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Table 1

Selected parameters of the main experiments.

Experiment n Thickness
[μm]
Penetration depth Stopping power Density



[μm] [eV/A] [eV/16u] [g cm−3]
VUV IR 10−15
CO2 at 20 K 1.35 0.24 ± 0.02 (a) 0.53 ± 0.11 (b) 0.04 2.85 7.79 0.98(c)
CO2 at 75 K 1.35 0.24 ± 0.02 (a) 0.25 ± 0.05 (b)
H2O at 20 K 1.34 0.12 ± 0.01 (a) 0.76 ± 0.15 (b) 0.06 1.66 4.45 1.07(d,e)
H2O at 80 K(f) 1.06 ± 0.22 (b) 0.94(e,g)
CO2:H2O (6:1) at 20 K 1.36 0.96 ± 0.09 (a) 1.87 ± 0.38 (b) 0.04 2.7 7.37 1.0(h)
CO2:H2O (6:1) at 80 K 1.36 0.96 ± 0.09 (a) 1.57 ± 0.32 (b) 1.0(h)

[nm] 10−16

a-H2CO3 irr at 20 K(i,j) 0.79 ± 0.16 (b) 0.06 0.02 0.59 1.0(k)
c-H2CO3 irr at 20 K(i,j) 4.81 ± 0.98 (b) 0.13 3.57
a-H2CO3 irr at 80 K(i,j) 1.09 ± 0.22 (b) 0.03 0.81
c-H2CO3 irr at 80 K(i,j) 2.41 ± 0.49 (b) 0.07 1.79

Notes. (a) The uncertainty in the ice thickness values is calculated by assuming a 10% error in the estimation of n; (b) the uncertainty in the ice thickness values is calculated by assuming a 10% error in the band strength and density of the ice; (c) Luna et al. (2012); (d) Narten et al. (1976); (e) Jenniskens & Blake (1994); (f) laser measurement not recorded; (g)Sceats & Rice (1982);(h)average value for a CO2 :H2O (6:1) mixture; (i)a- and c-H2CO3 stand for amorphous and crystalline H2CO3 ice, synthesized at either 20 or 80 K and then annealed to 200 and 220 K, respectively; (j) solid H2CO3 is thinner than the penetration depth of 1 keV electrons; (k) assumed value (Peeters et al. 2010).

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