Sasmirala Individual Information for NGC 1097

Description

NGC 1097 is a low-inclination grand-design spiral galaxy at a distance of D = 17.0 ± 5.3 Mpc (NED redshift-independent median) with a prominent nuclear starburst ring (diameter~ 18arcsec ~ 1.5 kpc; [hummel_circumnuclear_1987]) and an active nucleus both containing a LINER/Seyfert nucleus with broad double-peaked Balmer lines [storchi-bergmann_double-peaked_1993], and a young massive nuclear star cluster ([storchi-bergmann_evidence_2005]; see [nemmen_radiatively_2006] and [mason_dust_2007] for detailed studies of the AGN). The nucleus is also a flat-spectrum radio source [wolstencroft_vla_1984]. A system of two symmetrical jet-like systems was found around the nucleus (e.g., [lorre_enhancement_1978]). However, these seem to be merger or interaction remnants of stellar origin [carter_jets_1984, wehrle_nature_1997, higdon_minor-merger_2003]. NGC 1097 was first observed at MIR wavelengths by [rieke_10_1978], [telesco_ngc_1981] and [telesco_genesis_1993]. After IRAS, ISO observations [roussel_atlas_2001, ramos_almeida_mid-infrared_2007] and first subarcsecond-resolution N-band imaging with Palomar 5 m/MIRLIN followed [gorjian_10_2004]. The nucleus remained undetected in the latter. In the Spitzer/IRAC and MIPS images, the compact but resolved nucleus and the bright starburst ring are detected. The latter outshines the nucleus with increasing wavelength. Because me measure the nuclear component only, our IRAC 5.8 and 8.μm and MIPS 24 μm fluxes are significantly lower than in the literature (e.g., [dale_infrared_2005, gallimore_infrared_2010]). The IRS LR staring-mode spectrum appears completely star-formation dominated with strong PAH features, silicate 10 μm absorption and a red spectral slope in νFν-space (see also [brandl_mid-infrared_2006, mason_dust_2007, smith_mid-infrared_2007, wu_spitzer/irs_2009, bernard-salas_spitzer_2009, tommasin_spitzer-irs_2010, gallimore_infrared_2010]). At subarcsecond-resolution, the nuclear region of NGC 1097 was observed with VISIR in five narrow N-band filters and one Q-band filter in 2005 (unpublished, to our knowledge), 2006 [horst_mid_2008, horst_mid-infrared_2009, reunanen_vlt_2010], 2009 [asmus_mid-infrared_2011] and 2010 (unpublished, to our knowledge). In addition, [mason_dust_2007, mason_nuclear_2012] used T-ReCS to acquire both a Si5 and a Qa filter image in 2005. The compact MIR nucleus and at least part of the starburst ring are detected in all images, albeit partly with very low S/N (e.g., PAH1). The ring is not discussed (but see [mason_dust_2007]). In all images with sufficient S/N (but Qa), the nucleus is marginally resolved (FWHM ~ 0.45arcsec ~ 37 pc). Therefore, we measure only the unresolved nuclear component which provides fluxes lower than total nuclear fluxes in [horst_mid_2008] and [asmus_mid-infrared_2011], but consistent with the PSF fluxes in [reunanen_vlt_2010] and [mason_nuclear_2012]. The subarcsecond fluxes are on average ~ 90% lower than the Spitzer spectrophotometry, which indicates that even the central region inside the starburst ring is totally dominated by diffuse star formation. The nuclear MIR SED indicates that the PAH 11.3 μm feature is also present in the projected central ~ 30 pc. Any AGN contribution in the MIR must thus be very low as already indicated by the absence of [O IV] and [Ne V] emission [bernard-salas_spitzer_2009].

Images

Optical image (DSS, red filter). Displayed are the central 4 arcmin with North being up and East to the left. The colour scaling is linear with white corresponding to the median background (BG) and black to the 0.01% pixels with the highest intensity.

Spitzer MIR images. Displayed are the inner 40 arcsec with North being up and East to the left. The colour scaling is logarithmic with white corresponding to median BG and black to the 0.1% pixels with the highest intensity. The label in the bottom left states instrument and central wavelength of the filter in micron (I: IRAC, M: MIPS).

Subarcsecond-resolution MIR images sorted by increasing filter central wavelength. Displayed are the inner 4 arcsec with North being up and East to the left. The colour scaling is logarithmic with white corresponding to median BG and black to the 75% of the highest intensity of all images in units of sig_bg. The inset image (where present; either bottom or top right) shows the central arcsecond of the PSF from the calibrator star, scaled to match the science target. The labels in the bottom left state instrument and filter names (C: COMICS, M: Michelle, T: T-ReCS, V: VISIR).

