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Star Formation Rates from C II 158 μm and Mid-infrared Emission Lines for Starbursts and Active Galactic Nuclei

机译:C II158μm的恒星形成速率和星爆和活动星系核的中红外发射线

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摘要

A summary is presented for 130 galaxies observed with the Herschel Photodetector Array Camera and Spectrometer instrument to measure fluxes for the [C II] 158 μm emission line. Sources cover a wide range of active galactic nucleus to starburst classifications, as derived from polycyclic aromatic hydrocarbon strength measured with the Spitzer Infrared Spectrograph. Redshifts from [C II] and line to continuum strengths (equivalent width (EW) of [C II]) are given for the full sample, which includes 18 new [C II] flux measures. Calibration of L([C II)]) as a star formation rate (SFR) indicator is determined by comparing [C II] luminosities with mid-infrared [Ne II] and [Ne III] emission line luminosities; this gives the same result as determining SFR using bolometric luminosities of reradiating dust from starbursts: log SFR = log L([C II)]) - 7.0, for SFR in M yr and L([C II]) in L . We conclude that L([C II]) can be used to measure SFR in any source to a precision of ~50%, even if total source luminosities are dominated by an active galactic nucleus (AGN) component. The line to continuum ratio at 158 μm, EW([C II]), is not significantly greater for starbursts (median EW([C II]) = 1.0 μm) compared to composites and AGNs (median EW([C II]) = 0.7 μm), showing that the far-infrared continuum at 158 μm scales with [C II] regardless of classification. This indicates that the continuum at 158 μm also arises primarily from the starburst component within any source, giving log SFR = log νL (158 μm) - 42.8 for SFR in M yr-1 and νL (158 μm) in erg s.
机译:总结介绍了用Herschel光​​电探测器阵列照相机和光谱仪仪器观测到的130个星系,以测量[C II] 158μm发射线的通量。根据Spitzer红外光谱仪测得的多环芳烃强度,其来源涵盖了从星系到星暴的各种活动星系核。从[C II]和线到连续强度([C II]的等效宽度(EW))的红移针对整个样本给出,其中包括18个新的[C II]磁通量度。通过比较[C II]光度与中红外[Ne II]和[Ne III]发射线的光度,确定作为星形成率(SFR)指标的L([C II)])的校准;这给出了与使用爆炸性辐射的辐射强度的辐射强度测定SFR相同的结果:log SFR = log L([C II)])-7.0,Myr中的SFR和L中的L([C II])。我们得出的结论是,即使总光源的光度由活跃的银河原子核(AGN)成分控制,L([C II])也可用于测量任何光源中的SFR,精确度约为50%。与合成材料和AGN(中位数EW([C II])相比,星爆(中位数EW([C II])= 1.0μm)在158μm处的线与连续体比率EW([C II])并不明显更大。 = 0.7μm),表明158μm的远红外连续谱标有[C II],与分类无关。这表明在158μm处的连续谱也主要来自于任何来源中的星爆成分,给出了Myr-1中SFR的log SFR = logνL(158μm)-42.8和erg s中νL(158μm)。

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