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Cosmological Evolution of Quasars
Author(s) -
Insu Yi
Publication year - 1996
Publication title -
the astrophysical journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.376
H-Index - 489
eISSN - 1538-4357
pISSN - 0004-637X
DOI - 10.1086/178178
Subject(s) - physics , qsos , astrophysics , quasar , accretion (finance) , redshift , dimensionless quantity , eddington luminosity , active galactic nucleus , galaxy , quantum mechanics
We present a model for the cosmological evolution of quasars (QSOs) under theassumption that they are powered by massive accreting black holes. Accretionflows around massive black holes make a transition from high radiativeefficiency ($\sim 10%$) to low efficiency, advection-dominated flows when${\dot M}/{\dot M}_{Edd}$ falls below the critical rate $\sim 0.3\alpha^2\sim10^{-2}$ where ${\dot M}$ is the mass accretion rate, ${\dot M}_{Edd}\propto M$is the usual Eddington rate with the nominal 10% efficiency, and $\alpha (\le1)$ is the dimensionless viscosity parameter. We identify this transition withthe observed break at a redshift $\sim 2$ in the QSOs' X-ray luminosityevolution. Growth of black holes through accretion could naturally lead to sucha transition at a critical redshift $z_c\sim 1-3$, provided that most of highredshift QSOs appear with near Eddington luminosities at $z\sim 3-4$ and theaccretion rates decline over the Hubble time in a roughly synchronous manner.Before the transition, the QSOs' luminosities (with a high efficiency) slowlydecrease and after the transition at $z_c$, the QSO luminosities evolveapproximately as $\propto (1+z)^{K(z)}$ where $K(z)$ gradually varies from$z=z_c$ to $z\sim 0$ around $K\sim3$. The results depend on the details of theQSO X-ray emission mechanism. We discuss some further implications.Comment: Latex, 2 PS figures, To Appear in Ap

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