The intensity of the SO2 signal in WASP-39b varies through epochs, contrary to the CO2 signal which remains stable (figure adapted from Figure 2 in the main paper)
This kind of variability is a hallmark of a satellite source. A moon orbiting its planet will naturally change its position relative to our line of sight, sometimes contributing more gas to the observed spectrum, sometimes less. In our Solar System, Io’s volcanic torus produces exactly this sort of variability in Jupiter’s environment.
So, to test the idea, the group behind this research built simulations of WASP-39b’s system. By adding a putative moon (call it WASP-39b I) and letting it vent SO2, sodium, and potassium, they were able to reproduce many of the spectral features seen in real JWST and Hubble data.
The numbers are staggering. The models suggest such a moon could outgas material at rates more than 100 times greater than Io, driven by tidal heating (which is the process where an astronomical body’s interior warms up due to the gravitational stretching and squeezing it experiences while orbiting another body) far stronger than anything in our Solar System.
How tidal heating powers eruptions
Why would an exomoon be so much more active than Io? The answer lies in its environment. Hot Jupiters like WASP-39b orbit extremely close to their stars. A moon in such a system doesn’t just feel the tug of its planet; it’s also constantly pulled by the star’s gravity. The result is a complex three-body tidal interaction that pumps enormous amounts of energy into the moon’s interior.
Calculations show that this three-body heating could exceed the volcanic output of Io by an order of magnitude or more. Instead of sporadic eruptions, such a moon might experience continuous, planet-reshaping volcanism, constantly spewing out SO2, sodium, potassium, and other gases into space.
Those gases wouldn’t just vanish. They would form clouds and toroidal (doughnut-shaped) structures around the planet, just as Io and Enceladus do around Jupiter and Saturn. From Earth, those extended clouds could show up in exoplanet transmission spectra, masquerading as part of the planet’s atmosphere.
Could such a moon survive?
One obvious question is whether a moon could even exist in such an extreme system. Close-in gas giants are often thought to lose their moons due to tidal forces, orbital decay, or outright disintegration near the Roche limit (the point where a moon is torn apart by its planet’s gravity).
The simulations suggest that a moon around WASP-39 b could indeed be stable, at least for billions of years. Its orbit would sit comfortably within the planet’s Hill sphere (the region where the planet’s gravity dominates over the star’s), and migration timescales are long enough that it wouldn’t quickly spiral inwards.