2018
DOI: 10.1063/1.5017467
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Particle-in-cell simulations of anomalous transport in a Penning discharge

Abstract: Electrostatic particle-in-cell simulations of a Penning discharge are performed in order to investigate azimuthally asymmetric, spoke-like structures previously observed in experiments. Two-dimensional simulations show that for Penning-discharge conditions, a persistent nonlinear spoke-like structure forms readily and rotates in the direction of ExB and electron diamagnetic drifts. The azimuthal velocity is within about a factor of two of the ion acoustic speed. The spoke frequency follows the experimentally o… Show more

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Cited by 33 publications
(25 citation statements)
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“…The cross field anomalous E ×B electron transport due to the large-scale spoke perturbations was measured insitu and, for the dielectric, seen to account for a 40−100% of the total discharge current, resulting in a β D eff ≈ 10 consistent with computational work 33,36 . Transport becomes more spread and closer to levels of classical collisional transport with the metal as boundary (β M eff ≈ 10β D eff ).…”
Section: Discussionsupporting
confidence: 63%
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“…The cross field anomalous E ×B electron transport due to the large-scale spoke perturbations was measured insitu and, for the dielectric, seen to account for a 40−100% of the total discharge current, resulting in a β D eff ≈ 10 consistent with computational work 33,36 . Transport becomes more spread and closer to levels of classical collisional transport with the metal as boundary (β M eff ≈ 10β D eff ).…”
Section: Discussionsupporting
confidence: 63%
“…This non-dimensional parameter is approximatedly β D eff ≈ 8(6) for B = 30 G in Case I at the edge r = 8 cm, consistent with values presented in some numerical PIC simulations of Penning discharges. 33,36 When the metallic flange is placed, the total cross field transport in the plasma drops very significantly (see Fig. FIG.…”
Section: Changes In Anomalous E × B Electron Cross-field Currentmentioning
confidence: 99%
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“…Instabilities in a large range of frequency and wavelength, from large scale "rotating spokes" to submillimeter structures have been reported experimentally or by simulations in the partially magnetized plasmas of Hall thrusters 7,8,[11][12][13][14][15][16][17][18][19][20][21][22][23][24] , magnetrons 8,[25][26][27][28][29] , ion sources for neutral beam injection 30 , cylindrical magnetized plasma column [31][32][33][34][35][36] and Penning ion sources [37][38][39] . These instabilities are very dependent on the specific conditions or regions of a particular device.…”
Section: Introductionmentioning
confidence: 99%
“…Fluctuating azimuthal electric fields can induce a radial E × B drift-diffusion of the electrons, which is called anomalous diffusion, and reduces the electron storage time in the trap [12][13][14][15]. There are various plasma instabilities; one example, which could be interesting for our Penning trap, is the cross-field (E × B) instability which requires a radial plasma density gradient and an inwardly directed radial electric field in the trap [16,17]. (c) The ions, created along with the secondary electrons, are not trapped inside the inter-spectrometer Penning trap and can leave toward the spectrometers.…”
Section: Inter-spectrometer Penning Trap Problem and Countermeasuresmentioning
confidence: 99%