On the Jet Production Efficiency in a Sample of the Youngest Radio Galaxies

TL;DR

This study investigates jet production efficiency in 17 young radio galaxies, revealing how it correlates with accretion rates and spectral states, and finding efficiencies below theoretical maximums with state-dependent variations.

Contribution

It provides the first detailed analysis of jet efficiency in young radio galaxies, linking accretion properties and spectral states to jet power and efficiency.

Findings

Jet power correlates with accretion rate up to a saturation point.

Jet efficiency varies from below 0.001 to about 0.2.

Jets are most efficient during high/hard spectral states.

Abstract

Here we discuss the jet production efficiency in a sample of 17 young radio galaxies with measured redshifts, kinematic ages, and nuclear X-ray fluxes, for which the observed luminosities of compact jets/lobes and accretion disks correspond to the same episode of the AGN activity. For the targets, we analyze the available optical data, estimating the bolometric luminosities of the accretion disks $L_{\rm bol}$, and the black hole masses; we also derive the minimum jet kinetic luminosities, $P_{\rm j}$. With such, we investigate the distribution of our sample in the three-dimensional space of the accretion rate $\lambda_{\rm Edd} \equiv L_{\rm bol}/L_{\rm Edd}$, the nuclear X-ray luminosity $L_{\rm X}$ considered here as a limit for the emission of the disk coronae, and $P_{\rm j}$, expressing the latter two parameters either in the Eddington units, or in the units of the disk luminosity. We find that (i) the accretion rate $\lambda_{\rm Edd}$ in our sample is distributed within a narrow range $\lambda_{\rm Edd} \sim 0.01 - 0.2$; (ii) the normalized jet power $P_{\rm j}/L_{\rm Edd}$ formally correlates with the accretion rate $\lambda_{\rm Edd}$, with some saturation at the largest values $\lambda_{\rm Edd}> 0.05$; (iii) the jet production efficiency $\eta_{\rm jet} \equiv P_{\rm j}/\dot{M}_{\rm acc} c^2$ spans a range from $\eta_{\rm jet} \lesssim 10^{-3}$ up to $\sim 0.2$ at maximum, which is below the level expected for magnetically arrested disks around maximally spinning black holes; and (iv) there is a diversification in $\eta_{\rm jet}$ on the hardness--intensity diagram $L_{\rm X}/L_{\rm bol} - \lambda_{\rm Edd}$, with the jets being produced most efficiently during the high/hard states, and suppressed during the soft states.