2008
DOI: 10.1134/s0016793208060042
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Solar proton increases and dynamics of the electron outer radiation belt during solar events in December 2006

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Cited by 5 publications
(3 citation statements)
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“…Mechanisms that are thought to act on the outer proton radiation belt include radial diffusion caused by magnetic and electric perturbations [e.g., Nakada et al , ; Cornwall , ; Beutier et al , ; Boscher et al , ; Vacaresse et al , ; Panasyuk , ] including substorm perturbations [ Spjeldvik , ; Smolin , ], pitch angle scattering by magnetic field curvature effects in the stretched nightside magnetic field [ Tsyganenko , ; Sergeev et al , ], pitch angle scattering and energy diffusion by plasmaspheric whistler mode hiss [ Kozyra et al , ; Villalon and Burke , ] and by ion cyclotron waves [ Søraas et al , ; Shoji and Omura , ], and charge exchange and Coulomb scattering [ Liemohn , ; Beutier et al , ; Walt et al , ]. Potential sources for the outer proton radiation belt include solar protons [ Lazutin et al , ; Panasyuk , ; Tverskaya et al , ] and substorm particle injections [ Vacaresse et al , ]. Finite gyroradius effects can be important for the proton radiation belt, whereas in the nominal dipole field strength of 106 nT at geosynchronous orbit (6.6 R E ) a 1 MeV ( γ = 1.001) proton has a gyroradius r g of 1370 km, whereas a 1 MeV ( γ = 2.96) electron has a gyroradius of 45 km (using the formula r g = [(2Em) 1/2 c/eB][1 + (E/2mc 2 )] 1/2 with kinetic energy E.…”
Section: Introductionmentioning
confidence: 99%
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“…Mechanisms that are thought to act on the outer proton radiation belt include radial diffusion caused by magnetic and electric perturbations [e.g., Nakada et al , ; Cornwall , ; Beutier et al , ; Boscher et al , ; Vacaresse et al , ; Panasyuk , ] including substorm perturbations [ Spjeldvik , ; Smolin , ], pitch angle scattering by magnetic field curvature effects in the stretched nightside magnetic field [ Tsyganenko , ; Sergeev et al , ], pitch angle scattering and energy diffusion by plasmaspheric whistler mode hiss [ Kozyra et al , ; Villalon and Burke , ] and by ion cyclotron waves [ Søraas et al , ; Shoji and Omura , ], and charge exchange and Coulomb scattering [ Liemohn , ; Beutier et al , ; Walt et al , ]. Potential sources for the outer proton radiation belt include solar protons [ Lazutin et al , ; Panasyuk , ; Tverskaya et al , ] and substorm particle injections [ Vacaresse et al , ]. Finite gyroradius effects can be important for the proton radiation belt, whereas in the nominal dipole field strength of 106 nT at geosynchronous orbit (6.6 R E ) a 1 MeV ( γ = 1.001) proton has a gyroradius r g of 1370 km, whereas a 1 MeV ( γ = 2.96) electron has a gyroradius of 45 km (using the formula r g = [(2Em) 1/2 c/eB][1 + (E/2mc 2 )] 1/2 with kinetic energy E.…”
Section: Introductionmentioning
confidence: 99%
“…Although the outer proton radiation belt has been observed by spacecraft instrumentation for five decades [e.g., Davis and Williamson , , ; Yershkovitch et al , ; Stevens et al , ; Spjeldvik , ; Fritz and Spjeldvik , ; Sheldon , ; Green et al , ; Lazutin et al , , ; Tverskaya et al , ; Forster et al , ], much less is known about its properties and dynamics than is known about the outer electron radiation belt. Modeling efforts for the outer proton radiation belt in those five decades [e.g., Nakada and Mead , ; Spjeldvik , ; Beutier et al , ; Bourdarie et al , ; Boscher et al , ; Vacaresse et al , ; Panasyuk , ; Smolin , , ] have been much less sophisticated than the modeling efforts for the outer electron radiation belt.…”
Section: Introductionmentioning
confidence: 99%
“…Within a few hours the European Giove, a research spacecraft in medium Earth orbit began reporting spacecraft charging effects that continued into January 2007 (Fig. 12, Cannon, 2013) as Earth's radiation belts were energized and remained so for weeks (Tverskaya et al, 2008).…”
Section: December 2006 Storm Event Timelinementioning
confidence: 99%