First Detection of [SI] in Near-IR JWST Observations of Io in Eclipse, and Comparison With SO Emissions, Evolving Volcanic Eruptions, and Prior UV HST-STIS [SI] Emissions
posted on 2025-11-20, 14:19authored byI de Pater, DF Strobel, AG Davies, J Saur, L Roth, K de Kleer, E Lellouch, Z Milby, C Schmidt, T Fouchet, MH Wong, Leigh FletcherLeigh Fletcher, J Harkett, M Roman, RJ Cartwright, JE Perry, J Renaud-Kim, C Jordan, S Schlegel, DA Williams, DM Nelson
We observed Io with the James Webb Space Telescope (JWST) NIRSpec/Integral Field Unit (1.0–5.3 μm, (Formula presented.)) in August 2023 while the satellite was in eclipse. Thermal emission from Kanehekili Fluctus is consistent with the cooling of lava flows after a vigorous eruption in November 2022. At Loki Patera, after a new brightening event was detected in November 2022, the lava lake was in a quiescent state, as expected from previous analyses. We mapped the SO emission band at 1.707 μm, and detected, for the first time, [SI] emission lines at 1.082 and 1.131 μm. The SO emissions are concentrated above Kanehekili Fluctus, and in two regions in the northern hemisphere. The disk-averaged brightness is 14.5 kR. The emissions are sourced from SO molecules ejected from 1,500 to 1,700 K vents in an excited state, with a typical SO column density above the northern hemisphere of (Formula presented.) (Formula presented.). Sulfur emissions are distributed homogeneously across a band in the northern hemisphere. The disk-averaged total brightness is 5.6 kR, versus 9.65 kR in the north. The emissions are produced through direct electron impact excitation by (Formula presented.) 4 eV electrons in the torus (density 2,500 (Formula presented.)) penetrating the atmosphere, and require the atmosphere to be hot ((Formula presented.) 1,700 K) to populate the upper levels before excitation. The sulfur column density over the northern hemisphere is (Formula presented.) (Formula presented.). These same parameters can explain recent 0.7725- (Formula presented.) m observations, as well as the 147.9-nm multiplet emissions observed with HST-STIS (Formula presented.) 20 years earlier. This suggests a quite stable system over decades-long timescales.<p></p>
Funding
Space Telescope Science Institute. Grant Number: JWST-ERS-01373
NASA : HST-GO-15425.002-A : NAS 5-26555. Grant Numbers: NAS 5-03127, 80NSSC22K0954, 80NSSC21K1138, HST-GO-17470, 80NM0018F0612
European Research Council. Grant Number: 884711
ANR. Grant Number: ANR-21-CE49-0020-01
A Consolidated Grant Proposal for Solar and Planetary Science at the University of Leicester, 2022 - 2025
The JWST data were obtained from the Mikulski Archive for Space Telescopes at the Space Telescope Science Institute, Observations #35 and #36 of ERS program #1373. The specific observations analyzed can be accessed via de Pater (2024). The Keck data were obtained from the Keck Archive (https://koa.ipac.caltech.edu). Juno/JIRAM data are published by Perry et al. (2025).
The data were reduced with the standard JWST pipeline (https://jwst-docs.stsci.edu/jwst-science-calibration-pipeline-overview) and a simple IDL command to correct the data for the 1/f noise, as described in Section 2 (the 1/f noise correction can now be done using the latest JWST pipeline). The resulting fits files were read into IDL, and aligned by using the Fast Fourier transform (FFT) cross-correlation algorithm. These data cubes were inspected and numerous cosmic rays and bad pixels were removed (mostly by hand), as explained in the text. To make spectra the authors used IDL routine apphot.pro (Perrin, 2013), after expanding the images by a factor of 5, and interpolating to the smaller-sized pixels.
The final cleaned spectral data cubes are uploaded to Zenodo. de Pater (2025a) contains the cleaned data cubes from the November 2022 dataset. de Pater (2025b) contains the data sets from 4 August 2023. de Pater (2025c) contains the data sets from 23 August 2023. Thermal emission, SO and [SI] spectra as displayed in the various figures can be retrieved from de Pater (2025d).