Observations of the [CI] (3P1^3P_1-3P0^3P_0) emission toward the massive star-forming region RCW38: further evidence for highly-clumped density distribution of the molecular gas

preprint2020arXivOpen access

Abstract

We present observations of the 3P1^3P_1-3P0^3P_0 fine-structure line of atomic carbon using the ASTE 10 m sub-mm telescope towards RCW38, the youngest super star cluster in the Milky Way. The detected [CI] emission is compared with the CO JJ = 1-0 image cube presented in Fukui et al. (2016) which has an angular resolution of 40′′^{\prime \prime} (∼\sim 0.33 pc). The overall distribution of the [CI] emission in this cluster is similar to that of the 13^{13}CO emission. The optical depth of the [CI] emission was found to be ττ = 0.1-0.6, suggesting mostly optically thin emission. An empirical conversion factor from the [CI] integrated intensity to the H2_2 column density was estimated as X[CI]X_{\rm [CI]} = 6.3 ×\times 1020^{20} cm−2^{-2} K−1^{-1} km−1^{-1} s (for visual extinction: AVA_V ≤\le 10 mag) and 1.4 ×\times 1021^{21} cm−2^{-2} K−1^{-1} km−1^{-1} s (for AVA_V of 10-100 mag). The column density ratio of the [CI] to CO (N[CI]/NCON_{\rm [CI]}/N_{\rm CO}) was derived as ∼\sim 0.1 for AVA_V of 10-100 mag, which is consistent with that of the Orion cloud presented in Ikeda et al. (2002). However, our results cover an AVA_V regime of up to 100 mag, which is wider than the coverage found in Orion, which reach up to ∼\sim 60 mag. Such a high [CI]/CO ratio in a high AVA_V region is difficult to be explained by the plane-parallel photodissociation region (PDR) model, which predicts that this ratio is close to 0 due to the heavy shielding of the ultraviolet (UV) radiation. Our results suggest that the molecular gas in this cluster is highly clumpy, allowing deep penetration of UV radiation even at averaged AVA_V values of 100 mag. Recent theoretical works have presented models consistent with such clumped gas distribution with a sub-pc clump size (e.g., Tachihara et al. 2018).

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