State-of-the-art energetic and morphological modelling of the launching site of the M87 jet

TL;DR

This paper combines advanced simulations and radiative transfer calculations to model the M87 jet's origin, constraining the black hole's spin and jet properties through broadband spectrum and collimation profile analysis.

Contribution

It introduces a comprehensive modeling approach that integrates general-relativistic magnetohydrodynamics and radiative transfer to study the M87 jet and estimate the black hole's spin.

Findings

Constraints on M87* spin: 0.5 to 1.0, possibly higher.

Reproduction of broadband spectrum from radio to near-infrared.

Match of observed jet collimation profile.

Abstract

M87 has been the target of numerous astronomical observations across the electromagnetic spectrum and Very Long Baseline Interferometry (VLBI) resolved an edge-brightened jet. However, the origin and formation of its jets remain unclear. In our current understand black holes (BH) are the driving engine of jet formation, and indeed the recent Event Horizon Telescope (EHT) observations revealed a ring-like structure in agreement with theoretical models of accretion onto a rotating Kerr BH. In addition to the spin of the BH being a potential source of energy for the launching mechanism, magnetic fields are believed to play a key role in the formation of relativistic jets. A priori, the spin, $a_\star$, of BH in M87* is unknown, however, when accounting for the estimates on the X-ray luminosity and jet power, values $\left |a_\star \right| \gtrsim 0.5$ appear favoured. Besides the properties of the accretion flow and the BH spin, the radiation microphysics including the particle distribution (thermal and non-thermal) as well as the particle acceleration mechanism play a crucial role. We show that general-relativistic magnetohydrodynamics simulations and general-relativistic radiative transfer calculations can reproduce the broadband spectrum from the radio to the near-infrared regime and simultaneously match the observed collimation profile of M87, thus allowing us to set rough constraints on the dimensionless spin of M87* to be $0.5\lesssim a_{\star}\lesssim 1.0$, with higher spins being possibly favoured.