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Title:
The nature of the near-infrared core source in 3C 433
Authors:
Ramírez, Edgar A.; Tadhunter, C. N.; Axon, D.; Batcheldor, D.; Young, S.; Packham, C.; Sparks, W. B.
Affiliation:
AA(Department of Physics and Astronomy, University of Sheffield, Sheffield S3 7RH), AB(Department of Physics and Astronomy, University of Sheffield, Sheffield S3 7RH), AC(Department of Physics, Rochester Institute of Technology, 85 Lomb Memorial Drive, Rochester, NY 14623, USA), AD(Department of Physics, Rochester Institute of Technology, 85 Lomb Memorial Drive, Rochester, NY 14623, USA), AE(Department of Physics, Rochester Institute of Technology, 85 Lomb Memorial Drive, Rochester, NY 14623, USA), AF(Department of Astronomy, University of Florida, 211 Bryant Science Center, PO Box 112055, Gainesville, FL 32611-2055, USA), AG(Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD 21218, USA)
Publication:
Monthly Notices of the Royal Astronomical Society, Volume 399, Issue 4, pp. 2165-2171. (MNRAS Homepage)
Publication Date:
11/2009
Origin:
MNRAS
MNRAS Keywords:
techniques: polarimetric , galaxies: active , galaxies: individual: 3C 433 , infrared: galaxies
Abstract Copyright:
(c) Journal compilation © 2009 RAS
DOI:
10.1111/j.1365-2966.2009.15417.x
Bibliographic Code:
2009MNRAS.399.2165R

Abstract

We report the analysis of near-infrared (near-IR) imaging, polarimetric and spectroscopic observations of the powerful radio galaxy 3C 433 (z = 0.1016), obtained with the Hubble Space Telescope (HST) and the United Kingdom Infrared Telescope. The high spatial resolution of HST allows us to study the near-nuclear regions of the galaxy (<1 kpc). In line with previous observations, we find that 3C 433 has an unresolved core source that is detected in all near-IR bands, but dominates over the host galaxy emission at 2.05μm.

Our analysis reveals (1) the presence of a dust lane aligned close to the perpendicular [position angle (PA) = 70° +/- 5°] to the inner radio jet axis (PA = -12° +/- 2°), (2) a steep slope to the near-IR spectral energy distribution (SED; α = 5.8 +/- 0.1; Fν ~ ν-α), (3) an apparent lack of broad permitted emission lines at near-IR wavelengths, in particular the absence of a broad Paα emission line and (4) high intrinsic polarization for the unresolved core nuclear source (8.6 +/- 1 per cent), with an E-vector perpendicular to the inner radio jet. Using five independent techniques, we determine an extinction to the compact core source in the range 3 < AV < 67 mag.

An analysis of the long wavelength SED rules out a synchrotron origin for the high near-IR polarization of the compact core source. Therefore, scattering and dichroic extinction are plausible polarizing mechanisms, although in both of these cases the broad permitted lines from the active galactic nuclei are required to have a width >104 km s-1 (full width at half-maximum) to escape detection in our near-IR spectrum. Dichroic extinction is the most likely polarization mechanism because it is consistent with the various available extinction estimates. In this case, a highly ordered, coherent toroidal magnetic field must be present in the obscuring structure close to the nucleus.

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