1. Monte Carlo modeling of Io's [OI] 6300A... and [SII] 6716A... auroral emission in eclipse
- Author
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Moore, C., Miki, K., Goldstein, D.B., Stapelfeldt, K., Varghese, P.L., Trafton, L.M., and Evans, R.W.
- Subjects
Monte Carlo method -- Models ,Monte Carlo method -- Analysis ,Volcanoes -- Models ,Volcanoes -- Analysis ,Magnetic fields -- Models ,Magnetic fields -- Analysis ,Planets -- Atmosphere ,Planets -- Models ,Planets -- Analysis ,Astronomy ,Earth sciences - Abstract
To link to full-text access for this article, visit this link: http://dx.doi.org/10.1016/j.icarus.2010.01.004 Byline: C. Moore (a), K. Miki (a), D.B. Goldstein (a), K. Stapelfeldt (a)(b), P.L. Varghese (a), L.M. Trafton (a), R.W. Evans (a)(b) Keywords: Io; Aurorae; Jupiter, Satellites; Satellites, Atmospheres; Collisional physics Abstract: We present a Monte Carlo (MC) model of [OI] 6300A and [SII] 6716A emission from Io entering eclipse. The simulation accounts for the 3-D distribution of SO.sub.2, O, SO, S, and O.sub.2 in Io's atmosphere, several volcanic plumes, and the magnetic field around Io. Thermal electrons from the jovian plasma torus are input along the simulation domain boundaries and move along the magnetic field lines distorted by Io, occasionally participating in collisions with neutrals. We find that the atmospheric asymmetry resulting from varying degrees of atmospheric collapse across Io (due to eclipse ingress) and the presence of volcanoes contributes significantly to the unique morphology of the [OI] 6300A emission. The [OI] radiation lifetime of [approximately equal to]134s limits the emission to regions that have a sufficiently low neutral density so that intermolecular collisions are rare. We find that at low altitudes (typically 4x10.sup.9 cm.sup.-3) to collisionally quench nearly all (>95%) of the excited oxygen for reasonable quenching efficiencies. Upstream (relative to the plasma flow), Io's perturbation of the jovian magnetic field mirrors electrons with high pitch angles, while downstream collisions can trap the electrons. This magnetic field perturbation is one of the main physical mechanisms that results in the upstream/downstream brightness asymmetry in [OI] emission seen in the observation by Trauger et al. (Trauger, J.T., Stapelfeldt, K.R., Ballester, G.E., Clarke, J.I., 1997. HST observations of [OI] emissions from Io in eclipse. AAS-DPS Abstract (1997DPS29.1802T)). There are two other main causes for the observed brightness asymmetry. First, the observation's viewing geometry of the wake spot crosses the dayside atmosphere and therefore the wake's observational field of view includes higher oxygen column density than the upstream side. Second, the phased entry into eclipse results in less atmospheric collapse and thus higher collisional quenching on the upstream side relative to the wake. We compute a location (both in altitude and latitude) for the intense wake emission feature that agrees reasonably well with this observation. Furthermore, the peak intensity of the simulated wake feature is less than that observed by a factor of [approximately equal to]3, most likely because our model does not include direct dissociation-excitation of SO.sub.2 and SO. We find that the latitudinal location of the emission feature depends not so much on the tilt of the magnetic field as on the relative north/south flux tube depletion that occurs due to Io's changing magnetic latitude in the plasma torus. From 1-D simulations, we also find that the intensity of [SII] 6716 and 6731A emission is much weaker than that of [OI] even if the [SII] excitation cross section is 10.sup.3 times larger than excitation to [OI]. This is because the density of S.sup.+ is much less than that of O and because the Einstein-A coefficient of the [SII] emission is a factor of [approximately equal to]10 smaller than that of [OI]. Author Affiliation: (a) The University of Texas at Austin, Austin, TX 78712, USA (b) JPL, Caltech, USA Article History: Received 28 July 2009; Revised 2 January 2010; Accepted 3 January 2010
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- 2010