Supermassive black holes in the early Universe

The recent discovery of the ultraluminous quasar SDSS J010013.02+280225.8 at redshift 6.3 has exacerbated the time compression problem implied by the appearance of supermassive black holes only $\sim 900$ Myr after the big bang, and only $\sim 500$ Myr beyond the formation of Pop II and III star...

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Main Authors: Melia, F., McClintock, T. M.
Other Authors: The University of Arizona
Language:en
Published: The Royal Society 2015
Online Access:http://hdl.handle.net/10150/614765
http://arizona.openrepository.com/arizona/handle/10150/614765
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spelling ndltd-arizona.edu-oai-arizona.openrepository.com-10150-6147652016-06-26T03:01:59Z Supermassive black holes in the early Universe Melia, F. McClintock, T. M. The University of Arizona The recent discovery of the ultraluminous quasar SDSS J010013.02+280225.8 at redshift 6.3 has exacerbated the time compression problem implied by the appearance of supermassive black holes only $\sim 900$ Myr after the big bang, and only $\sim 500$ Myr beyond the formation of Pop II and III stars. Aside from heralding the onset of cosmic reionization, these first and second generation stars could have reasonably produced the $\sim 5-20\;M_\odot$ seeds that eventually grew into $z\sim 6-7$ quasars. But this process would have taken $\sim 900$ Myr, a timeline that appears to be at odds with the predictions of $\Lambda$CDM without an anomalously high accretion rate, or some exotic creation of $\sim 10^5\;M_\odot$ seeds. There is no evidence of either of these happening in the local universe. In this paper, we show that a much simpler, more elegant solution to the supermassive black hole anomaly is instead to view this process using the age-redshift relation predicted by the $R_{\rm h}=ct$ Universe, an FRW cosmology with zero active mass. In this context, cosmic reionization lasted from $t\sim 883$ Myr to $\sim 2$ Gyr ($6\lesssim z\lesssim 15$), so $\sim 5-20\;M_\odot$ black hole seeds formed shortly after reionization had begun, would have evolved into $\sim 10^{10}\; M_\odot$ quasars by $z\sim 6-7$ simply via the standard Eddington-limited accretion rate. The consistency of these observations with the age-redshift relationship predicted by $R_{\rm h}=ct$ supports the existence of dark energy; but not in the form of a cosmological constant. 2015-12-16 Article Supermassive black holes in the early Universe 2015, 471 (2184):20150449 Proceedings of the Royal Society A: Mathematical, Physical and Engineering Science 1364-5021 1471-2946 10.1098/rspa.2015.0449 http://hdl.handle.net/10150/614765 http://arizona.openrepository.com/arizona/handle/10150/614765 Proceedings of the Royal Society A: Mathematical, Physical and Engineering Science en http://rspa.royalsocietypublishing.org/lookup/doi/10.1098/rspa.2015.0449 © The Authors. Published by the Royal Society under the terms of the Creative Commons Attribution License http://creativecommo ns.org/licenses/ by/4.0/, which permits unrestricted use, provided the origin al author and source are credited The Royal Society
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language en
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description The recent discovery of the ultraluminous quasar SDSS J010013.02+280225.8 at redshift 6.3 has exacerbated the time compression problem implied by the appearance of supermassive black holes only $\sim 900$ Myr after the big bang, and only $\sim 500$ Myr beyond the formation of Pop II and III stars. Aside from heralding the onset of cosmic reionization, these first and second generation stars could have reasonably produced the $\sim 5-20\;M_\odot$ seeds that eventually grew into $z\sim 6-7$ quasars. But this process would have taken $\sim 900$ Myr, a timeline that appears to be at odds with the predictions of $\Lambda$CDM without an anomalously high accretion rate, or some exotic creation of $\sim 10^5\;M_\odot$ seeds. There is no evidence of either of these happening in the local universe. In this paper, we show that a much simpler, more elegant solution to the supermassive black hole anomaly is instead to view this process using the age-redshift relation predicted by the $R_{\rm h}=ct$ Universe, an FRW cosmology with zero active mass. In this context, cosmic reionization lasted from $t\sim 883$ Myr to $\sim 2$ Gyr ($6\lesssim z\lesssim 15$), so $\sim 5-20\;M_\odot$ black hole seeds formed shortly after reionization had begun, would have evolved into $\sim 10^{10}\; M_\odot$ quasars by $z\sim 6-7$ simply via the standard Eddington-limited accretion rate. The consistency of these observations with the age-redshift relationship predicted by $R_{\rm h}=ct$ supports the existence of dark energy; but not in the form of a cosmological constant.
author2 The University of Arizona
author_facet The University of Arizona
Melia, F.
McClintock, T. M.
author Melia, F.
McClintock, T. M.
spellingShingle Melia, F.
McClintock, T. M.
Supermassive black holes in the early Universe
author_sort Melia, F.
title Supermassive black holes in the early Universe
title_short Supermassive black holes in the early Universe
title_full Supermassive black holes in the early Universe
title_fullStr Supermassive black holes in the early Universe
title_full_unstemmed Supermassive black holes in the early Universe
title_sort supermassive black holes in the early universe
publisher The Royal Society
publishDate 2015
url http://hdl.handle.net/10150/614765
http://arizona.openrepository.com/arizona/handle/10150/614765
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