Chandra observations of the galaxy group AWM 5: cool core re-heating and thermal conduction suppression

preprint2008arXivOpen access

Abstract

We present an analysis of a 40 ksec Chandra observation of the galaxy group AWM 5. It has a small (∼8\sim8 kpc) dense cool core with a temperature of ∼1.2\sim1.2 keV and the temperature profile decreases at larger radii, from ∼3.5\sim3.5 keV just outside the core to ∼2\sim2 keV at ∼300\sim300 kpc from the center. The abundance distribution shows a "hole" in the central ∼10\sim10 kpc, where the temperature declines sharply. An abundance of at least a few times solar is observed ∼15−20\sim15-20 kpc from the center. The deprojected electron density profile shows a break in slope at ∼13\sim13 kpc and can be fit by two ββ-models, with β=0.72−0.11+0.16β=0.72_{-0.11}^{+0.16} and rc=5.7−1.5+1.8r_c=5.7_{-1.5}^{+1.8} kpc, for the inner part, and β=0.34±0.01β=0.34\pm0.01 and rc=31.3−5.5+5.8r_c=31.3_{-5.5}^{+5.8} kpc, for the outer part. The mass fraction of hot gas is fairly flat in the center and increases for r>30r>30 kpc up to a maximum of ∼6.5\sim6.5% at r∼380r\sim380 kpc. The gas cooling time within the central 30 kpc is smaller than a Hubble time, although the temperature only declines in the central ∼8\sim8 kpc region. This discrepancy suggests that an existing cooling core has been partially re-heated. In particular, thermal conduction could have been a significant source of re-heating. In order for heating due to conduction to balance cooling due to emission of X-rays, the conductivity must be suppressed by a large factor (at least ∼100\sim100). Past AGN activity (still visible as a radio source in the center of the group) is however the most likely source that re-heated the central regions of AWM 5.

Explore this paper’s authors, topics and related work.

Building this map preview

BZPEER is loading the nearby papers, people, topics and institutions for this page.

Reviews 0

Write a reviewWrite

No reviews yet.

Discussion 0

Add a commentWrite

No comments yet.