Cosmological Evolution of Quasars

preprint1996arXivOpen access

Abstract

We present a model for the cosmological evolution of quasars (QSOs) under the assumption that they are powered by massive accreting black holes. Accretion flows around massive black holes make a transition from high radiative efficiency (∼10\sim 10%) to low efficiency, advection-dominated flows when M˙/M˙Edd{\dot M}/{\dot M}_{Edd} falls below the critical rate ∼0.3α2∼10−2\sim 0.3α^2\sim 10^{-2} where M˙{\dot M} is the mass accretion rate, M˙Edd∝M{\dot M}_{Edd}\propto M is the usual Eddington rate with the nominal 10% efficiency, and α(≤1)α(\le 1) is the dimensionless viscosity parameter. We identify this transition with the observed break at a redshift ∼2\sim 2 in the QSOs' X-ray luminosity evolution. Growth of black holes through accretion could naturally lead to such a transition at a critical redshift zc∼1−3z_c\sim 1-3, provided that most of high redshift QSOs appear with near Eddington luminosities at z∼3−4z\sim 3-4 and the accretion rates decline over the Hubble time in a roughly synchronous manner. Before the transition, the QSOs' luminosities (with a high efficiency) slowly decrease and after the transition at zcz_c, the QSO luminosities evolve approximately as ∝(1+z)K(z)\propto (1+z)^{K(z)} where K(z)K(z) gradually varies from z=zcz=z_c to z∼0z\sim 0 around K∼3K\sim3. The results depend on the details of the QSO X-ray emission mechanism. We discuss some further implications.

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