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Post Info TOPIC: 4C+29.30


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RE: 4C+29.30
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4C+29.30: Black Hole Powered Jets Plough Into Galaxy

4c2930_labeled_525.jpg

This multi-wavelength view shows 4C+29.30, a galaxy located some 850 million light years from Earth. The radio emission comes from two jets of particles that are speeding at millions of miles per hour away from a supermassive black hole at the center of the galaxy. The estimated mass of the black hole is about 100 million times the mass of our Sun. The ends of the jets show larger areas of radio emission located outside the galaxy.
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Title: Deep Chandra X-ray Imaging of a Nearby Radio Galaxy 4C+29.30: X-ray/Radio Connection
Authors: Aneta Siemiginowska (1), Lukasz Stawarz (2,3), Chi C. Cheung (4), Thomas L. Aldcroft (1), Jill Bechtold (5), D.J. Burke (1), Daniel Evans (1,6), Joanna Holt (7), Marek Jamrozy (3), Giulia Migliori (1). ((1) Harvard Smithsonian Center for Astrophysics, USA (2) ISAS/JAXA, Japan (3) Astronomical Observatory, Jagiellonian University, Poland (4) NRCR/NSF/NRL Washington, DC, USA (5) Steward Observatory, USA (6) Elon University, USA (7) Leiden Observatory, The Netherlands)

We report results from our deep Chandra X-ray observations of a nearby radio galaxy, 4C+29.30 (z=0.0647). The Chandra image resolves structures on sub-arcsec to arcsec scales, revealing complex X-ray morphology and detecting the main radio features: the nucleus, a jet, hotspots, and lobes. The nucleus is absorbed (N(H)=3.95 (+0.27/-0.33)x10^23 atoms/cm²) with an unabsorbed luminosity of L(2-10 keV) ~ (5.08 ±0.52) 10^43 erg/s characteristic of Type 2 AGN. Regions of soft (<2 keV) X-ray emission that trace the hot interstellar medium (ISM) are correlated with radio structures along the main radio axis indicating a strong relation between the two. The X-ray emission beyond the radio source correlates with the morphology of optical line-emitting regions. We measured the ISM temperature in several regions across the galaxy to be kT ~ 0.5 with slightly higher temperatures (of a few keV) in the center and in the vicinity of the radio hotspots. Assuming these regions were heated by weak shocks driven by the expanding radio source, we estimated the corresponding Mach number of 1.6 in the southern regions. The thermal pressure of the X-ray emitting gas in the outermost regions suggest the hot ISM is slightly under-pressured with respect to the cold optical-line emitting gas and radio-emitting plasma, which both seem to be in a rough pressure equilibrium. We conclude that 4C+29.30 displays a complex view of interactions between the jet-driven radio outflow and host galaxy environment, signalling feedback processes closely associated with the central active nucleus.

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