论文标题
扩展的HNCO,SIO和HC $ _ {3} $ n在43 Southern Star形成区域排放
Extended HNCO, SiO, and HC$_{3}$N emission in 43 southern star-forming regions
论文作者
论文摘要
我们已经选择了43个南部大型星形形成区域来研究HNCO 4 $ _ {04} $ - 3 $ _ {03} $,SIO 2-1和HC $ _ {3} $ n 10-9行排放并调查与尘埃排放的空间关联的空间分布。 HNCO 4 $ _ {04} $ - 3 $ _ {03} $和HC $ _ {3} $ N 10-9的形态与灰尘排放吻合很吻合。 HC $ _ {3} $ N 10-9倾向于起源于比HNCO 4 $ _ {04} $ -3 $ _ {03} $和SIO 2-1的更紧凑区域。我们将我们的源分为三组:中央分子区(CMZ),与气泡(气泡)相关的源和其余的来源,这些来源称为“正常恒星形成区域”(NMSFR)。这三个组分为三个不同的类别,相对于线条宽度,集成强度和柱密度,暗示存在不同的物理和化学过程。我们发现,灰尘温度$ t _ {\ rm d} $,并且丰度比为$ n _ {\ rm hnco}/n _ {\ rm sio} $和$ n _ {\ rm hnco hnco}/n _ {\ rm hnco}/n _ {\ rm hc3n} $ shounters of Centeral to Centernal to Centernal to Centernal to Centernal s sir sir sil d d sir sil d d sir sil d ded sirs $ n _ {\ rm hc3n}/n _ {\ rm sio} $移动到相反的方向。此外,在Bubble和NMSFR类别中找到了更好的协议,在$ t _ {\ rm d} $和$ n _ {\ rm hc3n}/n _ {\ rm sio} $之间。在16个气泡和NMSFR来源中的八个中都发现了流出和流入活动。低流出检测率表明,在这些来源中,SIO 2-1线翼的发射要么低于我们的敏感性极限,要么大部分SIO发射可以通过扩展H {\ sc \,II}区域或超级诺物Remnant来产生,这使得分子燃气会推动分子燃气形成冲击和产量SIO。
We have selected 43 southern massive star-forming regions to study the spatial distribution of HNCO 4$_{04}$-3$_{03}$, SiO 2-1 and HC$_{3}$N 10-9 line emission and to investigate their spatial association with the dust emission. The morphology of HNCO 4$_{04}$-3$_{03}$ and HC$_{3}$N 10-9 agrees well with the dust emission. HC$_{3}$N 10-9 tends to originate from more compact regions than HNCO 4$_{04}$-3$_{03}$ and SiO 2-1. We divided our sources into three groups: those in the Central Molecular Zone (CMZ), those associated with bubbles (Bubble), and the remaining sources, which are termed 'normal star forming regions' (NMSFR). These three groups, subdivided into three different categories with respect to line widths, integrated intensities, and column densities, hint at the presence of different physical and chemical processes. We find that the dust temperature $T_{\rm d}$, and the abundance ratios of $N_{\rm HNCO}/N_{\rm SiO}$ and $N_{\rm HNCO}/N_{\rm HC3N}$ show a decreasing trend towards the central dense regions of CMZ sources, while $N_{\rm HC3N}/N_{\rm SiO}$ moves into the opposite direction. Moreover, a better agreement is found between $T_{\rm d}$ and $N_{\rm HC3N}/N_{\rm SiO}$ in Bubble and NMSFR category sources. Both outflow and inflow activities have been found in eight of the sixteen bubble and NMSFR sources. The low outflow detection rate indicates that in these sources the SiO 2-1 line wing emission is either below our sensitivity limit or that the bulk of the SiO emission may be produced by the expansion of an H{\sc\,ii} region or supernova remnant, which has pushed molecular gas away forming a shock and yielding SiO.