Sasmirala Individual Information for NGC 2992

Description

NGC 2992 is a highly-inclined spiral galaxy interacting with NGC 2993 2.9arcmimin  to the south at a redshift of z = 0.0077 (D ~ 39.7 Mpc) with a well-studied AGN belonging to the nine-month BAT AGN sample. This AGN exhibits huge X-ray variations (factor of ~ 20; e.g., [murphy_monitoring_2007]) and has changed its optical type between Sy 1.5 and Sy 2.0, which is presumably caused by intrinsic changes in the ionizing continuum rather than varying obscuration [gilli_variability_2000, trippe_long-term_2008]. The nucleus is obscured by a crossing prominent dust lane instead [ward_new_1980]. The AGN is surrounded by an extended biconical NLR with a total extent of ~ 5 kpc (PA~ 125;e.g., [allen_physical_1999]). At radio wavelengths, a compact radio core and a prominent double loop structure extending in total 8arcsec (~ 1.5 kpc) to the north-west and south-east (PA~ 154; [ulvestad_radio_1984, wehrle_radio_1988]), which are possibly generated by an AGN-driven jet [colbert_large-scale_1998, veilleux_biconical_2001]. The first MIR observations were performed by [glass_mid-infrared_1982], [lonsdale_infrared_1984], followed by [aitken_8-13_1985], [ward_continuum_1987], and [roche_atlas_1991]. Subarcsecond N-band imaging was then performed with Palomar 5 m/MIRLIN [gorjian_10_2004], with Keck/LWS [soifer_high_2004], and with ESO 3.6 m/TIMMI2 [galliano_mid-infrared_2005]. In all cases an unresolved MIR nucleus without extended host emission was detected. In the Spitzer/IRAC images lenticular extended host emission was detected in addiction to the MIR nucleus, while NGC 2992 appears compact in the MIPS images. We extract the nuclear component resulting in an IRAC 5.8 flux consistent with [gallimore_infrared_2010], while the 8.μm value is significantly lower. The IRS LR staring-mode spectrum exhibits silicate 10 μm absorption, prominent PAH features and forbidden emission lines, and a generally red spectral slope in νFν-space (see also [wu_spitzer/irs_2009, deo_mid-infrared_2009, gallimore_infrared_2010]). Thus, it appears that NGC 2992 is significantly affected by star formation on arcsecond scales, although on nuclear scales [friedrich_adaptive_2010] constrain star formation to be minor. NGC 2992 was repeatedly observed with VISIR in four narrow N-band filters spread over 2004, 2005, 2006 and 2009. The first two measurements were published in [haas_visir_2007]. In addition, Michelle imaging in the N’ and Qa filters was performed in 2006 [ramos_almeida_infrared_2009]. A compact MIR nucleus was detected in all cases, while the deepest image (N’) shows very faint edge-on spiral-like emission extending from the nucleus similar to the IRAC 8 μm image (PA~ 30; diameter~ 13arcsec ~ 2.5 kpc). The nucleus itself is extended in the north-south directions in that image as well (PA~ 5; FWHM(major axis)~ 0.49arcsec ~ 90 pc). It appears resolved also in the sharpest image (NEII_1 from 2006-02-16) but with a slightly larger position angle (PA~ 12). Thus, we classify the nucleus of NGC 2992 as resolved in the MIR at subarcsecond resolution. On average, the nuclear PSF photometry is ~ 42% lower than the Spitzer spectrophotometry. However, we notice that the VISIR measurements from 2009 are systematically ~ 48% lower than the VISIR measurements from 2006 in the same filters. The Michelle and early VISIR total fluxes are rather consistent with the Spitzer data, and possibly also with the historical measurements. Such a comparison is however complicated by the strong MIR features in the N-band at arcsecond scales. Thus, it is possible that NGC 2992 exhibits long-term MIR flux variations similar to shorter wavelengths (e.g., [glass_variability_1997]). For these reasons, we are also unable to constrain the spectral features as silicate and PAH at subarcsecond resolution, despite the good N-band coverage.

