IRAS 04103-2838 is a disturbed ultra-luminous infrared galaxy at a redshift of z = 0.1175 with an active nucleus classified optically either as H II or LINER [veilleux_optical_1999, veilleux_new_1999] but also as Sy 2 [yuan_role_2010]. The presence of a Compton-thick AGN was demonstrated through deep X-ray observations [teng_xmm-newton_2008], confirming the type II nature of this source. IRAS 04103-2838 was observed with Spitzer/IRS in LR staring mode. The MIR spectrum indicates star formation with silicate 10 μm absorption, PAH emission and a red spectral slope in νFν-space (see also [imanishi_spitzer_2007]). IRAS 04103-2838 was observed with T-ReCS in the Qa filter in 2008 and a compact MIR nucleus was detected [imanishi_subaru_2011]. The nucleus is possibly marginally resolved (FWHM ~ 0.63arcsec ~ 1.3 kpc), but this needs to be verified with at least a second epoch of subarcsecond MIR imaging. Our measured nuclear Qa flux is consistent with the value from [imanishi_subaru_2011] and also the IRS spectrum. Therefore, we use the latter to compute the nuclear 12 μm continuum emission estimates corrected for the silicate 10 μm feature.
Object | RA [deg] | Dec [deg] | Filter | Image | Info | λ_c [um] | HWHM [um] | Instr | Pix. size [arcsec/pix] | T_exp [s] | Mode | Chop Throw [arcsec] | Chop Angle [deg] | Rot [deg] | Prog Id | Cal. Star | Cal. Date | Date Obs. | Factor [mJy/ct] | Err. Factor [mJy/ct] | Cal. Flux [mJy] | Upper Lim. Gauss? | F_Gauss [mJy] | E(F_Gauss) [mJy] | Upper Lim. PSF? | F_PSF [mJy] | E(F_PSF) [mJy] | Cal. Maj. [arcsec] | Cal. Min. [arcsec] | Cal. PA. [deg] | Maj. Ax [arcsec] | Min. Ax [arcsec] | Pos. Ang. [deg] |
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
IRAS 04103-2838 | 63.080833 | -28.506944 | Qa | IRAS04103-2838_Qa_2008-09-11T08-37.fits | [Details] | 18.3 | 0.76 | TRECS | 0.09 | 927.0 | PARA | 15.0 | 0.0 | 0.0 | GS-2008B-C-2 | HD25025 | 2008-09-11T08:24:00Z | 2008-09-11T08:36:58Z | 0.06082 | 0.00055 | 34560.0 | False | 281.9 | 12.1 | False | 250.0 | 12.0 | 0.64 | 0.55 | 34.0 | 0.69 | 0.57 | 77.0 |