M81 is a nearby grand-design spiral galaxy at a distance of D = 3,6 ± 0.5 Mpc (NED redshift-independent median) with one of the intrinsically weakest known AGN, which is also a flat-spectrum radio source (e.g., [ho_radio_2001]). It exhibits both LINER and Sy 1.8 characteristics [filippenko_detailed_1988, ho_new_1996] and extraordinary low obscuration (NH ~ 5 ⋅ 1020 cm-2; [page_x-ray_2003]). Motivated by its similarity to Sgr A*, an extensive multiwavelength campaign was performed on M 81 by [markoff_results_2008] in order to compare and characterize SED and the short-term (daily) variability that occurs in this object (in addition to the yearly variations). They found striking similarities to the hard state of X-ray binaries. The first MIR observations of M81 were performed by [kleinmann_infrared_1970], [rieke_10_1978] and [dyck_photometry_1978], followed by first subarcsecond-resolution N-band imaging with Palomar 5 m/MIRLIN in 1999 [grossan_high-resolution_2001, gorjian_10_2004] with a possibly resolved nucleus and a significantly higher than the previous measurements. M81 was followed up by [soifer_high_2004] with Keck/LWS in the SIC filter in 2000 (and 2002 but under non-photometric conditions by [grossan_high_2004]), who find the nucleus marginally resolved (FWHM= 0.36arcsec ~ 7 pc). Spitzer/IRAC has observed M81 seven times between 2003 and 2005 and Spitzer/MIPS was used for three observations between 2003 and 2004. In all cases, a compact nucleus embedded in extended host emission was detected (see also [willner_infrared_2004, smith_anomalous_2010]). Because we measure the photometry of the nuclear component only, our IRAC 5.8 and 8.0 μm and MIPS 24 μm fluxes are significantly lower than the values in the literature (e.g., [dale_infrared_2005, munoz-mateos_radial_2009]). However, our nuclear IRAC fluxes are a factor of two higher than those of [willner_infrared_2004] for unknown reasons, but are on the other hand roughly consistent with the Spitzer/IRS LR mapping mode spectrum. The latter shows very strong silicate emission and also a prominent PAH 11.3 μm feature but no other significant PAH features (see e.g., [smith_anomalous_2010, wu_spitzer/irs_2009, dale_spitzer_2009, mason_nuclear_2012]). The steep spectral slope at the short wavelength side of the silicate 10 μm is most likely the cause for the apparent flux variations reported earlier as already noted by [smith_anomalous_2010].
We observed the nucleus of M81 with Michelle in two N-band filters in 2010. Additional Michelle imaging in three N and one Q-band filters was performed in 2011 [mason_nuclear_2012]. A compact MIR nucleus was detected in all Michelle images, which appears marginally resolved in our Si-5 and Si-6 images but not in the Si-2 image from 2011 which shows the highest angular resolution. Therefore, it remains uncertain, whether the nucleus of M81 is in general resolved at subarcsecond resolution in the MIR but the results of [mason_nuclear_2012] suggest it to be rather unresolved. Our nuclear flux measurements are on average ~ 24% lower than the Spitzer spectrophotometry and consistent with previous measurements but for unknown reasons systematically ~ 20% higher than the values of [mason_nuclear_2012] for the same data. The silicate 10 μm feature is reproduced with the subarcsecond data and thus originates in the projected central ~ 7 pc of the nucleus of M81. Therefore, we use the IRS spectrum to correct our 12 and 18 μm continuum emission estimate for the silicate features.
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] |
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
M81 | 148.888333 | 69.065278 | Qa | M081_Qa_2011-02-04T12-11.fits | [Details] | 18.1 | 0.95 | MICHELLE | 0.101 | 324.0 | PARA | 15.0 | 0.0 | 0.0 | GN-2011A-Q-55 | HD92523 | 2011-02-04T12:38:53Z | 2011-02-04T12:11:31Z | 8.4461 | 0.11644 | 2927.0 | False | 330.9 | 29.5 | False | 263.9 | 29.4 | 0.58 | 0.54 | 33.0 | 0.66 | 0.59 | 18.0 |
M81 | 148.888333 | 69.065278 | Si-2 | M081_Si-2_2011-02-03T11-16.fits | [Details] | 8.8 | 0.45 | MICHELLE | 0.101 | 311.0 | PARA | 15.0 | 0.0 | 0.0 | GN-2011A-Q-55 | HD92523 | 2011-02-03T10:52:19Z | 2011-02-03T11:15:22Z | 1.0411 | 0.01182 | 10698.0 | False | 67.9 | 2.3 | False | 72.4 | 2.3 | 0.5 | 0.44 | 35.0 | 0.46 | 0.43 | 31.0 |
M81 | 148.888333 | 69.065278 | Si-4 | M081_Si-4_2011-02-03T11-35.fits | [Details] | 10.3 | 0.5 | MICHELLE | 0.101 | 309.0 | PARA | 15.0 | 0.0 | 0.0 | GN-2011A-Q-55 | HD92523 | 2011-02-03T10:52:19Z | 2011-02-03T11:35:31Z | 1.7694 | 0.02807 | 8704.0 | False | 188.5 | 4.9 | False | 154.8 | 4.5 | 0.5 | 0.44 | 45.0 | 0.53 | 0.51 | 145.0 |
M81 | 148.888333 | 69.065278 | Si-5 | M081_Si-5_2010-02-04T11-13.fits | [Details] | 11.6 | 0.55 | MICHELLE | 0.101 | 156.0 | PARA | 15.0 | 0.0 | 0.0 | GN-2010A-C-7 | HD83126 | 2010-02-04T10:48:00Z | 2010-02-04T11:13:55Z | 0.90322 | 0.01059 | 4300.0 | False | 170.2 | 4.1 | False | 127.1 | 3.8 | 0.45 | 0.41 | 31.0 | 0.52 | 0.48 | 28.0 |
M81 | 148.888333 | 69.065278 | Si-6 | M081_Si-6_2010-02-04T11-04.fits | [Details] | 12.5 | 0.6 | MICHELLE | 0.101 | 141.0 | PARA | 15.0 | 0.0 | 0.0 | GN-2010A-C-7 | HD83126 | 2010-02-04T10:40:48Z | 2010-02-04T11:03:50Z | 1.23728 | 0.01334 | 3777.0 | False | 156.0 | 4.2 | False | 116.8 | 4.1 | 0.44 | 0.41 | 60.0 | 0.52 | 0.46 | 31.0 |
M81 | 148.888333 | 69.065278 | Si-6 | M081_Si-6_2011-02-03T11-57.fits | [Details] | 12.5 | 0.6 | MICHELLE | 0.101 | 329.0 | PARA | 15.0 | 0.0 | 0.0 | GN-2011A-Q-55 | HD92523 | 2011-02-03T10:58:05Z | 2011-02-03T11:57:07Z | 1.19845 | 0.01247 | 5956.0 | False | 168.1 | 3.5 | False | 138.7 | 3.4 | 0.47 | 0.43 | 43.0 | 0.5 | 0.48 | 172.0 |