JWST observations of segregated $^{12}$CO$_2$ and $^{13}$CO$_2$ ices in protostellar envelopes

TL;DR

This study uses JWST observations to analyze the vibrational modes of $^{12}$CO$_2$ and $^{13}$CO$_2$ ices in protostellar envelopes, revealing segregation due to heating and consistent isotopic ratios, advancing understanding of interstellar ice evolution.

Contribution

First detailed profile decomposition of CO$_2$ ice vibrational modes in protostars, showing segregation and isotopic consistency, with implications for ice formation and thermal processing.

Findings

CO$_2$ ice segregates from water-rich layers upon heating.

Similar $^{12}$CO$_2$ and $^{13}$CO$_2$ contributions suggest minimal fractionation.

Derived $^{12}$C/$^{13}$C ratio of 90 ± 9 in IRAS 20126.

Abstract

The evolution of interstellar ices can be studied with thermal tracers such as the vibrational modes of CO$_2$ ice that show great diversity depending on their local chemical and thermal environment. In this work we present JWST observations of the 15.2 $\mu$m bending mode, the 4.39 $\mu$m stretching mode and the 2.70 $\mu$m combination mode of $^{12}$CO$_2$ and $^{13}$CO$_2$ ice in the high-mass protostar IRAS 20126 and the low-mass protostar Per-emb 35. The 15.2 $\mu$m bending mode of both protostars shows the characteristic double peak profile that is associated with pure CO$_2$ ice and a sharp short-wavelength peak is observed at 4.38 $\mu$m in the $^{13}$CO$_2$ bands of the two sources. Furthermore, a narrow short-wavelength feature is detected at 2.69 $\mu$m in the $^{12}$CO$_2$ combination mode of Per-emb 35. We perform a consistent profile decomposition on all three vibrational modes and show that the profiles of all three bands can be reproduced with the same linear combination of CO$_2$ ice in mixtures with mostly CH$_3$OH and H$_2$O ices when the ices undergo segregation due to heating. The findings show that upon heating, CO$_2$ ice is likely segregating from mostly the water-rich ice layer and the CO$_2$-CH$_3$OH component becomes dominant in all three vibrational modes. Additionally, we find that the contribution of the different CO$_2$ components to the total absorption band is similar for both $^{12}$CO$_2$ and $^{13}$CO$_2$. This indicates that fractionation processes must not play a significant role during the different formation epochs, H$_2$O-dominated and CO-dominated. We quantify the $^{12}$CO$_2$ and $^{13}$CO$_2$ ice column densities and derive $^{12}$C/$^{13}$C$_{ice}$ = 90 $\pm$ 9 in IRAS 20126. Finally, we report the detection of the $^{13}$CO$_2$ bending mode of pure CO$_2$ ice at 15.64 $\mu$m in both IRAS 20126 and Per-emb 35.