来自斯隆数字巡天的类星体的射电光度、黑洞质量和爱丁顿比

W. Bian, Yan-Mei Chen, Chen Hu, Kai Huang, Yan Xu
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引用次数: 6

摘要

我们研究了斯隆数字巡天(SDSS)数据发布3中红移z < 0.83的射电声类星体的M-BH-sigma*关系。该样本由3772个具有较好的H β和[O III]谱线模型和可用射电光度的类星体组成,其中306个类星体为射电高声类星体,3466个类星体具有测量到的射电光度或射电光度上限(181个类星体具有测量到的射电光度)。维里超大质量黑洞的质量(M-BH)是由宽的H β线计算出来的,而宿主恒星的速度色散(sigma*)是由核心[O III]的气体速度色散来追踪的。射电亮度和响度来自FIRST星表。研究结果如下:(1)对于射电安静类星体,我们证实当考虑到M-BH的不确定性和光度偏差时,它们与非活动星系定义的M-BH-sigma*关系没有明显的偏差。(2)我们发现射电大声类星体比射电安静类星体更偏离M-BH-sigma*关系。这种偏差只是部分地由于M-BH-sigma*关系的可能的宇宙学演化和光度偏差。(3)射电亮度与M-BH(1.28-0.16+ 0.023)(L-Bol/L-Edd)(1.29-0.24+0.31)和M-BH(3.10-0.70+0.60) (L-Bol/L-Edd)(4.18-1.10+1.40)成正比。射电亮度对类星体质量和爱丁顿比值的依赖性较弱,这表明其他物理效应可以解释它们的射电亮度,比如黑洞的自旋。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Radio Luminosity, Black Hole Mass and Eddington Ratio for Quasars from the Sloan Digital Sky Survey
We investigate the M-BH-sigma* relation for radio-loud quasars with redshift z < 0.83 in Data Release 3 of the Sloan Digital Sky Survey (SDSS). The sample consists of 3772 quasars with better models of the H beta and [O III] lines and available radio luminosity, including 306 radio-loud quasars, 3466 radio-quiet quasars with measured radio luminosity or upper-limit of radio luminosity (181 radio-quiet quasars with measured radio luminosity). The virial supermassive black hole mass (M-BH) is calculated from the broad H beta line, and the host stellar velocity dispersion (sigma*) is traced by the core [O III] gaseous velocity dispersion. The radio luminosity and radio loudness are derived from the FIRST catalog. Our results are as follows: (1) For radio-quiet quasars, we confirm that there is no obvious deviation from the M-BH-sigma* relation defined for inactive galaxies when the uncertainties in M-BH and the luminosity bias are concerned. (2) We find that the radio-loud quasars deviate more from the M-BH-sigma* relation than do the radio-quiet quasars. This deviation is only partly due to a possible cosmological evolution of the M-BH-sigma* relation and the luminosity bias. (3) The radio luminosity is proportional to M-BH(1.28-0.16+.023) (L-Bol/L-Edd)(1.29-0.24+0.31) for radio-quiet quasars and to M-BH(3.10-0.70+0.60) (L-Bol/L-Edd)(4.18-1.10+1.40) for radio-loud quasars. The weaker dependence of the radio luminosity on the mass and the Eddington ratio for radio-loud quasars shows that other physical effects would account for their radio luminosities, such as the spin of the black hole.
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