1999
DOI: 10.1016/s0584-8547(99)00042-7
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Fundamental comparison between non-equilibrium aspects of ICP and MIP discharges

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Cited by 72 publications
(56 citation statements)
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“…Since n e values are for r = 0, we divided the value by 1.64 assuming a Bessel-like profile. For the value of C, we used R * = 3 mm, λ h = 0.0178 W(mK) −1 [26] and S heat = 6.7×10 −19 m 3 s −1 based on the work of references [27][28][29]. It can be seen that the agreement between theory and experiment is reasonable and falls in between the error bars.…”
Section: Discussionmentioning
confidence: 99%
“…Since n e values are for r = 0, we divided the value by 1.64 assuming a Bessel-like profile. For the value of C, we used R * = 3 mm, λ h = 0.0178 W(mK) −1 [26] and S heat = 6.7×10 −19 m 3 s −1 based on the work of references [27][28][29]. It can be seen that the agreement between theory and experiment is reasonable and falls in between the error bars.…”
Section: Discussionmentioning
confidence: 99%
“…This is the opposite to the top boundary where exp(−iβz) is used instead. As the BC should be applied to the total E r field, we substitute the relation E − r = E r − E + r into equation (20), which, using (19), gives…”
Section: Homogeneous Inhomoneous Dirichletmentioning
confidence: 99%
“…[5] that it works remarkably well for the ICP. However, discrepancies between the dBR-theory and experiments were found for the MIP created by the TIA (Torche injection axiale [6]).…”
Section: Introductionmentioning
confidence: 74%
“…It will be shown that the new detection system reveals more details in the n e -and T e -fields, but also, that despite of the more precise information, the same conflict between the experimental and theoretical results as found for the TIA [5,6] remains. This means that the experimentally found T evalue is substantially larger and the experimental n e -value much smaller than what is found theoretically.…”
Section: Introductionmentioning
confidence: 82%
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