Plasma sheath around sunlit moon: monotonic & non-monotonic structures

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dc.contributor.author Sana, Trinesh
dc.contributor.author Mishra, S. K.
dc.coverage.spatial United Kingdom
dc.date.accessioned 2023-01-25T13:27:17Z
dc.date.available 2023-01-25T13:27:17Z
dc.date.issued 2023-03
dc.identifier.citation Sana, Trinesh and Mishra, S. K., “Plasma sheath around sunlit moon: monotonic & non-monotonic structures”, Monthly Notices of the Royal Astronomical Society, DOI: 10.1093/mnras/stad155, vol. 520, no. 1, pp. 233-246, Mar. 2023. en_US
dc.identifier.issn 0035-8711
dc.identifier.issn 1365-2966
dc.identifier.uri https://doi.org/10.1093/mnras/stad155
dc.identifier.uri https://repository.iitgn.ac.in/handle/123456789/8521
dc.description.abstract An analytical investigation of the sheath formation over sunlit Moon under the influence of observed solar ultraviolet/ extreme ultraviolet radiation and solar wind plasma has been presented. Poisson's equation is coupled with the latitude-dependent Fermionic photoelectrons, non-Maxwellian solar wind electrons and cold ions to derive the electric potential, electric field, and population density profiles within the photoelectron sheath. We notice that the high energy photons of the solar spectra in addition to Lyman- α, significantly contribute in determining the surface charge and subsequent sheath structure. A traditional Debye (Type C) sheath forms around the terminator due to dominant plasma electron accretion and marginal photoemission. While moving towards the equator, the photoelectron contribution increases, yielding monotonic (Type B) and non-monotonic (Type A) sheath solutions over sunlit locations. The calculations show that the non-monotonic potential structures are more stable near the terminator region, while both types of potential structures are probable near the equator region for the nominal solar wind plasma. A vertical sheath extension of ∼60 m and ∼12 m is predicted for typical solar wind plasma at the equator corresponding to Type A and Type B sheath, respectively. Under exotic plasma conditions (e.g. Earth's magnetospheric tail lobe, plasma sheet), non-monotonic solutions become stable for the photoemission-dominated region, and the entire sunlit lunar surface may acquire negative potential.
dc.description.statementofresponsibility by Trinesh Sana and S. K. Mishra
dc.format.extent vol. 520, no. 1, pp. 233-246
dc.language.iso en_US en_US
dc.publisher Oxford University Press en_US
dc.subject Plasma sheath en_US
dc.subject Poisson's equation en_US
dc.subject Fermionic photoelectrons en_US
dc.subject Photoemission en_US
dc.subject Solar wind plasma en_US
dc.title Plasma sheath around sunlit moon: monotonic & non-monotonic structures en_US
dc.type Journal Paper en_US
dc.relation.journal Monthly Notices of the Royal Astronomical Society


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