Description
NGC 2623 is an infrared-luminous advanced merger system at a redshift of z = 0.0185 (D ~ 87.3 Mpc) with only
one identified nucleus (see [evans_off-nuclear_2008] for a recent multiwavelength study of the system). An AGN
was detected at X-ray and radio wavelengths inside the compact central starburst [maiolino_elusive_2003,
lonsdale_starburst-agn_1993] but is optically ”elusive” with a spectral properties similar to NGC 4945
[maiolino_elusive_2003]. It has also been classified as a LINER or AGN/starburst composite (e.g.,
[lipari_infrared_2004]). In addition, the detection of [Ne V] provides further evidence for an AGN
in NGC 2623 [dudik_mid-infrared_2007]. After the discovery of its MIR brightness through IRAS,
NGC 2623 was observed by [carico_iras_1988], [wright_recent_1988], [wynn-williams_luminous_1993],
[bushouse_distribution_1998], and [dudley_new_1999]. The first subarcsecond-resolution N-band images were
made with Keck/LWS [soifer_high-resolution_2001] where a marginally resolved MIR nucleus with
east-west elongation coinciding with the radio morphology was detected (major axis~ 2arcsec ~ 0.8 kpc;
PA~ 90∘). In the Spitzer/IRAC and MIPS images, NGC 2623 appears a compact MIR nucleus with
faint host emission, which becomes weaker towards longer wavelengths. Our nuclear IRAC 5.8 and
8.0 μm and MIPS 24 μm fluxes agree in general with the values by [u_spectral_2012]. The IRS LR
staring-mode spectrum exhibits deep silicate 10 μm and possible silicate 18 μm absorption features, prominent
PAH emission and a steep red spectral slope in νFν-space (see also [brandl_mid-infrared_2006,
bernard-salas_spitzer_2009]). NGC 2623 was observed with COMICS in the Q17.7 filter in 2008
[imanishi_subaru_2011] and a marginally resolved MIR nucleus was detected (~ 1arcsec ~ 0.4 kpc) but with a
position angle of ~ 50∘. Because this is inconsistent with the previous Keck/LWS images, we classify NGC 2623 as
possibly extended only. Our remeasured nuclear Q17.7 flux is significantly higher than the value by
[imanishi_subaru_2011] but consistent with the Spitzer spectrophotometry and the Keck/LWS data.
Therefore, we use the IRS spectrum to calculate the 12 μm continuum emission estimate corrected for the
silicate feature. Note however, that the nuclear fluxes would be significantly lower if the presence of
subarcsecond-extended emission can be verified. Owing to the presence of PAH emission in the IRS spectrum and
the object distance, the subarcsecond MIR values of NGC 2623 are presumably heavily star-formation
contaminated.
-
[bernard-salas_spitzer_2009]
J. Bernard-Salas, H. W. W. Spoon, V. Charmandaris, V. Lebouteiller,
D. Farrah, D. Devost, B. R. Brandl, Yanling Wu, L. Armus, L. Hao, G. C.
Sloan, D. Weedman, and J. R. Houck.
A spitzer
high-resolution mid-infrared spectral atlas of starburst galaxies
.
ApJS
,
184
pp. 230–247, October 2009.
-
[brandl_mid-infrared_2006] B. R. Brandl,
J. Bernard-Salas, H. W. W. Spoon, D. Devost, G. C. Sloan, S. Guilles, Y. Wu,
J. R. Houck, D. W. Weedman, L. Armus, P. N. Appleton, B. T. Soifer,
V. Charmandaris, L. Hao, J. A. Marshall Higdon, and T. L. Herter.
The mid-infrared
properties of starburst galaxies from spitzer-IRS spectroscopy
.
ApJ
,
653
pp. 1129–1144, December 2006.
-
[bushouse_distribution_1998] Howard A.
Bushouse, C. M. Telesco, and Michael W. Werner.
The distribution
of mid- and far-infrared emission in 10 interacting galaxy systems
.
AJ
,
115
pp. 938–946, March 1998.
