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Excitation Mechanisms for HCN (1-0) and HCO+ (1-0) in Galaxies from the Great Observatories All-sky LIRG Survey

机译:大天文台全天候LIRG测量中星系中HCN(1-0)和HCO +(1-0)的激发机制

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摘要

We present new Institut de Radioastronomie Millimétrique (IRAM) 30 m spectroscopic observations of the ~88 GHz band, including emission from the CCH (N = 1 → 0) multiplet, HCN (J = 1 → 0), HCO^+ (J = 1 → 0), and HNC(J = 1 → 0), for a sample of 58 local luminous and ultraluminous infrared galaxies from the Great Observatories All-sky LIRG Survey (GOALS). By combining our new IRAM data with literature data and Spitzer/IRS spectroscopy, we study the correspondence between these putative tracers of dense gas and the relative contribution of active galactic nuclei (AGNs) and star formation to the mid-infrared luminosity of each system. We find the HCN (1–0) emission to be enhanced in AGN-dominated systems (〈L'_(HCN(1-0))/L'_(HCN(1-0)^+(1-0)〉 =1.84), compared to composite and starburst-dominated systems 〈L'_(HCN(1-0))/L'_(HCN(1-0)^+(1-0)〉 = 1.14, and 0.88, respectively). However, some composite and starburst systems have 〈L'_(HCN(1-0))/L'_(HCN(1-0)^+(1-0)〉 ratios comparable to those of AGNs, indicating that enhanced HCN emission is not uniquely associated with energetically dominant AGNs. After removing AGN-dominated systems from the sample, we find a linear relationship (within the uncertainties) between log10 〈L'_(HCN(1-0))/L'_(HCN(1-0)^+(1-0)〉 and log10(L_(IR)), consistent with most previous findings. L'_(HCN(1-0))/L_(IR), typically interpreted as the dense-gas depletion time, appears to have no systematic trend with LIR for our sample of luminous and ultraluminous infrared galaxies, and has significant scatter. The galaxy-integrated L'_(HCN(1-0)) and L'_(HCN^+(1-0)) emission do not appear to have a simple interpretation in terms of the AGN dominance or the star formation rate, and are likely determined by multiple processes, including density and radiative effects.
机译:我们提出了〜88 GHz频带的新的天文学放射力学研究所(IRAM)30 m光谱学观察结果,包括CCH(N = 1→0)多重峰,HCN(J = 1→0),HCO ^ +(J = 1→0)和HNC(J = 1→0),这是来自大天文台全天空LIRG调查(GOALS)的58个局部发光和超发光红外星系的样本。通过将我们新的IRAM数据与文献数据和Spitzer / IRS光谱相结合,我们研究了这些推测的致密气体示踪剂与活性银河原子核(AGN)和恒星形成对每个系统的中红外光度的相对贡献之间的对应关系。我们发现在AGN主导的系统(〈L'_(HCN(1-0))/ L'_(HCN(1-0)^ +(1-0)〉中,HCN(1–0)发射得到增强= 1.84),而复合材料和以星爆为主的系统〈L'_(HCN(1-0))/ L'_(HCN(1-0)^ +(1-0)〉分别为1.14和0.88 )。但是,某些复合星爆系统的〈L'_(HCN(1-0))/ L'_(HCN(1-0)^ +(1-0)〉比值与AGN相当,表明增强的HCN排放并非与能量占优势的AGN唯一相关,从样品中去除AGN主导的系统后,我们发现log10 〈L'_(HCN(1-0))/ L'_之间存在线性关系(在不确定性内) (HCN(1-0)^ +(1-0)〉和log10(L_(IR)),与大多数以前的发现一致。L'_(HCN(1-0))/ L_(IR)通常解释为LIR_(HCN(1-0))和L'_(银河系积分)的密集气体耗竭时间,对于我们的发光和超发光红外星系样本,使用LIR似乎没有系统趋势,并且散射明显。 HCN ^ +(1-0))发射似乎没有简单的相互作用就AGN优势或恒星形成率而言,它们可能是由多种过程决定的,包括密度和辐射效应。

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