# The imprints of AGN feedback within a supermassive black hole's sphere of influence

## TL;DR

This study uses deep Chandra X-ray observations of M87 to analyze the hot gas properties near its supermassive black hole, revealing multiphase gas, steep density gradients, and evidence for cooling flows that may feed the central cold gas disk.

## Contribution

It provides detailed measurements of hot gas structure and cooling flows within the black hole's sphere of influence, challenging the Bondi accretion model in M87.

## Key findings

- Hot gas is multiphase with temperatures from 0.2 to 1 keV.
- Density gradients vary with direction, indicating inflows and outflows.
- Cooling gas at ~100 pc may form a mini cooling flow.

## Abstract

We present a new 300 ks Chandra observation of M87 that limits pileup to only a few per cent of photon events and maps the hot gas properties closer to the nucleus than has previously been possible. Within the supermassive black hole's gravitational sphere of influence, the hot gas is multiphase and spans temperatures from 0.2 to 1 keV. The radiative cooling time of the lowest temperature gas drops to only 0.1-0.5 Myr, which is comparable to its free fall time. Whilst the temperature structure is remarkably symmetric about the nucleus, the density gradient is steep in sectors to the N and S, with $\rho{\propto}r^{-1.5\pm0.1}$, and significantly shallower along the jet axis to the E, where $\rho{\propto}r^{-0.93\pm0.07}$. The density structure within the Bondi radius is therefore consistent with steady inflows perpendicular to the jet axis and an outflow directed E along the jet axis. By putting limits on the radial flow speed, we rule out Bondi accretion on the scale resolved at the Bondi radius. We show that deprojected spectra extracted within the Bondi radius can be equivalently fit with only a single cooling flow model, where gas cools from 1.5 keV down below 0.1 keV at a rate of 0.03 M$_{\odot}$/yr. For the alternative multi-temperature spectral fits, the emission measures for each temperature component are also consistent with a cooling flow model. The lowest temperature and most rapidly cooling gas in M87 is therefore located at the smallest radii at ~100 pc and may form a mini cooling flow. If this cooling gas has some angular momentum, it will feed into the cold gas disk around the nucleus, which has a radius of ~80 pc and therefore lies just inside the observed transition in the hot gas structure.