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Table 2

Compositional constraints for the crater floors (f) and ejecta blankets (e) of the dune and plain craters given by percentages of the six main constituents (H2O, NH3, CO2, CH4 -like, tholin-like, and dark material).

Dune craters Ksa Selk Santorini Guabonito
Unit f e f e f e f e
Tholin 16% 47% 21% 36% 30% 42% 13% 40%
(± 4%) (± 13%) (± 6%) (± 13%) (± 5%) (± 11%) (± 3%) (± 11%)
Dark material 84% 53% 79% 64% 70% 58% 87% 60%
(± 7%) (± 15%) (± 8%) (± 15%) (± 8%) (± 13%) (± 10%) (± 15%)
H2O
CH4-like
NH3
CO2
Emissivity 0.92 0.93 0.93 0.85 1 0.95 0.98 0.95
Degradation state well-preserved intermediate degraded degraded

Plain craters Forseti Afekan Soi
Unit f e f e f e
Tholin 53% 46% 54% 50% 80% 82%
(± 17%) (± 15%) (± 15%) (± 13%) (± 16%) (± 15%)
Dark material 27% 24% 31% 30%
(± 8%) (± 7%) (± 7%) (± 10%)
H2O 20% 30% 15% 12% 20% 18%
(± 5%) (± 5%) (± 3%) (± 3%) (± 5%) (± 5%)
CH4-like 8%
(± 2%)
NH3
CO2
Emissivity 0.93 0.83 0.95 0.93 0.93 0.90
Degradation state intermediate intermediate degraded

Special cases Menrva Sinlap
Unit f e f e
Tholin 82% 83% 15% 22%
(± 19%) (± 18%) (± 4%) (± 5%)
Dark material 65% 53%
(± 6%) (± 13%)
H2O 18% 17% 20% 15%
(± 5%) (± 4%) (± 5%) (± 5%)
CH4 -like 10%
(± 3%)
NH3
CO2
Emissivity 0.90 0.87 0.84 0.85
Degradation state well-preserved well-preserved

Notes. The associated error under each percentage corresponds to the uncertainty of the abundances of the component within the mixtures. The microwave emissivity measurements from the Cassini RADAR radiometry data set are provided in Werynski et al. (2019) and shown in Fig. 1c. As in Werynski et al. (2019), we interpret the low emissivity values (<0.90) to be consistent with an enrichment in water ice and the high emissivity values (>0.95) with an enrichment in organic materials in the top decimeter of the regolith. The relative degradation state is taken from information in Neish et al. (2013, 2018), and Werynski et al. (2019).

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