Composition ,
Moon and Callisto of dark cratered plains (red) and the
Asgard impact structure (blue), showing the presence of more water ice (
absorption bands from 1 to 2
μm) and less rocky material within Asgard The average
density of Callisto, 1.83 g/cm3, The mass fraction of ices is 49–55%. and possibly
ammonia and various
organic compounds. is darker than the trailing one. This is different from other
Galilean satellites, where the reverse is true. Many fresh
impact craters like
Lofn also show enrichment in carbon dioxide. It was found that Callisto responds to Jupiter's varying background magnetic field like a perfectly
conducting sphere; that is, the field cannot penetrate inside Callisto, suggesting a layer of highly conductive fluid within it with a thickness of at least 10 km. In this case the water-and-ice layer can be as thick as 250–300 km.—0.3549 ± 0.0042—determined during close flybys) suggest that, if Callisto is in
hydrostatic equilibrium, its interior is composed of compressed
rocks and
ices, with the amount of rock increasing with depth due to partial settling of its constituents. In other words, Callisto may be only partially
differentiated. The density and moment of inertia for an equilibrium Callisto are compatible with the existence of a small
silicate core in the center of the planet. The radius of any such core cannot exceed 600 km, and the density may lie between 3.1 and 3.6 g/cm3. However, a 2011 reanalysis of
Galileo data suggests that Callisto is not in hydrostatic equilibrium. In that case, the gravity data may be more consistent with a more thoroughly differentiated Callisto with a hydrated silicate core.
Surface features The ancient surface of Callisto is one of the most heavily
cratered in the Solar System. In fact, the crater density is close to
saturation: any new crater will tend to erase an older one. The large-scale
geology is relatively simple; on Callisto there are no large mountains, volcanoes or other
endogenic tectonic features. The impact craters and multi-ring structures—together with associated
fractures,
scarps and
deposits—are the only large features to be found on the surface. the surrounding terrain. They are possible
cryovolcanic deposits. with a central dome.
Chains of
secondary craters from formation of the more recent crater
Tindr at upper right crosscut the terrain Impact crater diameters seen range from 0.1 km—a limit defined by the
imaging resolution—to over 100 km, not counting the multi-ring structures. The second largest is
Asgard, measuring about 1,600 km in diameter. The most likely candidate process is the slow
sublimation of ice, which is enabled by a temperature of up to 165
K, reached at a subsolar point. Absolute dating has not been carried out, but based on theoretical considerations, the cratered plains are thought to be ~4.5
billion years old, dating back almost to the formation of the
Solar System. The ages of multi-ring structures and impact craters depend on chosen background cratering rates and are estimated by different authors to vary between 1 and 4 billion years.. While CO2 was the first constituent identified, the presence of a substantial O2 component has been inferred through observations of the moon’s ionospheric density and far-ultraviolet auroral emissions. The CO2 component was initially detected by the
Galileo Near Infrared Mapping Spectrometer (NIMS) via a prominent absorption feature at 4.22
μm. Recent spectral analysis from ground-based facilities has confirmed that this CO2 is not merely localized but exists as a thin global gaseous envelope. The surface pressure is estimated at approximately 7.5 picobar (0.75
μPa), corresponding to a neutral particle density of ≈ 4 x 108 cm-3. However, the inferred molecular oxygen column density is significantly higher, with values in the range of 4 x 1014 cm-2 to 4 x 1015 cm-2 depending on the solar zenith angle and orbital position. Because this exosphere is considered non-collisional and would be depleted by atmospheric escape on timescales of approximately four years, it requires continuous replenishment. The O2 source remains a subject of active debate. Current kinetic modeling indicates that standard radiolysis of exposed surface ice (about ~10% of the total surface for the model) fails to account for the observed O2 densities by two to three orders of magnitude. Even if a model assumes the surface is 100% ice, the radiolysis induced in the ice would still be an insufficient source to produce the values inferred from observations. Hybrid modeling demonstrates that Callisto's ionosphere effectively diverts magnetospheric plasma flow around the moon, shielding the surface and reducing the efficiency of radiolysis-driven production. To resolve this gap, current research suggests that the exosphere may be supplied by a reservoir of O2 trapped within the porous regolith or radiation-altered ice grains, which then thermally releases into the atmosphere. Callisto's ionosphere was initially identified through Galileo radio occultations, which revealed peak electron densities ranging from approximately 1.5 to 1.7 x 104 cm-3 Spectral images taken on 15 and 24 December 2001 were re-examined, revealing a faint signal of scattered light that indicates a hydrogen corona. The observed brightness from the scattered sunlight in Callisto's hydrogen corona is approximately two times larger when the leading hemisphere is observed. This asymmetry may originate from a different hydrogen abundance in both the leading and trailing hemispheres. However, this hemispheric difference in Callisto's hydrogen corona brightness is likely to originate from the extinction of the signal in Earth's
geocorona, which is greater when the trailing hemisphere is observed. This detection supports earlier constraints from the Hubble Space Telescope that estimated the O2 column density is significantly high, in the range of ~1015 cm-2. ==Origin and evolution==