Table A.1
Infrared band positions and apparent band strength (A) values of water-methanol mixed ices derived for the amorphous state at 8 K, and for a more ordered state at a higher temperature (n.d. stands for non detected).
Ice | Frequency (cm-1) | Frequencypure (cm-1)a | Temperature | A (cm molec-1)b | Apure (cm molec-1)c |
|
|||||
H2O:CH3OH (1:1) | |||||
CH3OH | n.d. | 303 | 8 | n.d. | 9.3 (4.8) × 10-20 |
H2O | 203 | 219 | ≤5.5 × 10-18d | 4.4 (1.7) × 10-18 | |
|
|||||
CH3OH | 344 | 347 | 130 | 8.1 × 10-19 | 1.3 (6.6) × 10-18e |
170f | 177 | n.d. | 8.2 (4.3) × 10-19e | ||
H2O | 215 | 227 | 4.6 × 10-18g | 5.3 (2.0) × 10-18h | |
160 | |||||
H2O:CH3OH (3:1) | |||||
CH3OH | n.d. | 303 | 8 | n.d. | 9.3 (4.8) × 10-20 |
H2O | –i | 219 | ≤5.1 × 10-18d | 4.4 (1.7) × 10-18 | |
|
|||||
CH3OH | 345 | 347 | 130 | 1.4 × 10-18 | 1.3 (6.6) × 10-18e |
176f | 177 | 8.2 (4.3) × 10-19e | |||
H2O | 219 | 227 | 5.5 × 10-18g | 5.3 (2.0) × 10-18h | |
160 | |||||
H2O:CH3OH (10:1) | |||||
CH3OH | n.d. | 303 | 8 | n.d. | 9.3 (4.8) × 10-20 |
H2O | 205 | 219 | ≤8.3 × 10-18d | 4.4 (1.7) × 10-18 | |
|
|||||
CH3OH | n.d. | 347 | 135 | n.d. | 1.3 (6.6) × 10-18e |
n.d. | 177 | n.d. | 8.2 (4.3) × 10-19e | ||
H2O | 223 | 227 | ≤5.5 × 10-18j | 5.3 (2.0) × 10-18h | |
160 |
Notes.
Peak frequency of the related band in the pure ice, from Giuliano et al. (2014).
Band strength of the related band in the pure ice, from Giuliano et al. (2014).
The band corresponding to amorphous water is blended with the wide undetected band of methanol at ~303 cm-1.
With contribution of the peak observed at ~160 cm-1 in the red side of the crystalline water far-IR band (see text).
Assuming that the band strength of the ~177 cm-1 vibrational mode is modified by the same factor than the ~347 cm-1 mode with respect to the pure ice case, and substracting the hypothetical area of the ~177 cm-1 band to the total area of the ~227 cm-1 band.
The band was detected, but the peak frequency could not be derived because of the noise in that region of the spectrum (see Fig. 4).
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