2010
DOI: 10.1088/0004-637x/711/1/50
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Black Hole Spin and the Radio Loud/Quiet Dichotomy of Active Galactic Nuclei

Abstract: Radio loud active galactic nuclei (AGN) are on average 1000 times brighter in the radio band compared to radio quiet AGN. We investigate whether this radio loud/quiet dichotomy can be due to differences in the spin of the central black holes that power the radio-emitting jets. Using general relativistic magnetohydrodynamic simulations, we construct steady state axisymmetric numerical models for a wide range of black hole spins (dimensionless spin parameter 0.1 ≤ a ≤ 0.9999) and a variety of jet geometries. We … Show more

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Cited by 480 publications
(621 citation statements)
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References 62 publications
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“…This is consistent with state of the art numerical simulations which show the jet base starts magnetically dominated and accelerates in the parabolic region reaching a terminal bulk Lorentz factor at equipartition after which the jet becomes ballistic and conical [2], [3], [4] and [5]. Here we use an emission model with a magnetically dominated, accelerating, parabolic base transitioning at equipartition to a slowly decelerating, conical jet to test this emerging picture of jets and to try to determine their properties.…”
Section: Introductionsupporting
confidence: 88%
“…This is consistent with state of the art numerical simulations which show the jet base starts magnetically dominated and accelerates in the parabolic region reaching a terminal bulk Lorentz factor at equipartition after which the jet becomes ballistic and conical [2], [3], [4] and [5]. Here we use an emission model with a magnetically dominated, accelerating, parabolic base transitioning at equipartition to a slowly decelerating, conical jet to test this emerging picture of jets and to try to determine their properties.…”
Section: Introductionsupporting
confidence: 88%
“…These then affect the peak luminosity, since the total radiated energy E ∝ M cl is the same for a given clump mass. More specifically, we find that the peak luminosity of the flares scales with their initial position as (roughly) R −1.4 in , the peak time scales as 3 Apart, possibly, from the very early phases associated to the prompt emission (Tchekhovskoy, Narayan & McKinney 2010).…”
Section: Early Flares: Prompt Viscous Spreadingmentioning
confidence: 69%
“…One of the most appealing scenarios to explain the formation of steady jets is the Blandford-Znajek mechanism (Blandford & Znajek 1977), in which magnetic fields threading the BH event horizon are twisted and can extract the rotational energy of the spinning BH, producing an electromagnetic jet. Numerical simulations show that the mechanism can be very efficient and depends strongly on the BH spin (McKinney 2005;Tchekhovskoy et al 2010Tchekhovskoy et al , 2011. At the moment it is not clear if the Blandford-Znajek mechanism can be responsible for the production of steady jets, and in the literature there are some controversial results.…”
Section: Jet Powermentioning
confidence: 99%