2016
DOI: 10.1016/j.cap.2016.03.011
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Improving discharge uniformity of industrial-scale very high frequency plasma sources by launching a traveling wave

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Cited by 3 publications
(2 citation statements)
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“…At a lower operating gas pressure (50 mTorr), the maximum of the density profile is found in the tile-centre, whereas, tiletile boundary density is lower. The plasma non-uniformity is calculated by ((n max − n min ) / (n max + n min )) × 100, where n max and n min are maximum and minimum electron density respectively [43,44]. It is shown in figure 4, on increasing RF power, the plasma uniformity is significantly improved.…”
Section: Plasma Densitymentioning
confidence: 99%
“…At a lower operating gas pressure (50 mTorr), the maximum of the density profile is found in the tile-centre, whereas, tiletile boundary density is lower. The plasma non-uniformity is calculated by ((n max − n min ) / (n max + n min )) × 100, where n max and n min are maximum and minimum electron density respectively [43,44]. It is shown in figure 4, on increasing RF power, the plasma uniformity is significantly improved.…”
Section: Plasma Densitymentioning
confidence: 99%
“…Both experimental [19][20][21] and numerical [22][23][24] research indicated that by varying the phase difference between the two sources applied to the top and bottom electrodes, i.e., the so-called phase-shift control, the plasma currents redistributed and therefore the plasma uniformity could be optimized. Moreover, Chen et al pointed out that the plasma nonuniformity decreased significantly by launching a traveling wave, which was generated by the superposition of two standing waves with the same amplitude and out of phase by 90 • in space and time [25][26][27]. Bera et al introduced the electric potential and the magnetic vector potential to calculate the ES field and the EM field, respectively, and they presented different electron density distributions with various combinations of powers at 60 MHz and 180 MHz [28].…”
Section: Introductionmentioning
confidence: 99%