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 2992146.425417-14.326389NEII_1NGC2992_NEII_1_2006-02-16T05-07.fits[Details]12.270.18VISIR0.0751264.0PERP8.00.00.0076.B-0468(A)HD826602006-02-16T05:45:36Z2006-02-16T05:08:10Z0.055890.00123224.4False277.712.9False236.213.60.330.3199.00.360.3412.0
NGC 2992146.425417-14.326389NEII_1NGC2992_NEII_1_2006-02-17T05-17.fits[Details]12.270.18VISIR0.0751267.0PERP8.00.00.0076.B-0468(A)HD826602006-02-17T04:33:36Z2006-02-17T05:18:14Z0.057360.000973224.4False283.06.3False271.66.90.350.34148.00.360.35119.0
NGC 2992146.425417-14.326389NEII_1NGC2992_NEII_1_2009-11-30T08-12.fits[Details]12.270.18VISIR0.075181.0PARA8.045.00.0084.B-0606(A)HD756912009-11-30T08:03:50Z2009-11-30T08:12:29Z0.055780.0018210187.9False193.115.9False146.112.50.390.3665.00.460.3913.0
NGC 2992146.425417-14.326389NEII_1NGC2992_NEII_1_2009-12-02T07-07.fits[Details]12.270.18VISIR0.075181.0PARA8.045.00.0084.B-0606(A)HD756912009-12-02T06:50:24Z2009-12-02T07:07:41Z0.052650.000910187.9False166.03.0False155.79.00.410.36111.00.410.3734.0
NGC 2992146.425417-14.326389NEIINGC2992_NEII_2006-02-16T04-40.fits[Details]12.810.21VISIR0.0751267.0PERP8.00.00.0076.B-0468(A)HD817992006-02-16T03:44:38Z2006-02-16T04:40:48Z0.068240.001473715.1False361.312.5False277.98.90.350.32104.00.380.3866.0
NGC 2992146.425417-14.326389NEIINGC2992_NEII_2006-02-17T04-51.fits[Details]12.810.21VISIR0.0751267.0PERP8.00.00.0076.B-0468(A)HD826602006-02-17T04:40:48Z2006-02-17T04:52:19Z0.066130.001373077.5False364.710.1False294.911.30.360.35147.00.40.3897.0
NGC 2992146.425417-14.326389NEII_2NGC2992_NEII_2_2009-12-02T07-11.fits[Details]13.040.22VISIR0.075181.0PARA8.045.00.0084.B-0606(A)HD756912009-12-02T06:57:36Z2009-12-02T07:12:00Z0.054310.000429388.8False223.25.0False180.217.90.390.34100.00.420.3948.0
NGC 2992146.425417-14.326389N_primeNGC2992_N_prime_2006-05-12T05-56.fits[Details]11.21.2MICHELLE0.101188.0PARA15.00.00.0GN-2006A-Q-11HD826602006-05-12T05:45:36Z2006-05-12T05:57:07Z0.565270.006123946.0False229.84.0False161.23.50.40.34175.00.490.415.0
NGC 2992146.425417-14.326389PAH2NGC2992_PAH2_2004-12-22T08-55.fits[Details]11.250.59VISIR0.1272120.0PERP20.00.00.060.A-9244(A)HD826602004-12-22T08:48:29Z2004-12-22T08:55:41Z0.150530.001293963.8False289.614.6False312.614.60.410.3798.00.390.3697.0
NGC 2992146.425417-14.326389PAH2NGC2992_PAH2_2005-02-01T06-30.fits[Details]11.250.59VISIR0.127883.0PERP20.00.00.060.A-9244(A)HD826602005-02-01T06:57:36Z2005-02-01T06:30:14Z0.171970.002213963.8False300.733.3False318.722.70.410.38152.00.40.3813.0
NGC 2992146.425417-14.326389PAH2NGC2992_PAH2_2009-11-30T08-08.fits[Details]11.250.59VISIR0.075181.0PARA8.045.00.0084.B-0606(A)HD756912009-11-30T07:55:12Z2009-11-30T08:08:10Z0.014110.0002412500.7False146.515.6False92.49.60.340.31110.00.420.3928.0
NGC 2992146.425417-14.326389PAH2NGC2992_PAH2_2009-12-02T07-02.fits[Details]11.250.59VISIR0.075181.0PARA8.045.00.0084.B-0606(A)HD756912009-12-02T06:50:24Z2009-12-02T07:03:22Z0.013790.0001312500.7False141.213.3False125.47.40.390.3399.00.390.3744.0
NGC 2992146.425417-14.326389QaNGC2992_Qa_2006-05-12T06-09.fits[Details]18.10.95MICHELLE0.101163.0PARA15.00.00.0GN-2006A-Q-11HD826602006-05-12T05:45:36Z2006-05-12T06:08:38Z10.032380.202061557.0False631.821.6False541.920.50.530.51155.00.60.5219.0