MIST
Magnetosphere, Ionosphere and Solar-Terrestrial
Temporal Variability of Saturn's H2 Dayglow and Northern Aurora Observed by Hisaki and Cassini
Temporal Variability of Saturn's H2 Dayglow and Northern Aurora Observed by Hisaki and Cassini
By Leah Clare (Lancaster University)
The ultraviolet (UV) emissions from Saturn are composed of the dayglow from the sunlit atmosphere and the aurorae at the poles. Investigation into the daily variability of the dayglow remains somewhat unconstrained, particularly on timescales of weeks. Utilising coincident Hisaki and Cassini observations across ~3 weeks in 2014, we determine the temporal variability of the UV emitted power, assess the response of the dayglow to solar activity, and constrain the contribution from the northern aurora to the total emitted power. We find that the power varies by a factor of 2.26 over 23 days with Hisaki, and 1.29 over 17 days with Cassini. Upon separation of the northern auroral contribution with Cassini, the contribution is found to be between 10% - 26%. Additionally, the dayglow component displays a strong correlation with solar activity, confirming that the dayglow is controlled by the UV solar flux as shown by previous studies (Gustin et al., 2010; Liu & Dalgarno 1996). This study demonstrates the first analysis of the Saturn campaigns by Hisaki, allowing an assessment of the robustness of such a mission in observing outer planet targets. The multi-mission analysis confirmed that Hisaki was able to track the variability of the UV emissions from Saturn, with comparative trends to the Cassini data.
References:
Gustin, J., Stewart, I., Gérard, J. C., & Esposito, L. (2010). Characteristics of Saturn’s FUV airglow from limb-viewing spectra obtained with Cassini-UVIS. Icarus, 210(1), 270–283. https://doi.org/10.1016/j.icarus.2010.06.031
Liu, W., & Dalgarno, A. (1996). The Ultraviolet Spectrum of the Jovian Dayglow. The Astrophysical Journal, (462), 502–518.
See publication for more details:
https://doi.org/10.1029/2026JA035194
(a) The total emitted UV power obtained from Hisaki/EXCEED. The points are daily average H2 powers from 70 to 148 nm. (b) The total emitted UV power determined with Cassini UVIS; each point is the daily average H2 power for the wavelength range 70–148 nm. (c) The daily average solar F10.7 radio index, a proxy for EUV radiation, scaled to Saturn. Data from Space Weather Canada. (d) The solar EUV power into Saturn's thermosphere. Solar spectral irradiance data are obtained from LISIRD, which uses the Flare Solar Irradiance Model (Chamberlin et al., 2008) and Earth irradiance measurements. The calculation is from Gershman and DiBraccio (2024). (e) The solar H‐Lyman β irradiance at Saturn; data are obtained from LISIRD, which uses the Flare Solar Irradiance Model (Chamberlin et al., 2008) and Earth irradiance measurements.
Solar Activity References:
Chamberlin, P. C., Woods, T. N., & Eparvier, F. G. (2008). Flare irradiance spectral model (fism): Flare component algorithms and results. Space Weather, 6(5). https://doi.org/10.1029/2007SW000372
Gershman, D. J., & DiBraccio, G. A. (2024). Quantifying External Energy Inputs for Giant Planet Magnetospheres. Geophysical Research Letters, 51(15). https://doi.org/10.1029/2024GL109660
The Jupiter Auroral Ionosphere Code
The Jupiter Auroral Ionosphere Code
By Jonathan Nichols (University of Leicester)
We present a new model of auroral precipitation and associated phenomena at Jupiter, called the Jupiter Auroral Ionosphere Code (JAIC). The hybrid model follows the primary electron population using a Monte Carlo code that runs on a GPU, and computes the contribution of the secondaries using a two‐stream approximation. The model includes modules that compute high resolution far‐ultraviolet H2 spectra, the H3+ density using simple ion chemistry, and the resulting Pedersen conductivity and H3+ radiance. We illustrate the validity of the model and present a number of initial applications. We show that the model successfully relates Juno auroral electron and UV observations, and that an auroral polar transient form is consistent with excitation by ∼ 23± 4 keV electrons. We also compute a self‐consistent relation between field‐aligned current density and Pedersen conductance and show that it is consistent with Juno in situ observations. We suggest that Joule heating enabled by the electron contribution to the Pedersen conductivity may explain heating observed at mbar levels. We further show that, in contrast with initial analysis, polar H3+ emissions observed by the James Webb Space Telescope are consistent with the electron population above the auroral zone.
The model is publicly available at GitHub and Zenodo: https://github.com/jdnplanets/jaic
See publication for more details:
Nichols, J. D. (2026). Jupiter's auroral ionosphere: Hybrid Monte Carlo, auroral spectrum and conductivity modeling. Journal of Geophysical Research: Space Physics, 131, e2026JA035228. https://doi.org/10.1029/2026JA035228
A selection of outputs from JAIC: ionisation rates, Pedersen conductivity and FUV spectra. For further details see Nichols (2026).
Analysis of Chorus Wave Power on Burst‐Mode Timescales During the Van Allen Probes Era
Analysis of Chorus Wave Power on Burst‐Mode Timescales During the Van Allen Probes Era
By Rachel Black (University of Exeter/British Antarctic Survey)
Interactions between whistler‐mode chorus waves and electrons are a key driver of dynamics in Earth’s radiation belts. These global dynamics are often described using Fokker‐Planck diffusion models. Whilst, in many cases, such models effectively describe the large scale changes within the region, they often rely upon spatially and temporally averaged representations of the wave properties. However, observations have shown that whistler‐mode chorus can display large sub‐second powers that challenge model assumptions and potentially give rise to non‐diffusive processes.
In this work, we investigate the power of whistler‐mode chorus on sub‐second timescales using the high‐resolution data capture mode on the Van Allen Probes’ Electric and Magnetic Field Instrument Suite and Integrated Science (EMFISIS). We show that peak chorus power on sub‐second timescales is regularly larger than the corresponding spacecraft “survey” power by over a factor of 100. The work also explores the magnetospheric conditions under which the largest sub‐second power variability of chorus waves is observed, and we find that trends vary across different chorus frequency bands. Notably, the largest powers are observed in the lower‐band frequency range during active conditions and between 21:00–12:00 MLT, where >46% of burst samples contain an instantaneous wave intensity that exceeds 2.25 × 104 pT2. Further, binning the lower‐band power by the ratio of plasma‐to‐gyrofrequency separates the waves into two distinct low and high variability populations. The results quantify sub‐second wave power variability that may influence energetic electron dynamics not currently captured in time‐averaged wave models.
See publication for more details:
Black, R., Allanson, O., Meredith, N. P., Hillier, A., & Hartley, D. P. (2026). Analysis of chorus wave power on burst-mode timescales during the Van Allen Probes era. Journal of Geophysical Research: Space Physics, 131, e2026JA035082. https://doi.org/10.1029/2026JA035082
Chorus-containing records in the burst-mode measurements from the Van Allen Probes' EMFISIS instruments when at equatorial latitudes ($|\lambda_m|<$6.$^\circ$). Chorus emissions are divided into low frequency, lower-band and upper-band frequency ranges. For each frequency range, the subpanels show (a)-(c) average chorus power for corresponding survey-mode events; (d)-(f) maximum chorus power from burst-mode events; (g)-(i) ratio between the maximum burst power and the survey power; and (j)-(l) the normalized inter-quartile range ($\frac{Q3-Q1}{Q2}$) for each burst record.