2020
DOI: 10.1063/1.5132596
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Kinetic sheath in presence of multiple positive ions, negative ions, and particle wall emission

Abstract: The region between a Maxwellian plasma source and a floating or current-carrying surface is described by a static, one-dimensional collisionless kinetic sheath model. In the plasma source, electrons, negative ions and several positive ion species with different temperatures can be included. The surface (wall) can emit electrons and/or negative ions. When the flux of surface-emitted negative ions and/or electrons reaches a critical value, the sheath becomes spacecharge saturated which leads to the formation of … Show more

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Cited by 7 publications
(7 citation statements)
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References 56 publications
(90 reference statements)
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“…For Φ well ∼ −1.3 V, the saturation current is on the order of 6.8 A.m −2 , close to the calculated value (6 A.m −2 ). The threshold for the appearance of the saturated regime has been recently derived analytically and extended to the case of multiple charge species in the work of Schiesko et al 143 . By applying −5 V at the LB plane, negative ions move back and forth trapped by the electric potential before being destroyed by detachment processes or extracted.…”
Section: Extraction Of Negative Ionsmentioning
confidence: 99%
“…For Φ well ∼ −1.3 V, the saturation current is on the order of 6.8 A.m −2 , close to the calculated value (6 A.m −2 ). The threshold for the appearance of the saturated regime has been recently derived analytically and extended to the case of multiple charge species in the work of Schiesko et al 143 . By applying −5 V at the LB plane, negative ions move back and forth trapped by the electric potential before being destroyed by detachment processes or extracted.…”
Section: Extraction Of Negative Ionsmentioning
confidence: 99%
“…The intricacies of sheaths have made them one of the most researched topics in plasma physics. Although they have been studied and understood by both fluid [1][2][3][4][5][6][7] and kinetic approaches [8][9][10][11][12], there is enough scope to investigate the problem further. In the case of the fluid approach, usually, the ions are governed by the hydrodynamic equations and the distribution of electrons are defined by Maxwell-Boltzmann statistics.…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, the Boltzmann behaviour restricts the electron distribution to the macroscopic ergodic equilibrium state and is often found to be inadequate to describe long-range interactions [20]. Also, the plasma sheath is regarded as a transition region between the plasma and the wall and is considered a non-neutral region besides possessing a non-Maxwellian nature [12,21]. Due to such characteristics, the sheath plays a substantial role in influencing the particle and energy transport towards the wall.…”
Section: Introductionmentioning
confidence: 99%
“…Although the magnetic filter field is helpful for increasing the extraction probability of negative ions [14] and decreasing the electron temperature, the negative ion density is almost unchanged because of the decreased electron density [15]. Furthermore, a higher value of plasma density near the plasma grid is helpful for the surface production [15][16][17]. Hence, it is of significant importance to control the magnetic field topology to increase the plasma density.…”
Section: Introductionmentioning
confidence: 99%