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首页> 外文期刊>The Astrophysical journal >DECOMPOSING STAR FORMATION AND ACTIVE GALACTIC NUCLEUS WITH SPITZER MID-INFRARED SPECTRA: LUMINOSITY FUNCTIONS AND CO-EVOLUTION
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DECOMPOSING STAR FORMATION AND ACTIVE GALACTIC NUCLEUS WITH SPITZER MID-INFRARED SPECTRA: LUMINOSITY FUNCTIONS AND CO-EVOLUTION

机译:借助斯皮茨中红外光谱分解恒星形成和活跃的银河系核:发光度函数和共同演化

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We present Spitzer 7-38 μm spectra for a 24 μm flux-limited sample of galaxies at z ~ 0.7 in the COSMOS field. The detailed high-quality spectra allow us to cleanly separate star formation (SF) and active galactic nucleus (AGN) in individual galaxies. We first decompose mid-infrared luminosity functions (LFs). We find that the SF 8 μm and 15 μm LFs are well described by Schechter functions. AGNs dominate the space density at high luminosities, which leads to the shallow bright-end slope of the overall mid-infrared LFs. The total infrared (8-1000 μm) LF from 70 μm selected galaxies shows a shallower bright-end slope than the bolometrically corrected SF 15 μm LF, owing to the intrinsic dispersion in the mid-to-far-infrared spectral energy distributions. We then study the contemporary growth of galaxies and their supermassive black holes (BHs). Seven of the thirty-one luminous infrared galaxies with Spitzer spectra host luminous AGNs, implying an AGN duty cycle of 23% ± 9%. The time-averaged ratio of BH accretion rate and SF rate matches the local M BH – M bulge relation and the M BH – M host relation at z ~ 1. These results favor co-evolution scenarios in which BH growth and intense SF happen in the same event but the former spans a shorter lifetime than the latter. Finally, we compare our mid-infrared spectroscopic selection with other AGN identification methods and discuss candidate Compton-thick AGNs in the sample. While only half of the mid-infrared spectroscopically selected AGNs are detected in X-ray, ~90% of them can be identified with their near-infrared spectral indices.
机译:对于COSMOS场中z〜0.7的24μm通量受限的星系样本,我们展示了Spitzer 7-38μm光谱。详细的高质量光谱使我们能够清晰地分离出各个星系中的恒星形成(SF)和活动银河核(AGN)。我们首先分解中红外发光度函数(LFs)。我们发现SF 8μm和15μmLFs由Schechter函数很好地描述了。在高亮度下,AGN在空间密度中占主导地位,这导致整个中红外LF的亮端斜率较小。来自70μm选定星系的总红外(8-1000μm)LF显示出比经辐射热校正的SF 15μmLF浅的亮端斜率,这归因于中远红外光谱能量分布的固有色散。然后,我们研究星系及其超质量黑洞(BHs)的当代增长。具有Spitzer光谱的31个发光红外星系中的七个拥有发光AGN,这意味着AGN占空比为23%±9%。 BH增生率和SF率的时间平均比率与z〜1处的局部M BH –M凸起关系和M BH –M宿主关系相匹配。这些结果有利于BH增长和强烈SF发生的共同演化场景。相同的事件,但前者的生存期比后者短。最后,我们将我们的中红外光谱选择与其他AGN识别方法进行了比较,并讨论了样品中康普顿厚的候选AGN。虽然只有一半的中红外光谱选择的AGN在X射线中被检测到,但它们中的约90%可以通过其近红外光谱指数来识别。

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