Table 1
Deposited molecules.
Sample | Conc.a | Thicknessb | Moleculec | N d | Beam | Energy | See | Fluence | Dosef |
N2:CH4 | [μm] | [cm-2] | [MeV] | [keV μm-1] | [ions cm-2] | [eV molecule-1] | |||
|
|||||||||
a | 90:10 | 8.4 ± 0.4 | CH4 | 1.7 × 1018 | 58Ni11+ | 44 | 3794 | 1.0 × 1013 | 18 |
H2O | 1.6 × 1016 | ||||||||
b | 90:10 | 9.9 ± 0.5 | CH4 | 1.5 × 1018 | 58Ni11+ | 44 | 3794 | 3.0 × 1013 | 54 |
H2O | 1.6 × 1016 | ||||||||
c | 98:2 | 10.0 ± 0.6 | CH4 | 2.6 × 1017 | 40Ar15+ | 160 | 1617 | 3.4 × 1012 | 3 |
H2O | 8.3 × 1015 | ||||||||
d | 98:2 | 20 ± 2 | CH4 | 6.3 × 1017 | 40Ar15+ | 160 | 1617 | 2.2 × 1013 | 18 |
H2O | 4.4 × 1016 |
Notes.
The thickness is estimated from the interference fringes period via the formula e ≈ 1/2nΔν, where e is the thickness, n the refractive index of the ice film, and Δν the period of interference fringes.
Calculated with SRIM (Ziegler et al. 2010), assuming an ice density of 0.94 g cm-3 (Satorre et al. 2008).
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