2018
DOI: 10.3847/1538-4357/aadbac
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Globally Distributed Energetic Neutral Atom Maps for the “Croissant” Heliosphere

Abstract: A recent study by Opher et al. (2015) suggested the heliosphere has a "croissant" shape, where the heliosheath plasma is confined by the toroidal solar magnetic field. The "croissant" heliosphere is in contrast to the classically accepted view of a comet-like tail. We investigate the effect of the "croissant" heliosphere model on energetic neutral atom (ENA) maps. Regardless of the existence of a split tail, the confinement of the heliosheath plasma should appear in ENA maps. ENA maps from the Interstellar Bou… Show more

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Cited by 19 publications
(30 citation statements)
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References 53 publications
(106 reference statements)
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“…We also note, that in the case of 𝛼 = 𝛽, the bi-Maxwellian boundary condition (11) transforms into a single Maxwellian distribution function with number density 𝑛 pui and temperature 𝑇 pui . Even though the assumption of thermal equilibrium of the populations is not justified, the attempts to model the pickup ion velocity distribution using the superposition of Maxwell distributions are made by some authors (see, e.g., Zank et al 2010;Zirnstein et al 2017;Kornbleuth et al 2018).…”
Section: «Bi-maxwellian» Scenariomentioning
confidence: 99%
See 1 more Smart Citation
“…We also note, that in the case of 𝛼 = 𝛽, the bi-Maxwellian boundary condition (11) transforms into a single Maxwellian distribution function with number density 𝑛 pui and temperature 𝑇 pui . Even though the assumption of thermal equilibrium of the populations is not justified, the attempts to model the pickup ion velocity distribution using the superposition of Maxwell distributions are made by some authors (see, e.g., Zank et al 2010;Zirnstein et al 2017;Kornbleuth et al 2018).…”
Section: «Bi-maxwellian» Scenariomentioning
confidence: 99%
“…Additionally, we note that the partition of PUIs into two Maxwellian populations is performed only immediately after (downstream) the TS, and in the IHS, the solution (1) of the kinetic equation is used. This method compares favorably with other existing approaches since it does not imply the assumption of fixed temperature fraction in the whole inner heliosheath (like it was done in Zirnstein et al 2017;Kornbleuth et al 2018), which is not justified. As can be seen from Figure 1, the power-law «tail» in the PUI distribution forms the proper slope of the spectrum and makes the fluxes higher at energies 2 keV.…”
Section: «Bi-maxwellian» Scenariomentioning
confidence: 99%
“…The ENA Flux model is the same as used in Kornbleuth et al (2020), which is an update to the model used in Kornbleuth et al (2018). We interpolate our Cartesian grid to a spherical grid of 2 AU × 6 • × 6 • .…”
Section: Ena Modelmentioning
confidence: 99%
“…Measured ENA intensities represent the line-of-sight integral of local proton intensities times the neutral H density, which means modeling is required to interpret the observations. To model ENAs in the heliosphere, global heliospheric solutions can be used to simulate ENA fluxes directly (Heerikhuisen et al 2008) or can be used in post-processing to simulate ENA fluxes from the plasma and neutral distributions (Prested et al 2008;Zirnstein et al 2013;Kornbleuth et al 2018;Baliukin et al 2020).…”
Section: Introductionmentioning
confidence: 99%
“…Zirnstein et al (2016Zirnstein et al ( , 2017, using a time dependent simulation with solar cycle variations of the solar wind, reproduced the spectral dependence and heliotail ENA maps as shown by IBEX with a model of the heliotail resembling a long comet-like tail. Kornbleuth et al (2018) investigated the ENA maps from the "croissant" heliosphere (Opher et al 2015) with a uniform solar wind. The collimation of the heliosheath plasma by the solar magnetic field created high latitude lobes despite the lack of fast solar wind at the poles.…”
Section: Introductionmentioning
confidence: 99%