2015
DOI: 10.1002/2015ja021539
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Interstellar hydrogen ionization in the heliosheath

Abstract: The expanding solar wind plasma undergoes a shock transition at the interstellar boundary of the solar system and fills the inner heliosheath, the region between the termination shock and the heliopause. The nonequilibrium heliosheath plasma is a main source of energetic neutral atoms that allow remote probing of the heliospheric interface region. Global models of the heliosphere interaction with the interstellar medium often disregard solar photoionization and electron impact ionization of interstellar gas in… Show more

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Cited by 9 publications
(4 citation statements)
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“…Observations of the F-corona continuum in the near-infrared show a sharp drop off in brightness that scale between r −1.9 to r −2.5 for the equatorial and r −2.3 to r −2.8 for the polar solar regions below 10R which correspond to freeze-in distances in our simulations (Koutchmy & Lamy 1985;MacQueen & Greeley 1995;Leinert & Jackson 1998). In Gruntman (1994Gruntman ( , 1996, both n H and n H2 were estimated as ∝ r −1.15 below 1AU. However neutrals in the heliosphere are highly uncertain and remain relatively unknown in the vicinity of the Sun.…”
Section: Modeling Of Solar He + Ionssupporting
confidence: 50%
“…Observations of the F-corona continuum in the near-infrared show a sharp drop off in brightness that scale between r −1.9 to r −2.5 for the equatorial and r −2.3 to r −2.8 for the polar solar regions below 10R which correspond to freeze-in distances in our simulations (Koutchmy & Lamy 1985;MacQueen & Greeley 1995;Leinert & Jackson 1998). In Gruntman (1994Gruntman ( , 1996, both n H and n H2 were estimated as ∝ r −1.15 below 1AU. However neutrals in the heliosphere are highly uncertain and remain relatively unknown in the vicinity of the Sun.…”
Section: Modeling Of Solar He + Ionssupporting
confidence: 50%
“…In most self-consistent models of heliospheric dynamics, so far, only the influence of neutral hydrogen is considered by taking into account its charge exchange with solar wind protons and its ionization by the solar radiation (e.g., [153,91,154] and references therein). The dynamical relevance of both the electron impact ionization of hydrogen, although recognized by [155], [36] as well as [156], and the photo-ionization of helium, although recognized as being filtered in the inner heliosheath [157,158], have not yet been explored in detail. There is only one attempt to include helium self-consistently in the heliospheric modeling [36], in which the emphasis is on the additional ram pressure due to the charged helium ions.…”
Section: The Effect Of Helium Charge Exchangementioning
confidence: 99%
“…The second term in Equation (1) describes the advection with the solar wind with velocity u , p the third term describes diffusion of particles in velocity space, the fourth term describes adiabatic heating/cooling, and the last term describes a source (or sink) for the distribution due to, for example, charge-exchange with interstellar neutral atoms. Other ionization processes are ignored, such as photoionization (which is negligible at large distances from the Sun) and electron-impact ionization (the distribution of electrons in the IHS is not known, even though it has had recent attention, see e.g., Chalov & Fahr 2013;Chashei & Fahr 2013;Scherer et al 2014;Fahr et al 2015;Gruntman 2015).…”
Section: Pui Transportmentioning
confidence: 99%