2020
DOI: 10.3847/2041-8213/abcaaa
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Combined ∼10 eV to ∼344 MeV Particle Spectra and Pressures in the Heliosheath along the Voyager 2 Trajectory

Abstract: We report a unique combination of ∼10 eV to ∼344 MeV in situ ion measurements from the Plasma Science (PLS), Low Energy Charged Particle (LECP), and Cosmic Ray Subsystem (CRS) experiments on the Voyager 2 (V2) spacecraft, and remotely sensed ∼110 eV to ∼55 keV energetic neutral atom (ENA) measurements from the Interstellar Boundary Explorer (IBEX) mission and Ion and Neutral Camera (INCA) on the Cassini mission. This combination is done over the time period from 2009 to the end of 2016, along the V2 trajectory… Show more

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Cited by 34 publications
(61 citation statements)
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“…Beyond 350 AU at low latitudes, the ISM flows between the two lobes in the BU model, which leads to the lower thermal pressure and higher magnetic pressure in the tail. Both models have total pressures which agree with Voyager observations (Rankin et al 2019;Dialynas et al 2020).…”
Section: Interstellar Medium Propertiessupporting
confidence: 81%
“…Beyond 350 AU at low latitudes, the ISM flows between the two lobes in the BU model, which leads to the lower thermal pressure and higher magnetic pressure in the tail. Both models have total pressures which agree with Voyager observations (Rankin et al 2019;Dialynas et al 2020).…”
Section: Interstellar Medium Propertiessupporting
confidence: 81%
“…The findings of [68] are supported by more recent studies, such as [72,73], but also posed a challenging question: given their surprisingly similar time profiles, why was the cosmic ray disturbance isotropic in the heliosheath but highly anisotropic in the VLISM? An interesting solution was put forth by [74], who simulated the perturbation of cosmic-rays by GMIRs in the heliosheath and employed a Vlasov-Fokker-Planck equation to allow for the transport of particles having significant anisotropy.…”
Section: Pos(icrc2021)032supporting
confidence: 67%
“…The resulting spectra from the model are softer (harder) than the observed ones in the 0.52-8 keV energy range (beyond ∼8 keV), i.e., the ratio between the measurements and the model within that energy range is increasing (decreasing). The overall best comparison between the model and the measurements occurs for >18 keV, which is not surprising considering that (i) the PUIs from the hybrid simulation that we use (Giacalone et al 2021) agree well with the ∼28 keV measurements from LECP in V2, and (ii) the conversions of the in situ ∼28 to 540 keV LECP ions to ENAs (Dialynas et al 2020) result in ENA spectra that retain power-law slopes similar to those of the measured 5.2-55 keV ENA spectra from Cassini/INCA (Krimigis et al 2009;Dialynas et al 2020).…”
Section: Comparison Of Modeled and Observed Ena Spectramentioning
confidence: 57%
“…Spectral agreements between Cassini/ INCA ENA measurements and the Voyager ion measurements suggest that the source of ENA emissions at energies above 5.2 keV are most likely produced by charge-exchange interactions inside the HS (Dialynas et al 2013(Dialynas et al , 2017. Therefore, understanding the PUI distribution downstream of the TS is essential to study the pressure balance and acceleration mechanisms inside the HS (Dialynas et al 2019(Dialynas et al , 2020. This understanding is needed to determine the emission of ENAs from the HS because these ENAs are used to remotely sense the boundaries of our heliosphere and its interaction with the VLISM.…”
Section: Introductionmentioning
confidence: 99%