-
[carico_iras_1988] David P. Carico, D. B. Sanders,
B. T. Soifer, J. H. Elias, K. Matthews, and G. Neugebauer.
The IRAS
bright galaxy sample. III - 1-10 micron observations and coadded IRAS
data for galaxies with l(IR) equal to or greater than 10 to the 11th solar
luminosities
.
AJ
,
95
pp. 356–373, February 1988.
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[dudik_mid-infrared_2007] R. P. Dudik, J. C.
Weingartner, S. Satyapal, Jacqueline Fischer, C. C. Dudley, and
B. O'Halloran.
Mid-infrared
fine-structure line ratios in active galactic nuclei observed with the
spitzer IRS: evidence for extinction by the torus
.
ApJ
,
664
pp. 71–87, July 2007.
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[dudley_new_1999] C. C. Dudley.
New 8-13mum
spectroscopy of luminous and ultraluminous infrared galaxies
.
MNRAS
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307
pp. 553–576, August 1999.
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[evans_off-nuclear_2008] A. S. Evans,
T. Vavilkin, J. Pizagno, F. Modica, J. M. Mazzarella, K. Iwasawa, J. H.
Howell, J. A. Surace, L. Armus, A. O. Petric, H. W. W. Spoon, J. E. Barnes,
T. A. Suer, D. B. Sanders, B. Chan, and S. Lord.
Off-nuclear
star formation and obscured activity in the luminous infrared galaxy NGC
2623
.
ApJL
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pp. L69–L72, March 2008.
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[imanishi_subaru_2011] Masatoshi Imanishi,
Keisuke Imase, Nagisa Oi, and Kohei Ichikawa.
Subaru and
gemini high spatial resolution infrared 18 μm imaging observations of nearby
luminous infrared galaxies
.
AJ
,
141
pp. 156, May 2011.
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[lipari_infrared_2004] S. Lípari,
E. Mediavilla, R. J. Díaz, B. García-Lorenzo, J. Acosta-Pulido, M. P.
Agüero, and R. Terlevich.
Infrared
mergers and infrared quasi-stellar objects with galactic winds - i. NGC
2623: nuclear outflow in a proto-elliptical candidate
.
MNRAS
,
348
pp. 369–394, February 2004.
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[lonsdale_starburst-agn_1993] Colin J.
Lonsdale, Harding J. Smith, and Carol J. Lonsdale.
The
starburst-AGN connection - a sensitive VLBI survey of luminous IRAS
galaxies
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ApJL
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405
pp. L9–L12, March 1993.
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[maiolino_elusive_2003] R. Maiolino,
A. Comastri, R. Gilli, N. M. Nagar, S. Bianchi, T. Böker, E. Colbert,
A. Krabbe, A. Marconi, G. Matt, and M. Salvati.
Elusive active
galactic nuclei
.
MNRAS
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344
pp. L59–L64, October 2003.
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[soifer_high-resolution_2001] B. T.
Soifer, G. Neugebauer, K. Matthews, E. Egami, A. J. Weinberger, M. Ressler,
N. Z. Scoville, S. R. Stolovy, J. J. Condon, and E. E. Becklin.
High-resolution
mid-infrared imaging of infrared-luminous starburst galaxies
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AJ
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pp. 1213–1237, September 2001.
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[u_spectral_2012] Vivian U, D. B. Sanders, J. M.
Mazzarella, A. S. Evans, J. H. Howell, J. A. Surace, L. Armus, K. Iwasawa,
D.-C. Kim, C. M. Casey, T. Vavilkin, M. Dufault, K. L. Larson, J. E. Barnes,
B. H. P. Chan, D. T. Frayer, S. Haan, H. Inami, C. M. Ishida, J. S.
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[wright_recent_1988] G. S. Wright, R. D. Joseph,
N. A. Robertson, P. A. James, and W. P. S. Meikle.
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[wynn-williams_luminous_1993] C. G.
Wynn-Williams and E. E. Becklin.
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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.