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CH3CCH as a thermometer in warm molecular gas

Yuqiang Li, Junzhi Wang, Juan Li, Xing Lu, Siqi Zheng, Chao Ou, Qian Huang, Miguel Santander-García, José Jairo Díaz Luis, Seokho Lee, Tie Liu, Zhiqiang Shen

TL;DR

This study directly compares CH3CCH and NH3 as thermometers in warm molecular gas around massive young stars. Using CH3CCH J=5-4 observations (55 detections) and NH3 (1,1)–(2,2) data (33 sources) across 55 regions, it shows that CH3CCH rotation temperatures better reflect the kinetic temperature than NH3 in the 20–100 K range. Statistical-equilibrium modeling confirms CH3CCH tracks $T_{kin}$ for densities above ~1×10^4 cm^-3, while NH3 becomes insensitive at higher temperatures, leading to systematic underestimation. The results advocate CH3CCH as the preferred thermometer for warm gas in massive star-forming regions and highlight the limitations of NH3-based thermometry in this regime.

Abstract

Kinetic temperature is a fundamental parameter in molecular clouds. Symmetric top molecules, such as NH$_3$ and CH$_3$CCH, are often used as thermometers. However, at high temperatures, NH$_3$(2,2) can be collisionally excited to NH$_3$(2,1) and rapidly decay to NH$_3$(1,1), which can lead to an underestimation of the kinetic temperature when using rotation temperatures derived from NH$_3$(1,1) and NH$_3$(2,2). In contrast, CH$_3$CCH is a symmetric top molecule with lower critical densities of its rotational levels than those of NH$_3$, which can be thermalized close to the kinetic temperature at relatively low densities of about 10$^{4}$ cm$^{-3}$. To compare the rotation temperatures derived from NH$_3$(1,1)$\&$(2,2) and CH$_3$CCH rotational levels in warm molecular gas, we used observational data toward 55 massive star-forming regions obtained with Yebes 40m and TMRT 65m. Our results show that rotation temperatures derived from NH$_3$(1,1)$\&$(2,2) are systematically lower than those from CH$_3$CCH 5-4. This suggests that CH$_3$CCH rotational lines with the same $J$+1$\rightarrow$$J$ quantum number may be a more reliable thermometer than NH$_3$(1,1)$\&$(2,2) in warm molecular gas located in the surroundings of massive young stellar objects or, more generally, in massive star-forming regions.

CH3CCH as a thermometer in warm molecular gas

TL;DR

This study directly compares CH3CCH and NH3 as thermometers in warm molecular gas around massive young stars. Using CH3CCH J=5-4 observations (55 detections) and NH3 (1,1)–(2,2) data (33 sources) across 55 regions, it shows that CH3CCH rotation temperatures better reflect the kinetic temperature than NH3 in the 20–100 K range. Statistical-equilibrium modeling confirms CH3CCH tracks for densities above ~1×10^4 cm^-3, while NH3 becomes insensitive at higher temperatures, leading to systematic underestimation. The results advocate CH3CCH as the preferred thermometer for warm gas in massive star-forming regions and highlight the limitations of NH3-based thermometry in this regime.

Abstract

Kinetic temperature is a fundamental parameter in molecular clouds. Symmetric top molecules, such as NH and CHCCH, are often used as thermometers. However, at high temperatures, NH(2,2) can be collisionally excited to NH(2,1) and rapidly decay to NH(1,1), which can lead to an underestimation of the kinetic temperature when using rotation temperatures derived from NH(1,1) and NH(2,2). In contrast, CHCCH is a symmetric top molecule with lower critical densities of its rotational levels than those of NH, which can be thermalized close to the kinetic temperature at relatively low densities of about 10 cm. To compare the rotation temperatures derived from NH(1,1)(2,2) and CHCCH rotational levels in warm molecular gas, we used observational data toward 55 massive star-forming regions obtained with Yebes 40m and TMRT 65m. Our results show that rotation temperatures derived from NH(1,1)(2,2) are systematically lower than those from CHCCH 5-4. This suggests that CHCCH rotational lines with the same +1 quantum number may be a more reliable thermometer than NH(1,1)(2,2) in warm molecular gas located in the surroundings of massive young stellar objects or, more generally, in massive star-forming regions.
Paper Structure (10 sections, 4 equations)