Open Access

This article has an erratum: [https://doi.org/10.1051/0004-6361/201834787e]


Fig. 7

image

Left: H2O:CH3COOCH3 100:13 ice-film experiment. Right, top panel: ice column density measurements from IR spectra. The black dashed lines represent the fits to the destruction cross section of water and CH3COOCH3. Middle panel: QMS-normalised masses we used to follow water, methanol, and m = 28 (CO, H2CO, and CO2) upon irradiation. m = 28 increases atthe beginning because it is mainly composed of fragments from the radiolytic products of the initial ice mixture. Lower panel: CH3COOCH3/H2O abundance ratio deduced from the IR spectra of the ice film as a function of fluence (red dots). Comparison with the QMS-determined abundance ratio of the same desorbed molecules (dark blue line). The blue and cyan star indicates the gas ratio measurement with the QMS during the ice-film deposition.

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