PKS1949+02

Flux data

Available Data Downloads

(definitions)Definitions.html
link to NED pagehttp://nedwww.ipac.caltech.edu/cgi-bin/nph-objsearch?objname=1949%2B02&extend=no&hconst=73&omegam=0.27&omegav=0.73&corr_z=1&out_csys=Equatorial&out_equinox=J2000.0&obj_sort=RA+or+Longitude&of=pre_text&zv_breaker=30000.0&list_limit=5&img_stamp=YES

Infrared data

Radio data

Optical data

X-Ray data

Spitzer 70um DataPKS1949+02_files/1949_70um.fits
Spitzer 160um DataPKS1949+02_files/1954_160um.fits

Chandra

1.4GHzPKS1949+02_files/3c403HIcont.fits
ESO Optical spectraPKS1949+02_files/s1949.zip

Spitzer IRS spectra

PKS1949+02

Optical spectrum taken with ESO telescopes.

Tadhunter et al. (1993)

PKS1949+02

Spitzer IRS spectra

Dicken et al. (in preperation)

Spitzer 24um DataPKS1949+02_files/1949_24um.fits

PKS1949+02

Spitzer MIPS infrared photometric observations. Left to right: 24 microns, 70 microns and 160 microns (when available). FOV are 5x5 arcmins for 24 microns, 5x2.5 arcmins for 70 microns and 0.5x5 arcmins for 160 microns.

Dicken et al. (2008)

Next objectPKS1954-38.html
PreviousPKS1938-15.html
ISAAC K-band dataPKS1949+02_files/out_1949.fits

PKS1949+02

baum et al. (1988)

Wavelength/
Frequency       Flux      Units	                Reference                
5GHz	         2.39        Jy                       Morganti et al. (1993)
[OIII] λ5007     -13.13      Log erg/cm2/s     Tadhunter et al. (1993)
15GHz core       20.0        mJy        	        Dicken et al. (2008)
22 GHz core      8.5          mJy	                 Dicken et al. (2008)
24 microns	193.0      mJy	                 Dicken et al. (2008)
70 microns	348.4      mJy	                 Dicken et al. (2008)
160 microns      251.3       mJy	                 Dicken et al. (2008)
X-ray            	-	        -	                 -http://adsabs.harvard.edu/abs/1993MNRAS.263.1023Mhttp://adsabs.harvard.edu/abs/1993MNRAS.263..999Thttp://adsabs.harvard.edu/abs/2008ApJ...678..712Dhttp://adsabs.harvard.edu/abs/2008ApJ...678..712Dhttp://adsabs.harvard.edu/abs/2008ApJ...678..712Dhttp://adsabs.harvard.edu/abs/2008ApJ...678..712Dhttp://adsabs.harvard.edu/abs/2008ApJ...678..712Dshapeimage_20_link_0shapeimage_20_link_1shapeimage_20_link_2shapeimage_20_link_3shapeimage_20_link_4shapeimage_20_link_5shapeimage_20_link_6

Other name:

Redshift:

RA (j2000):

Dec (j2000):

Optical class:

Radio Class:

Gemini imagePKS1949+02_files/p1949.fits

0.059

19 52 15.77

+02 30 23.1

NLRG

FRII

3C403

PKS1949+02

K-band ISAAC (2.2 microns) image. 1x1 arcmins.

Inskip et al. (2010)


N

E

PKS1949+02

Gemini GMOS-S Smooth galaxy subtracted image

Ramos Almeida et al. (2011a)


Gemini/GMOS-S: Unsharp mask image

Images, Maps, Spectra and SEDs

    6cm VLA radio map

Notes

    This NLRG/FRII galaxy with an X-shaped radio morphology (Black et al. 1992) was observed in the optical with HST by Martel et al. (1999) and de Koff et al. (2000), who reported the existence of dust lanes and a low-surface brightness halo with a sharp boundary surrounding the central region at a radius of ∼2.5 arcsec. Our Gemini optical image confirms the latter feature, and, for the first time, also reveals an extraordinary series of concentric arc/shell features extending to a maximum radius of ∼12 kpc to the west, and ∼20 kpc to the south (Ramos Almeida et al. 2011a). The brightest of these shell features has a corrected surface brightness of μ_V = 22.6 mag arcsec^−2 . The K-band model-subtracted residual images presented in Inskip et al. (2010) reveal hints of the shells, indicating their continuum-emitting nature. Our long-slit spectra confirm that the outer arc and shell features are not dominated by emission-line radiation. It is possible that this source has undergone merger activity in the relatively recent past. The X-shaped radio source has been linked to rapid jet reorientation ∼10^7 yr previously (Dennett-Thorpe et al. 2002).

The optical spectrum reveals high-ionization emission lines of high equivalent width.


PKS1949+02

Spectral energy distribution.  The blue solid line is fitted to the data from 109 to 1010 Hz. Extrapolating this line from the radio to the infrared SED tests whether non-thermal synchrotron emission from the lobes can contaminate the Spitzer mid-infrared flux. In this case the lobes emission lies out of the Spitzer beam so cannot contaminate the Spitzer data.  The weak, flat spectrum, non-thermal radio core emission is also not likely to contaminate the Spitzer infrared flux data for this object.

Dicken et al. (2008)