Signatures of the interplanetary helium cone reflected by pick-up ions

Citation
Sv. Chalov et Hj. Fahr, Signatures of the interplanetary helium cone reflected by pick-up ions, SOLAR PHYS, 187(1), 1999, pp. 123-144
Citations number
47
Categorie Soggetti
Space Sciences
Journal title
SOLAR PHYSICS
ISSN journal
00380938 → ACNP
Volume
187
Issue
1
Year of publication
1999
Pages
123 - 144
Database
ISI
SICI code
0038-0938(199906)187:1<123:SOTIHC>2.0.ZU;2-X
Abstract
As known for a long time, interstellar wind neutral helium atoms deeply pen etrate into the inner heliosphere and, when passing through the solar gravi ty field, form a strongly pronounced helium density cone in the downwind di rection. Helium atoms are photoionized and picked-up by the solar wind magn etic field, but as pick-up ions they are not simply convected outwards with the solar wind in radial directions as assumed in earlier publications. Ra ther they undergo a complicated diffusion-convection process described here by an appropriate kinetic transport equation taking into account adiabatic cooling and focusing, pitch angle scattering and energy diffusion. In this paper, we solve this equation for He+ pick-up ions which are injected into the solar wind mainly in the region of the helium cone. We show the result ing He+ pick-up ion density profile along the orbit of the Earth in many re spects differs from the density profile of the neutral helium cone: dependi ng on solar-wind-entrained Alfvenic turbulence levels, the density maximum when looking from the Earth to the Sun is shifted towards the right side of the cone, the ratio of peak-densities to wing-densities varies and a left- to-right asymmetry of the He+-density profile is pronounced. Derivation of interstellar helium parameters from these He+-structures, such as the local interstellar medium (LISM) wind direction, LISM velocity and LISM temperat ure, are very much impeded. In addition, the pitch-angle spectrum of He+ pi ck-up ions systematically becomes more anisotropic when passing from the le ft to the right wing of the cone structure. All effects mentioned are more strongly pronounced in high velocity solar wind compared to the low velocit y solar wind.