2013
DOI: 10.1063/1.4826949
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Transition of electron kinetics in weakly magnetized inductively coupled plasmas

Abstract: Transition of the electron kinetics from nonlocal to local regime was studied in weakly magnetized solenoidal inductively coupled plasma from the measurement of the electron energy probability function (EEPF). Without DC magnetic field, the discharge property was governed by nonlocal electron kinetics at low gas pressure. The electron temperatures were almost same in radial position, and the EEPFs in total electron energy scale were radially coincided. However, when the DC magnetic field was applied, radial no… Show more

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Cited by 10 publications
(6 citation statements)
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References 37 publications
(39 reference statements)
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“…The primary aim of this work was to show that for conditions where a magnetized plasma is in free expansion, i.e., the mean free path for electron neutral collisions is greater than the scale length of the plasma system, the eepf can be described by nonlocal parameters [12][13][14]. A rf compensated Langmuir probe was used to measure the eepfs which were then normalized by a small factor so that they coincided at one bias voltage (−30 V).…”
Section: Resultsmentioning
confidence: 99%
“…The primary aim of this work was to show that for conditions where a magnetized plasma is in free expansion, i.e., the mean free path for electron neutral collisions is greater than the scale length of the plasma system, the eepf can be described by nonlocal parameters [12][13][14]. A rf compensated Langmuir probe was used to measure the eepfs which were then normalized by a small factor so that they coincided at one bias voltage (−30 V).…”
Section: Resultsmentioning
confidence: 99%
“…The characteristic of skin depth transit from normal to that of magnetized and vice versa within RF cycle with double frequency. This phenomena lead to transition of electron energy distribution function (EEDF) from non-local to local nature [33]. (e) In the transformer model, physics of power transfer is not modelled adequately.…”
Section: Resultsmentioning
confidence: 99%
“…2. 1.340T10 15 2.010T10 15 2.680T10 15 3.350T10 15 4.020T10 15 4.690T10 15 5.360T10 15 0 2.925T10 15 5.850T10 15 8.775T10 15 1.170T10 16 1.463T10 16 1.755T10 16 2.048T10 16 2.340T10 16 0 1.900T10 17 3.800T10 17 5.700T10 17 7.600T10 17 9.500T10 17 1.140T10 18 1.330T10 18 1.520T10 18 0 2.075T10 19 4.150T10 19 6.225T10 19 8.300T10 19 1.038T10 20 1.245T10 20 1.153T10 20 1.660T10 20 Fig. 2.…”
Section: Application and Discussionunclassified
“…For example, the electromagnetic wave effects in a common 13.56 MHz RF-driven capacity coupled plasma can be neglected and the electrostatic solver is enough. [18,19] Theoretically, magnetized capacity coupled plasma (CCP), [1] magnetic-biased inductive coupled plasma (ICP), [20] magnetron, [5] and the pre-ionization of magnetized target fusion (MTF) [21] are of these cases and can be considered as electrostatic plasmas plus driving fields. Besides, we can expect that electrostatic implicit algorithms can give a better simulating speed and convergency in these cases because this algorithm can get rid of instabilities relative to electromagnetic waves.…”
Section: Introductionmentioning
confidence: 99%