2014
DOI: 10.1088/0963-0252/23/6/065037
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SF6and C4F8global kinetic models coupled to sheath models

Abstract: Global kinetic models combined with Monte Carlo sheath models are developed for SF 6 and C 4 F 8 plasma discharges for silicon etching under the Bosch process. In SF 6 plasma, the dominant positive ions are SF + 5 , SF + 4 , SF + 3 and F + while in C 4 F 8 the dominant positive ions are CF + 3 and C 2 F + 3 . The simulation results show that the electrical parameters, such as the electron density and electron temperature, clearly affect the sheath dynamics and consequently the ion energy distribution function … Show more

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Cited by 16 publications
(13 citation statements)
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“…The simulation approach developed in this study is an updated version of an approach presented in a previous work [27]. In the present version, we show strong variations of electrical parameters under some specific operating conditions for C 4 F 8 plasmas.…”
Section: Introductionmentioning
confidence: 81%
See 1 more Smart Citation
“…The simulation approach developed in this study is an updated version of an approach presented in a previous work [27]. In the present version, we show strong variations of electrical parameters under some specific operating conditions for C 4 F 8 plasmas.…”
Section: Introductionmentioning
confidence: 81%
“…Details of the plasma kinetic model of C 4 F 8 have been presented in previous publications [27,32,33]. The plasma model is based on the 0D global model.…”
Section: Modelmentioning
confidence: 99%
“…Note there is discrepancy in literature concerning the variation of the fluorine atom density which must be discussed. Yang pressure, in which the variation is thought to be related to the dissociation of SF 6 [42]. The major difference between the different simulation studies is mainly due to the electronic density which can strongly increase with the decreasing pressure, or at the opposite, exhibits a low variation.…”
Section: A Micromasking Effectmentioning
confidence: 99%
“…where z is the axial coordinate (z = 0 at the sheath entrance), n is constant between 0.5 and 1. In our simulations, n is estimated to 0.75. l s is the sheath thickness that depends on T e and n e ; it is evaluated from the plasma model [75]. The potential drop acros the sheath (V CS ) depends on the DC bias [75].…”
Section: Sheath Modelmentioning
confidence: 99%