Infrared images of ionized and molecular hydrogen emission in S106

被引:16
作者
Hayashi, Saeko S.
Hasegawa, Tetsuo
Tanaka, Masuo
Hayashi, Masafhko
Aspin, Colin
Mclean, Ian S.
Brand, Peter W. J. L.
Gatley, Ian
机构
[1] Joint Astron Ctr, James Clerk Maxwell Telescope, Hilo, HI 96720 USA
[2] Nobeyama Radio Observ, Nagano, Japan
[3] Univ Tokyo, Inst Astron, Tokyo 181, Japan
[4] Univ Tokyo, Dept Astron, Bunkyo Ku, Tokyo 113, Japan
[5] Joint Astron Ctr, United Kingdom Infrared Telescope, Hilo, HI USA
[6] Univ Edinburgh, Royal Observ, Dept Astron, Edinburgh EH9 3HJ, Midlothian, Scotland
[7] Natl Opt Astron Observ, Tucson, AZ 85726 USA
关键词
interstellar : molecules; nebulae : HII regions; nebulae : individual (S106); stars : formation;
D O I
10.1086/168684
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present high-resolution emission-line images of the central arcminute of S106 in Br gamma and H-2 v = 1-0 S(1). The images were taken at UKIRT through a Fabry-Perot filter of 130 km s(-1) resolution using the infrared array camera IRCAM with a pixel size of 0.'' 62. The Bry emission shows a clear bipolar distribution which resembles that of the radio continuum emission. The central dark lane caused by the disk is wider in the Bry image than in comparable radio continuum images. The molecular hydrogen emission is predicted to originate in the dynamically shocked regions and/or in the photodissociation regions formed at the interface between the H II region and the clumpy molecular gas. For the case of S106, the peaks of the H-2 emission are located similar to 5 '' outside the corresponding Bry peaks; that is, further from the central star. The assumption that this displacement corresponds to the typical depth of the H2 emitting zone in the photodissociation region, at which A(v) similar or equal to 2 mag, leads to a density estimate of similar to 10(5) cm(-3). This high density, together with the low excitation temperature reported earlier for S106, suggests that the origin of the thermal component in the H-2 emission measured by Tanaka et al. is either high-density fluorescence, that is, collisional de-excitation of the UV pumped H-2 in photodissociation regions formed on the dense molecular clumps beyond the ionization fronts, or it is radiation from slow shocks driven by the wind from the central source, propagating into the dense clumps. In either case, a novel physical environment is required to understand the observations.
引用
收藏
页码:242 / U11
页数:7
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