4.7 Article

On the thermodynamic self-similarity of the nearest, most relaxed, giant ellipticals

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 425, Issue 4, Pages 2731-2740

Publisher

OXFORD UNIV PRESS
DOI: 10.1111/j.1365-2966.2012.21245.x

Keywords

galaxies: active; galaxies: ISM; X-rays: galaxies

Funding

  1. National Aeronautics and Space Administration [PF8-90056, PF9-00070, GO9-0088X, NAS8-03060]
  2. US Department of Energy [DE-AC02-76SF00515]

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We present detailed spatially resolved measurements of the thermodynamic properties of the X-ray-emitting gas in the inner regions of the five nearest, X-ray and optically brightest, and most X-ray morphologically relaxed giant elliptical galaxies known. Beyond the innermost region at r greater than or similar to 1 kpc, and out to r similar to 6 kpc, the density, pressure, entropy and cooling time distributions for the X-ray-emitting gas follow remarkably similar, simple, power-law-like distributions. Notably, the entropy profiles follow a form K proportional to r(alpha), with an index alpha = 0.92-1.07. The cumulative hot X-ray-emitting gas mass profiles and the gas mass to stellar light ratios of all five galaxies are also similar. Overall the observed similarity of the thermodynamic profiles in this radial range argues that, in these systems, relativistic jets heat the gas at a similar rate averaged over time-scales longer than the cooling time t(cool) greater than or similar to 10(8) yr. These jets are powered by accretion from the hot gas, or material entrained within it, on to the central supermassive black hole. This jet heating creates an energy balance where heating and cooling are in equilibrium, keeping the hot galactic atmospheres in a 'steady state'. Within r less than or similar to 1 kpc, this similarity breaks down: the observed entropy profiles show well-resolved flattening and the values differ from system to system substantially. The accretion rate on to the black hole and the active galactic nucleus activity, heating the interstellar medium, must therefore vary significantly on time-scales shorter than t(cool) = 10(7)-10(8) yr.

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