Plasma currents and electron distribution functions under a dc electric field of arbitrary strength

The currents induced by arbitrarily strong dc electric fields in plasma and the evolution of electron distributions have been studied by Fokker-Planck simulations. We find that the electron distributions evolve distinctly under different fields; especially, the electron distribution is well represen...

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Main Authors: Weng, S, Sheng, Z, He, M, Zhang, J, Norreys, P, Sherlock, M, Robinson, A
Format: Journal article
Language:English
Published: 2008
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author Weng, S
Sheng, Z
He, M
Zhang, J
Norreys, P
Sherlock, M
Robinson, A
author_facet Weng, S
Sheng, Z
He, M
Zhang, J
Norreys, P
Sherlock, M
Robinson, A
author_sort Weng, S
collection OXFORD
description The currents induced by arbitrarily strong dc electric fields in plasma and the evolution of electron distributions have been studied by Fokker-Planck simulations. We find that the electron distributions evolve distinctly under different fields; especially, the electron distribution is well represented by the sum of a stationary and drifting Maxwellian at the moderate field. A set of hydrodynamiclike equations, similar to Spitzer's but without the weak-field limit, is given for calculating the current. It is more suitable for application in hybrid particle-in-cell simulations and may extend plasma transport theory in models that do not employ a kinetic description of the electrons. © 2008 The American Physical Society.
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spelling oxford-uuid:25e08c30-b436-4ee6-9b01-8e061d218efd2022-03-26T11:57:58ZPlasma currents and electron distribution functions under a dc electric field of arbitrary strengthJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:25e08c30-b436-4ee6-9b01-8e061d218efdEnglishSymplectic Elements at Oxford2008Weng, SSheng, ZHe, MZhang, JNorreys, PSherlock, MRobinson, AThe currents induced by arbitrarily strong dc electric fields in plasma and the evolution of electron distributions have been studied by Fokker-Planck simulations. We find that the electron distributions evolve distinctly under different fields; especially, the electron distribution is well represented by the sum of a stationary and drifting Maxwellian at the moderate field. A set of hydrodynamiclike equations, similar to Spitzer's but without the weak-field limit, is given for calculating the current. It is more suitable for application in hybrid particle-in-cell simulations and may extend plasma transport theory in models that do not employ a kinetic description of the electrons. © 2008 The American Physical Society.
spellingShingle Weng, S
Sheng, Z
He, M
Zhang, J
Norreys, P
Sherlock, M
Robinson, A
Plasma currents and electron distribution functions under a dc electric field of arbitrary strength
title Plasma currents and electron distribution functions under a dc electric field of arbitrary strength
title_full Plasma currents and electron distribution functions under a dc electric field of arbitrary strength
title_fullStr Plasma currents and electron distribution functions under a dc electric field of arbitrary strength
title_full_unstemmed Plasma currents and electron distribution functions under a dc electric field of arbitrary strength
title_short Plasma currents and electron distribution functions under a dc electric field of arbitrary strength
title_sort plasma currents and electron distribution functions under a dc electric field of arbitrary strength
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