1999
DOI: 10.1109/27.799810
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Semianalytical description of nonlocal secondary electrons in a radio frequency capacitively coupled plasma at intermediate pressures

Abstract: Abstract-Index Terms-Nonlocal ionization by secondary electrons, radio frequency capacitively coupled discharge.

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Cited by 10 publications
(10 citation statements)
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References 12 publications
(32 reference statements)
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“…Therefore, the presence of high‐energy electrons in the centre of the discharge of a high‐pressure RF microdischarge is related to the sheath width. This contrasts with the typical situation encountered in low‐pressure discharges where the presence of high‐energy electrons in the centre of the discharge is related to the non‐locality of high energy electrons 181…”
Section: Diagnostics and Simulations Of Microplasmasmentioning
confidence: 58%
“…Therefore, the presence of high‐energy electrons in the centre of the discharge of a high‐pressure RF microdischarge is related to the sheath width. This contrasts with the typical situation encountered in low‐pressure discharges where the presence of high‐energy electrons in the centre of the discharge is related to the non‐locality of high energy electrons 181…”
Section: Diagnostics and Simulations Of Microplasmasmentioning
confidence: 58%
“…For the smallest microplasmas discussed in this Letter, however, the mode could not be sustained and high-energy electrons can be considered to be in local equilibrium ( " 7 m L). It is also noted that contrary to what happens in low-pressure discharges [21,22], the ion flux to the electrodes (Fig. 4) and the ion density profile (not shown) are strongly time modulated both in the 100 and 75 m plasmas.…”
mentioning
confidence: 70%
“…In conventional low-pressure rf discharges, both the and modes are observed and an increase in the bulk plasma density accompanies the transition from the to the mode. This increase is due to the nonlocal spreading of the ionization caused by electrons [8,21]. For the smallest microplasmas discussed in this Letter, however, the mode could not be sustained and high-energy electrons can be considered to be in local equilibrium ( " 7 m L).…”
mentioning
confidence: 89%
“…The "nonlocal" approach is the opposite case to the "local" description of a plasma, where f 0 (r, v) can be assumed to be a function of only the kinetic energy and the local rf electric field f 0 [mv 2 /2, E(r)] whereas gradients of the local rf electric field and the influence of the ambipolar electric field are neglected. The nonlocal approach has been successfully applied to the self-consistent kinetic modelling of various low-pressure discharges: the capacitively coupled plasmas [28][29][30][31], the inductively coupled plasmas [32][33][34][35], the dc discharges [36,37], the afterglow [38], and the surface-wave discharges [39]. Additional references can be found in reviews [40][41][42].…”
Section: Self-consistent System Of Equations For a Kinetic Descrimentioning
confidence: 99%