SEDs

MIR SED. The description of the symbols in all the SED plots (where present) is the following: Grey crosses and solid lines mark the Spitzer/IRAC, MIPS and IRS data. The colour coding of the other symbols is as follows: green for COMICS, magenta for Michelle, blue for T-ReCS and red for VISIR data. Darker-coloured solid lines mark spectra of the corresponding instrument. The black filled circles mark the nuclear 12 and 18 micron continuum emission estimate from the data (where present). The ticks on the top axis mark positions of common MIR emission lines, while the light grey horizontal bars mark wavelength ranges affected by the silicate 10 and 18 micron features.

Photometry details and reduced FITS files

ObjectRA
[deg]
Dec
[deg]
FilterImageInfoλ_c
[um]
HWHM
[um]
InstrPix. size
[arcsec/pix]
T_exp
[s]
ModeChop Throw
[arcsec]
Chop Angle
[deg]
Rot
[deg]
Prog IdCal. StarCal. DateDate 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]
NGC 109741.579167-30.275000NEII_1NGC1097_NEII_1_2006-08-07T09-08.fits[Details]12.270.18VISIR0.0752524.0PARA8.045.00.0077.B-0137(A)HD7872006-08-07T08:48:29Z2006-08-07T09:08:38Z0.05280.001036085.6False27.93.1False18.71.80.340.32119.00.430.39169.0
NGC 109741.579167-30.275000PAH1NGC1097_PAH1_2010-07-12T09-36.fits[Details]8.590.42VISIR0.075361.0PARA8.045.00.0085.B-0639(C)HD2179022010-07-12T09:21:36Z2010-07-12T09:37:26Z0.016880.000249922.6False14.70.8False14.60.80.350.3189.0N/AN/AN/A
NGC 109741.579167-30.275000PAH2NGC1097_PAH2_2005-10-09T08-02.fits[Details]11.250.59VISIR0.127883.0PARA25.00.00.0076.B-0656(A)HD168152005-10-09T07:12:00Z2005-10-09T08:02:24Z0.152060.001116961.8False30.35.1False13.05.10.390.36165.00.610.5493.0
NGC 109741.579167-30.275000PAH2NGC1097_PAH2_2009-07-15T09-17.fits[Details]11.250.59VISIR0.0751994.0PARA8.045.00.0083.B-0536(A)HD2179022009-07-15T09:00:00Z2009-07-15T09:17:17Z0.013920.000216617.0False29.17.5False19.64.20.430.3874.00.530.4578.0
NGC 109741.579167-30.275000PAH2_2NGC1097_PAH2_2_2005-10-09T08-22.fits[Details]11.880.37VISIR0.127883.0PARA25.00.00.0076.B-0656(A)HD226632005-10-09T09:17:17Z2005-10-09T08:22:34Z0.231890.006434372.6False22.43.7False18.43.70.430.41103.00.520.422.0
NGC 109741.579167-30.275000PAH2_2NGC1097_PAH2_2_2006-09-04T08-48.fits[Details]11.880.37VISIR0.0752528.0PARA25.00.00.0077.B-0728(A)HD269672006-09-04T10:01:55Z2006-09-04T08:48:29Z0.024580.000738761.1False17.50.9False16.40.50.340.3278.00.40.3481.0
NGC 109741.579167-30.275000Q2NGC1097_Q2_2006-09-05T06-31.fits[Details]18.720.88VISIR0.0751987.0PARA25.00.00.0077.B-0728(A)HD269672006-09-05T09:38:53Z2006-09-05T06:31:41Z0.330440.005243784.6False54.29.0False45.29.00.480.4777.00.550.49136.0
NGC 109741.579167-30.275000QaNGC1097_Qa_2005-09-16T06-11.fits[Details]18.30.76TRECS0.09912.0PARA15.0-90.00.0GS-2005B-Q-29HD148902005-09-16T06:00:00Z2005-09-16T06:11:31Z0.088250.002691866.0False47.411.2False54.111.30.550.52120.00.520.4856.0
NGC 109741.579167-30.275000SIV_2NGC1097_SIV_2_2010-07-12T09-48.fits[Details]10.770.19VISIR0.075724.0PARA8.045.00.0085.B-0639(C)HD2179022010-07-12T09:28:48Z2010-07-12T09:47:31Z0.033960.000676818.3False26.89.0False21.01.10.40.3585.00.470.3889.0
NGC 109741.579167-30.275000Si5NGC1097_Si5_2005-09-17T06-28.fits[Details]11.660.57TRECS0.09456.0PARA15.0-90.00.0GS-2005B-Q-29HD148902005-09-17T06:14:24Z2005-09-17T06:28:48Z0.007326e-054280.0False26.51.9False20.71.90.430.41100.00.480.4667.0