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arXiv 0705.3377astro-ph
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中红外恒星形成率指示器的定标

The Calibration of Mid-Infrared Star Formation Rate Indicators

D. Calzetti, R. C. Kennicutt, C. W. Engelbracht, C. Leitherer, B. T. Draine, L. Kewley, J. Moustakas, M. Sosey, D. A. Dale, K. D. Gordon, G. X. Helou, D. J. Hol… 展开作者

D. Calzetti, R. C. Kennicutt, C. W. Engelbracht, C. Leitherer, B. T. Draine, L. Kewley, J. Moustakas, M. Sosey, D. A. Dale, K. D. Gordon, G. X. Helou, D. J. Hollenbach, L. Armus, G. Bendo, C. Bot, B. Buckalew, T. Jarrett, A. Li, M. Meyer, E. J. Murphy, M. Prescott, M. W. Regan, G. H. Rieke, H. Roussel, K. Sheth, J. D. T. Smith, M. D. Thornley, F. Walter

摘要:

为了研究中红外辐射对恒星形成率的影响程度,我们分析了斯皮策8 μ m和24 μ m的恒星形成区数据,这些数据来自于附近33个星系的Paschen-alpha(1.8756 μ m)辐射线上的HST/NICMOS图像。这些星系是从斯皮策红外邻近星系巡天(SINGS)样本中提取的,涵盖了一系列的形态和氧丰度的10倍。已发表的数据,本地低金属丰度星暴星系和发光红外星系也包括在分析中。减去恒星连续谱的8 μ m发射和24 μ m发射都与修正后的Pa-α线发射相关,尽管两者的关系都不是线性的。简单的模型的恒星星族和尘埃消光和排放能够再现观察到的非线性趋势的24微米的排放与电离光子的数量,包括适度的不足,24微米的排放在低金属含量的地区,这是由于在低光度的尘埃不透明度和尘埃温度降低相结合。相反,8 μ m的发射作为电离光子数的函数的趋势不能很好地再现相同的模型。8 μ m的发射贡献,在更大的措施比24 μ m的发射,由尘埃加热的非电离恒星星族,与以前的研究结果一致。两个SFR校准,一个使用24 μ m发射,另一个使用24 μ m和H-α光度的组合(Kennicutt等人,2007年),提出。没有校准8微米的发射,因为它的显着依赖于金属丰度和环境。这里提出的校准应直接适用于正在进行的恒星形成占主导地位的系统。

英文摘要:

With the goal of investigating the degree to which the mid-infrared emission traces the star formation rate (SFR), we analyze Spitzer 8 um and 24 um data of star-forming regions in a sample of 33 nearby galaxies with available HST/NICMOS images in the Paschen-alpha (1.8756 um) emission line. The galaxies are drawn from the Spitzer Infrared Nearby Galaxies Survey (SINGS) sample, and cover a range of morphologies and a factor ~10 in oxygen abundance. Published data on local low-metallicity starburst galaxies and Luminous Infrared Galaxies are also included in the analysis. Both the stellar-continuum-subtracted 8 um emission and the 24 um emission correlate with the extinction-corrected Pa-alpha line emission, although neither relationship is linear. Simple models of stellar populations and dust extinction and emission are able to reproduce the observed non-linear trend of the 24 um emission versus number of ionizing photons, including the modest deficiency of 24 um emission in the low metallicity regions, which results from a combination of decreasing dust opacity and dust temperature at low luminosities. Conversely, the trend of the 8 um emission as a function of the number of ionizing photons is not well reproduced by the same models. The 8 um emission is contributed, in larger measure than the 24 um emission, by dust heated by non-ionizing stellar populations, in agreement with previous findings. Two SFR calibrations, one using the 24 um emission and the other using a combination of the 24 um and H-alpha luminosities (Kennicutt et al. 2007), are presented. No calibration is presented for the 8 um emission, because of its significant dependence on both metallicity and environment. The calibrations presented here should be directly applicable to systems dominated by on-going star formation.

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