TY - JOUR
T1 - Chandra observations of the hybrid morphology radio sources 3C 433 and 4C 65.15
T2 - FR IIs with asymmetric environments
AU - Miller, B. P.
AU - Brandt, W. N.
N1 - Publisher Copyright:
© 2009. The American Astronomical Society. All rights reserved. Printed in the U.S.A.
PY - 2009/4/10
Y1 - 2009/4/10
N2 - We present Chandra observations of the hybrid morphology radio sources 3C 433 and 4C 65.15, two members of the rare class of objects possessing an FR I jet on one side of the core and an FR II lobe on the other. The X-ray spectrum of 3C 433 shows intrinsic absorption (with a column density of NH ≃ 8 × 1022 cm-2), such as is typical of FR II narrow-line radio galaxies. There is excess X-ray emission below 2 keV containing contributions from diffuse soft X-ray emission (likely hot gas with kT ∼ 1.2 keV) as well as from the nucleus. The core of 3C 433 is extended in hard X-rays, presumably due to X-ray emission from the inner-jet knot on the FR I side that is apparent in the radio map. It is possible that the X-ray emission from this inner-jet knot is absorbed by the dust known to be present in the host galaxy. The spectrum of 4C 65.15 can be modeled with a simple power law with perhaps mild intrinsic absorption (NH ≃ 1.3 × 1021 cm-2). X-ray emission is detected at the bend in the FR I jet. This X-ray jet emission lies above the extrapolation from the high-frequency radio synchrotron emission and has a spectral slope flatter than αrx, indicating that the jet spectral energy distribution is concave as with other FR II quasar jets. Both 3C 433 and 4C 65.15 have unabsorbed X-ray luminosities, radio luminosities, and optical spectra typically seen in comparable sources with FR II morphologies. Presumably, the FR I structure seen on one side in these hybrid sources is generated by a powerful jet interacting with a relatively dense environment.
AB - We present Chandra observations of the hybrid morphology radio sources 3C 433 and 4C 65.15, two members of the rare class of objects possessing an FR I jet on one side of the core and an FR II lobe on the other. The X-ray spectrum of 3C 433 shows intrinsic absorption (with a column density of NH ≃ 8 × 1022 cm-2), such as is typical of FR II narrow-line radio galaxies. There is excess X-ray emission below 2 keV containing contributions from diffuse soft X-ray emission (likely hot gas with kT ∼ 1.2 keV) as well as from the nucleus. The core of 3C 433 is extended in hard X-rays, presumably due to X-ray emission from the inner-jet knot on the FR I side that is apparent in the radio map. It is possible that the X-ray emission from this inner-jet knot is absorbed by the dust known to be present in the host galaxy. The spectrum of 4C 65.15 can be modeled with a simple power law with perhaps mild intrinsic absorption (NH ≃ 1.3 × 1021 cm-2). X-ray emission is detected at the bend in the FR I jet. This X-ray jet emission lies above the extrapolation from the high-frequency radio synchrotron emission and has a spectral slope flatter than αrx, indicating that the jet spectral energy distribution is concave as with other FR II quasar jets. Both 3C 433 and 4C 65.15 have unabsorbed X-ray luminosities, radio luminosities, and optical spectra typically seen in comparable sources with FR II morphologies. Presumably, the FR I structure seen on one side in these hybrid sources is generated by a powerful jet interacting with a relatively dense environment.
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U2 - 10.1088/0004-637X/695/1/755
DO - 10.1088/0004-637X/695/1/755
M3 - Article
AN - SCOPUS:67649882712
SN - 0004-637X
VL - 695
SP - 755
EP - 764
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1
ER -