Synergistic observations of the giant planets with HST and JWST: Jupiter's auroral emissions

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Synergistic observations of the giant planets with HST and JWST: Jupiter's auroral emissions Denis GRODENT Laboratory for Planetary and Atmospheric Physics Université de Liège Belgium

Denis GRODENT Jean-Claude GERARD Bertrand BONFOND Aikaterini RADIOTI Zhonghua YAO Benjamin PALMAERTS Maïté DUMONT 37 HST programs, giant planets aurora GTO-1269 (FOC) in 1991 C0 GO-14634 (STIS) Juno era 2016-2018

First published image of Jupiter s FUV Ly-α aurora FOC (DD time) Dols et al., 1992 F. Paresce

star.ulg.ac.be More than 100 researchers Planetology Stellar Physics Extragalactic Astrophysics & Astro-particles Instrumentation Trappist-1

Instrumentation Centre Spatial de Liège HST - FOC Development of the photon counting detector and space qualification of the FOC instrument

Instrumentation Centre Spatial de Liège JWST - MIRI Contribution to the Input Optics and Calibration Unit (IOC), the Instrument Control Electronics (ICE) and various optics for MIRIM

Solar System Planets Jupiter s aurora OK HST OK JWST «JWST will be able to observe the outer planets without saturating in at least some modes.»

Auroral process applies to all magnetized bodies surrounded by plasma Brown dwarf aurora (Hallinan et al., 2015) Maxwell-Faraday induction law Ganymede aurora (Saur et al., 2015) Ampere law Nichols, 2011 Current system

Jupiter (North) FUV aurora HST STIS TTAG F25SRF2 MIRFUV GO-14634 H2 / H / He /CH4 Total emitted UV Power ~1 TW ~200km/pix 30sec

Saturn (South) FUV aurora HST STIS Accum 25MAMA MIRCUV GO-10083 540 sec ~500km/pix 0.1 TW Clarke et al., 2005

Uranus (?) FUV aurora HST STIS Accum F25MAMA MIRCUV GO-12601 1000 sec ~1000km/pix 0.001 TW Lamy et al., 2012

John Spencer, SwRI

NASA Juno mission 53.5d orbit PJ03 Magnetic coordinates (tilted) Sun

Jupiter (North) FUV aurora HST STIS TTAG F25SRF2 MIRFUV GO-14634 151 HST orbits Coordinated with Juno PI: D. Grodent

Magnetic Anomaly near the surface of Jupiter Grodent et al., 2008

Multiple satellite footprints D TEB =max D RAW =max Bonfond et al., 2016 D TEB =max D RAW =min Bonfond et al., 2016

Spectral auroral scan (unsupported mode) HST STIS FUV MAMA G140L slit 52x0.5 1425A

EUV - FUV aurora H2 + e H2* + e H2 + hν H2 + e H + H* + e 2H + hν Grodent et al., 2001

IR aurora H2 + e H2 + + 2e H2 + + H2 H3 +* + H H3 +* H3 + + hν H3 + + CH4 CH5 + + H2 H3 + + e H2 + H H3 +* + H2 H3 + + H2* H2 * H2 + hν τ ~1000 sec H2 quadrupolar Grodent et al., 2001

Jupiter IR aurora ESO VLT CRIRES (AO, 8m) Spectral scan (similar to UV) pixel scale ~0.1 (0.2, STISx8) L-band 3-4 μm long-slit 10 sec for 15 min Stallard et al., 2016

Jupiter IR aurora NASA IRTF NSFCam (3m) 120 sec Images Pixel scale ~0.15 (0.2 STISx8) narrow band 3.45 μm Stallard et al., 2016

Subaru Telescope 0.2 resolution with AO. 10 x 2 sec exposures. Unpublished material, courtesy Hadjime KITA, Haruna WATANABE (Tohoku Univ.) 8.2 m. National Astronomical Observatory of Japan, Mauna Kea Spatial resolution appears to be limited by H3 + lifetime (several minutes)

Juno - Jupiter flyby (next PJ05 on March, 27) JIRAM high-res images of the IR aurora NASA s eyes

Adriani et al., 2014

100 km/pix A. Adriani and the JIRAM Team

With appropriate IR instrument, it is possible to achieve the same image quality as that offered by HST-STIS in the UV. However, UV and IR do not show exactly the same features (ionospheric convection motion, Joule heating, atmospheric Temperature, ). Use JWST! Possible to use JWST for Jupiter s aurora? Yes, NIRCam (NIRSpec) is perfectly suited

0.032 /pix Near-infrared spectra of the four giant planets compared to the saturation limits of NIRCam filters, assuming 640 640 pixel sub-array imaging. H2 (2.12 μm) H3 + (3.3-3.6 μm) 0.065 /pix Norwood et al., 2015

Possible configuration for observing Jupiter using the 640x640 sub-arrays on NIRCam Norwood et al., 2015

0.2 x3 slit 3 x3 @ 0.1 IFU Near-infrared spectra of the four giant planets compared to saturation limits of the NIRSpec IFU (black) and slit (red). Maximum spectral resolution mode (R=2700). Gray regions = 30% uncertainty in the saturation values. H2 (2.12 μm) H3 + (3.3-3.6 μm) Norwood et al., 2015

Thank You!