The PDR structure and kinematics around the compact H II regions S235 A and S235 C with [C II], [13C II], [O I], and HCO+ line profiles
Schneider, N.; Samal, M. R.; Okada, Y.; Buchbender, C.; Andersen, M.; Anderson, L. D.; Kirsanova, M. S.; Sobolev, A. M.; Boley, P. A.; Aladro, R.; Ossenkopf-Okada, V.; Pavlyuchenkov, Ya N.; Bieging, J. H.; Luisi, M.
Russia, Germany, United States, Chile, India
Abstract
The aim of this work is to study structure and gas kinematics in the photodissociation regions (PDRs) around the compact H II regions S235 A and S235 C. We observe the [C II], [13C II], and [O I] line emission, using SOFIA/upGREAT, and complement them by data of HCO+ and CO. We use the [13C II] line to measure the optical depth of the [C II] emission, and find that the [C II] line profiles are influenced by self-absorption, while the [13C II] line remains unaffected by these effects. Hence, for dense PDRs, [13C II] emission is a better tracer of gas kinematics. The optical depth of the [C II] line is up to 10 in S235 A. We find an expanding motion of the [C II]-emitting layer of the PDRs into the front molecular layer in both regions. Comparison of the gas and dust columns shows that gas components visible neither in the [C II] nor in low-J CO lines may contribute to the total column across S235 A. We test whether the observed properties of the PDRs match the predictions of spherical models of expanding H II region + PDR + molecular cloud. Integrated intensities of the [13C II], [C II], and [O I] lines are well represented by the model, but the models do not reproduce the double-peaked [C II] line profiles due to an insufficient column density of C+. The model predicts that the [O I] line could be a more reliable tracer of gas kinematics, but the foreground self-absorbing material does not allow using it in the considered regions.