ESO 428-14 is a spiral galaxy at a redshift of z = 0.0057 (D ~ 26 Mpc) close to the Galactic plane. It is hosting a Sy 2 nucleus [veron-cetty_catalogue_2010] and possesses a bended jet-like radio structure [ulvestad_radio_1989] aligned with a cone-like extended narrow-line region (PA~-50degre; [wilson_0714_1989, falcke_helical_1996]). ESO 428-14 was observed with Spitzer/IRAC, IRS and MIPS. The compact MIR nucleus detected in all images is embedded in weak extended host emission along the north-south direction visible in the IRAC 5.8 and 8.0 μm images. Two epochs of MIPS 24 μm images (2004 and 2006) are available. Our flux measurement of the nuclear source agrees with the value published in [temi_spitzer_2009]. The IRS LR staring-mode spectrum shows strong forbidden line emission, PAH features and silicate 10 μm absorption, indicating a star formation contribution (see also [shi_9.7_2006]). The MIR spectrum rises steeply and peaks around ~ 18 μm in νFν-space. We observed ESO 428-14 with VISIR in three narrow N-band and one Q-band filter during one night in 2007 and also obtained a VISIR N-band spectrum [honig_dusty_2010-1]. All images show a compact nuclear source embedded in increasingly prominent extended bar-like emission towards the longer wavelength filters. In the Q-band image (unpublished, to our knowledge), a knot ~ 1arcsec south-east of the nucleus becomes visible. The extended emission is oriented along the north-west direction (PA~ 140∘), aligned with the NLR emission and host galaxy major axis. The VISIR spectrum possesses the same continuum shape, silicate absorption and forbidden emission lines as the IRS spectrum. However, the continuum flux level is lower and the PAH emission is also absent, indicating that the subarcsecond scales do not have significant star formation contribution. While [honig_dusty_2010-1] have presented the VISIR spectrophotometry integrated over the inner 0.75arcsec, we now isolate the unresolved fluxes, which are significantly lower. In particular, the average subarcsecond nuclear fluxes are ~ 60% lower than the values of the Spitzer spectrophotometry.
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] |
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
ESO 428-14 | 109.130000 | -29.324722 | ARIII | ESO428-G014_ARIII_2007-03-01T03-33.fits | [Details] | 8.99 | 0.14 | VISIR | 0.075 | 699.0 | PARA | 8.0 | 45.0 | 0.0 | 078.B-0303(A) | HD75691 | 2007-03-01T03:07:12Z | 2007-03-01T03:34:34Z | 0.0613 | 0.00031 | 17864.4 | False | 115.2 | 0.6 | False | 70.0 | 0.4 | 0.33 | 0.29 | 143.0 | 0.41 | 0.38 | 116.0 |
ESO 428-14 | 109.130000 | -29.324722 | PAH1 | ESO428-G014_PAH1_2007-03-01T03-30.fits | [Details] | 8.59 | 0.42 | VISIR | 0.075 | 63.0 | PARA | 8.0 | 45.0 | 0.0 | 078.B-0303(A) | HD41047 | 2007-03-01T01:01:55Z | 2007-03-01T03:30:14Z | 0.0217 | 0.00033 | 10812.0 | False | 114.6 | 13.4 | False | 71.8 | 11.3 | 0.32 | 0.28 | 137.0 | 0.4 | 0.37 | 176.0 |
ESO 428-14 | 109.130000 | -29.324722 | PAH2_2 | ESO428-G014_PAH2_2_2007-03-01T03-42.fits | [Details] | 11.88 | 0.37 | VISIR | 0.075 | 362.0 | PARA | 8.0 | 45.0 | 0.0 | 078.B-0303(A) | HD75691 | 2007-03-01T03:07:12Z | 2007-03-01T03:41:46Z | 0.02367 | 0.00023 | 10819.2 | False | 211.8 | 5.4 | False | 114.7 | 12.7 | 0.33 | 0.32 | 141.0 | 0.48 | 0.4 | 130.0 |
ESO 428-14 | 109.130000 | -29.324722 | Q1 | ESO428-G014_Q1_2007-03-01T03-50.fits | [Details] | 17.65 | 0.83 | VISIR | 0.075 | 684.0 | PARA | 8.0 | 45.0 | 0.0 | 078.B-0303(A) | HD75691 | 2007-03-01T03:11:31Z | 2007-03-01T03:50:24Z | 0.43785 | 0.00908 | 5124.0 | False | 768.6 | 45.1 | False | 308.4 | 11.8 | 0.47 | 0.46 | 153.0 | 0.96 | 0.57 | 139.0 |