5–6 Nov 2020
Europe/Amsterdam timezone

Session

Oral presentations

5 Nov 2020, 14:00

Presentation materials

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  1. Elias Roussos (Max Planck Institute for Solar System Research)
    05/11/2020, 14:00
    Oral
  2. Leonardo Regoli (Johns Hopkins University Applied Physics Laboratory)
    05/11/2020, 14:20
    Oral
  3. Nicholas Achilleos (UCL)
    05/11/2020, 14:40
    Oral
  4. Nawapat Kaweeyanun (Imperial College London)
    05/11/2020, 15:00
    Oral
  5. Fuminori Tsuchiya (Graduate school of Science, Tohoku University)
    05/11/2020, 15:20
    Poster
  6. Fran Bagenal (University of Colorado, Boulder, CO USA)
    05/11/2020, 17:20
    Oral
  7. Harry Manners (Imperial College London)
    05/11/2020, 17:40
    Oral
  8. Carl Schmidt (Boston University)
    05/11/2020, 18:00
    Oral
  9. Howard Smith (JHU APL)
    05/11/2020, 18:20
    Oral
  10. Frank Crary (University of Colorado, LASP)
    05/11/2020, 18:40
    Oral
  11. Andrew Coates (UCL Mullard Space Science Laboratory)
    05/11/2020, 19:00
    Oral
  12. George Xystouris (Lancaster University)
    06/11/2020, 14:00
    Oral
  13. Michiko Morooka (Swedish Institute of Space Physics)
    06/11/2020, 14:20
    Oral
  14. Richard Haythornthwaite (University College London)
    06/11/2020, 14:40
    Oral
  15. Geraint Jones (UCL Mullard Space Science Laboratory)
    06/11/2020, 15:00
    Oral
  16. Ali Sulaiman (University of Iowa)
    06/11/2020, 15:30
    Oral
  17. Corentin Louis (IRAP - Toulouse)
    06/11/2020, 15:50
    Oral
  18. Mats Holmstrom (Swedish Institute of Space Physics)
    06/11/2020, 16:10
    Oral
  19. Tom Nordheim (NASA JPL)
    06/11/2020, 16:30
  20. Marina Galand (Imperial College London)
    06/11/2020, 18:00
    Oral
  21. Ingo Mueller-Wodarg (Imperial College London)
    06/11/2020, 18:20
    Oral
  22. Richard Cartwright (Carl Sagan Center at the SETI Institute)
    06/11/2020, 18:40
    Oral
  23. André Galli (University of Bern)
    06/11/2020, 19:00
    Oral
  24. Howard Smith (JHU APL)
    Oral

    The Jovian system is very intriguing with extremely different particle sources ranging from the volcanic Io to the frozen world of Europa with both existing within Jupiter’s relatively high radiation magnetospheric environment. While Voyager, Galileo and Cassini provided historic observations of this unique environment, they also raised numerous questions. As the dominant source of particles...

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  25. Prof. Andrew Coates (UCL Mullard Space Science Laboratory)
    Oral

    Ion pickup provides the key mechanism by which comets interact with the solar wind. Following ionization of neutral particles, the new-born ions are accelerated in the convection electric field and gyrate around the magnetic field – forming a cycloid in real space and an unstable ring in velocity space. Pickup is present at most other planetary objects, and in the outer solar system there are...

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  26. Frank Crary (University of Colorado, LASP)
    Oral

    Key aspect of moon-magnetosphere interactions are dependent on the diversion of the flow around the conducting body of the moon and the acceleration of the flow along the flanks of the moon. Analytic solutions for the magnetic field perturbations [Neubauer, 1980; Saur et al., 2004 and references therein] have been derived assuming the moon’s conductance is constant within a specified radius...

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  27. Harry Manners (Imperial College London)
    Oral

    The plasma torus at Io’s orbit has been shown to be a locus of intense Alfvén and ion cyclotron waves, which are trapped in the region by the waveguide properties of the torus. Research featuring these waves has progressed towards a detailed understanding of temporal variability in the region, which is vital to the upcoming JUICE mission’s aim to characterise the Galilean moons. Here we show...

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  28. Dr Carl Schmidt (Boston University)
    Oral

    The Io plasma torus offers our only opportunity to take a picture of a planetary magnetosphere. Torus ion emissions are excited through electron impact and so line ratios of like ions species can effectively map the plasma density and electron temperature. This provides us with some empirical constraints on the upstream plasma conditions that sweep past the moon. A rich spectrum of emission...

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