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The dense gas in the largest molecular complexes of the antennae: HCN and HCO+ observations of NGC 4038/39 using ALMA

机译:天线最大分子复合物中的致密气体:HCN和HCO +使用aLma观测NGC 4038/39

摘要

We present observations of the dense molecular gas tracers $mathrm{HCN}$, $mathrm{HNC}$, and ${mathrm{HCO}}^{+}$ in the $J=1-0$ transition using the Atacama Large Millimeter/submillimeter Array. We supplement our data sets with previous observations of $mathrm{CO}$ $J=1-0$, which trace the total molecular gas content. We separate the Antennae into seven bright regions in which we detect emission from all three molecules, including the nuclei of NGC 4038 and NGC 4039, five super giant molecular complexes in the overlap region, and two additional bright clouds. We find that the ratio of ${L}_{mathrm{HCN}}/{L}_{mathrm{CO}}$, which traces the dense molecular gas fraction, is greater in the two nuclei (${L}_{mathrm{HCN}}/{L}_{mathrm{CO}}$ $sim quad 0.07-0.08$) than in the overlap region (${L}_{mathrm{HCN}}/{L}_{mathrm{CO}}$ $lt 0.05$). We attribute this to an increase in pressure due to the stellar potential within the nuclei; a similar effect to what has been seen previously in the Milky Way and nearby spiral galaxies. Furthermore, the ratio of ${L}_{mathrm{HNC}}/{L}_{mathrm{HCN}}$ $sim quad 0.3-0.4$ does not vary by more than a factor of 1.5 between regions. By comparing our measured ratios to photon dominated region (PDR) models including mechanical heating, we find that the ratio of ${L}_{mathrm{HNC}}/{L}_{mathrm{HCN}}$ is consistent with mechanical heating contributing gsim5%–10% of the PDR surface heating to the total heating budget. Finally, the ratio of ${L}_{mathrm{HCN}}/{L}_{mathrm{HCO}+}$ varies from ~1 in the nucleus of NGC 4038 down to ~0.5 in the overlap region. The lower ratio in the overlap region may be due to an increase in the cosmic ray rate from the increased supernova rate within this region.
机译:我们使用以下方法在$ J = 1-0 $过渡中提供了对密集分子气体示踪剂$ mathrm {HCN} $,$ mathrm {HNC} $和$ { mathrm {HCO}} ^ {+} $的观测Atacama大毫米/亚毫米阵列。我们用先前的观测值 mathrm {CO} $ $ J = 1-0 $补充了数据集,这些观测值跟踪了总分子气体含量。我们将天线分成七个明亮的区域,在其中我们检测到所有三个分子的发射,包括NGC 4038和NGC 4039的原子核,重叠区域中的五个超大分子复合物以及另外两个明亮的云。我们发现,跟踪两个分子核中的致密分子气体分数的$ {L} _ { mathrm {HCN}} / {L} _ { mathrm {CO}} $之比在两个原子核中更大($ {L } _ { mathrm {HCN}} / {L} _ { mathrm {CO}} $ $ sim quad 0.07-0.08 $)比重叠区域($ {L} _ { mathrm {HCN}} / {L} _ { mathrm {CO}} $ $ lt 0.05 $)。我们将其归因于由于核内恒星电位而导致的压力增加。与先前在银河系和附近的旋涡星系中所见相似。此外,$ {L} _ { mathrm {HNC}} / {L} _ { mathrm {HCN}} $ $ sim quad 0.3-0.4 $的比率之间相差不超过1.5地区。通过将我们测量的比率与包括机械加热的光子主导区域(PDR)模型进行比较,我们发现$ {L} _ { mathrm {HNC}} / {L} _ { mathrm {HCN}} $的比率是一致的机械加热在总加热预算中占PDR表面加热的gsim5%至10%。最后,$ {L} _ { mathrm {HCN}} / {L} _ { mathrm {HCO} +} $的比率从NGC 4038核中的〜1降至重叠区域中的〜0.5。重叠区域中较低的比率可能是由于该区域中超新星发生率增加引起的宇宙射线率增加。

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