow rate and water on an argon inductively coupled plasma: spatially resolved emission, ion-atom intensity ratios and electron number densities

1990 ◽  
Vol 45 (7) ◽  
pp. 731-752 ◽  
Author(s):  
John W. Olesik ◽  
Su-Jane Den
1984 ◽  
Vol 38 (5) ◽  
pp. 647-653 ◽  
Author(s):  
G Angleys ◽  
J. M. Mermet

Based on a previously published work, calculations of the minimum plasma gas flow rate for torch tubes of various dimensions have been performed Predicted minimum rates have been verified by experiment It is possible to sustain a discharge at 600 W and 6 L/min without reducing drastically the external size of the torch One of the main parameters in torch design is the various flow velocities The main influence on the plasma gas flow rate is provided by the space between the external and the intermediate tube A practical design is proposed and a comparison is made with the literature


2020 ◽  
Vol 35 (9) ◽  
pp. 2033-2056 ◽  
Author(s):  
Shi Jiao ◽  
John W. Olesik

Comprehensive characterization of ICP-SFMS matrix effects as function of analyte mass, matrix mass, focus lens voltage and nebulizer gas flow rate.


Processes ◽  
2019 ◽  
Vol 7 (3) ◽  
pp. 133 ◽  
Author(s):  
Sangeeta Punjabi ◽  
Dilip Barve ◽  
Narendra Joshi ◽  
Asoka Das ◽  
Dushyant Kothari ◽  
...  

In this article, electrical characteristics of a high-power inductively-coupled plasma (ICP) torch operating at 3 MHz are determined by direct measurement of radio-frequency (RF) current and voltage together with energy balance in the system. The variation of impedance with two parameters, namely the input power and the sheath gas flow rate for a 50 kW ICP is studied. The ICP torch system is operated at near atmospheric pressure with argon as plasma gas. It is observed that the plasma resistance increases with an increase in the RF-power. Further, the torch inductance decreases with an increase in the RF-power. In addition, plasma resistance and torch inductance decrease with an increase in the sheath gas flow rate. The oscillator efficiency of the ICP system ranges from 40% to 80% with the variation of the Direct current (DC) powers. ICP has also been numerically simulated using Computational Fluid Dynamics (CFD) to predict the impedance profile. A good agreement was found between the CFD predictions and the impedance experimental data published in the literature.


1988 ◽  
Vol 117 ◽  
Author(s):  
N. S. Nogar ◽  
G. L. Keaton ◽  
J. E. Anderson ◽  
M. Trkula

AbstractEmission spectroscopy and laser-induced fluorescence have been used to monitor the field and tail-flame regions of a Hull-design 1 inductively coupled plasma. This plasma is used for a variety of syntheses 2,3 including SiC, TiC, BN, AlN and diamond. Temporallyand spatially-resolved spectra of both pure Ar and Ar/gas mixtures have been studied as a function of RF power, pressure and flow rate. Preliminary data suggest that the system is far from local thermodynamic equilibrium.


2007 ◽  
Vol 561-565 ◽  
pp. 1209-1212 ◽  
Author(s):  
Tsutomu Sakata ◽  
Katsunori Makihara ◽  
Hidenori Deki ◽  
Seiichiro Higashi ◽  
Seiichi Miyazaki

We have studied uniform growth of crystalline Ge films on quartz plate from VHF (60MHz)-ICP of 10% GeH4 diluted with H2 in the temperature range from 150 to 350°C. By optimizing total gas flow rate, gas pressure, VHF power and antenna-substrate distance, the growth rate as high as 7.4nm/s was obtained at 150°C and increased gradually up to ~7.9nm/s at 350°C. The crystallinity, which was evaluated by Raman scattering measurements as an integrated intensity ratio of TO phonons in crystalline phase to those in disordered phase, reached a value as high as ~93 % at 350°C, but degraded down to 64% at 150°C as a result of the formation of a 60~70nm-thick amorphous incubation (A. I.) layer on quartz. By applying a two-step deposition method at 150°C, in which the GeH4 concentration was selected to be 0.6% for the crystalline nucleation in the first 10s deposition, being as thin as 10nm in thickness, and then changed to 10% GeH4 for the high rate growth, the crystallinity was improved to 78% with keeping an effective growth rate as high as 7.5nm/s, because of a significant increase in the growth rate after the crystalline nucleation.


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