Helicon mode driven by O+ thermal anisotropy

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dc.contributor.author Mace, R.L.
dc.contributor.author Lakhina, G.S.
dc.date.accessioned 2015-09-28T10:56:49Z
dc.date.accessioned 2021-02-12T09:30:57Z
dc.date.available 2015-09-28T10:56:49Z
dc.date.available 2021-02-12T09:30:57Z
dc.date.issued 2000
dc.identifier.citation Waves in Dusty, Solar and Space Plasmas, edited by F.Verheest et al, CP537, AIP, 2000 en_US
dc.identifier.uri http://localhost:8080/xmlui/handle/123456789/499
dc.description.abstract Preliminary results from an investigation of the helicon instability in a plasma composed of protons, electrons and singly charged oxygen ions, are presented. The velocity distribution function for each plasma component is modeled by a bi-Lorentzian distribution, which allows each particle species to possess a power law tail of arbitrary spectral index. This permits us to model accurately the shape of the power law tails observed on particle species in the plasma sheet region, where the helicon mode is believed to play an important role. The presence of a hard power law tail on the oxygen component is found to dramatically enhance the maximum growth rate of the instability when the oxygen ions possess a small T∥>T⊥ anisotropy. Above a certain value of T∥/T⊥, however, this behavior is reversed. The growth rate decreases as the spectral index of the protons is decreased. The relevance of these effects to the central plasma sheet region is briefly discussed. en_US
dc.language.iso en en_US
dc.subject Helicon modes en_US
dc.subject Oxygen ions en_US
dc.subject Plasma sheet en_US
dc.subject Thermal anisotropy en_US
dc.title Helicon mode driven by O+ thermal anisotropy en_US
dc.type Article en_US
dc.identifier.accession 091010


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