2009MNRAS.399.2165R


Query : 2009MNRAS.399.2165R

2009MNRAS.399.2165R - Mon. Not. R. Astron. Soc., 399, 2165-2171 (2009/November-2)

The nature of the near-infrared core source in 3C 433.

RAMIREZ E.A., TADHUNTER C.N., AXON D., BATCHELDOR D., YOUNG S., PACKHAM C. and SPARKS W.B.

Abstract (from CDS):

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 (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.


Abstract Copyright: © 2009 The Authors. Journal compilation © 2009 RAS

Journal keyword(s): techniques: polarimetric - galaxies: active - galaxies: individual: 3C 433 - infrared: galaxies

Simbad objects: 10

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Number of rows : 10
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 HD 34317 Pu* 05 16 41.0394841152 +01 56 50.378438688   6.402 6.408     A0V 78 0
2 LEDA 19313 Sy2 06 36 32.2509554376 -20 34 53.181243300   18.27 17.58     ~ 139 2
3 3C 273 BLL 12 29 06.6998257176 +02 03 08.597629980   13.05 14.830 14.11   ~ 6022 1
4 QSO B1549-790 Bla 15 56 58.86979525 -79 14 04.2817241   18.80 18.800 17.84   ~ 221 1
5 MCG+07-41-003 Bla 19 59 28.35656837 +40 44 02.0972325   16.22 15.10     ~ 2537 2
6 3C 433.0 Sy2 21 23 44.5778423928 +25 04 27.670672416   17.660 16.350     ~ 338 1
7 [BBL92] 3C 433 C1 PoG ~ ~           ~ 2 0
8 [BBL92] 3C 433 S1 PoG ~ ~           ~ 2 0
9 [BBL92] 3C 433 N1 PoG ~ ~           ~ 2 0
10 [BBL92] 3C 433 C2 PoG ~ ~           ~ 2 0

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