2012A&A...543A..61B


Query : 2012A&A...543A..61B

2012A&A...543A..61B - Astronomy and Astrophysics, volume 543A61-61 (2012/7-1)

High resolution IR observations of the starburst ring in NGC 7552. One ring to rule them all ?

BRANDL B.R., MARTIN-HERNANDEZ N.L., SCHAERER D., ROSENBERG M. and VAN DER WERF P.P.

Abstract (from CDS):

Approximately 20% of all spiral galaxies display starburst activity in nuclear rings of a few hundred parsecs in diameter. It is our main aim to investigate how the starburst ignites and propagates within the ring, leading to the formation of massive stellar clusters. We observed the ring galaxy NGC7552 with the mid-infrared (MIR) instrument VISIR at an angular resolution of 0.3"-0.4" and with the near-infrared (NIR) integral-field spectrograph SINFONI on the VLT, and complement these observations with data from ISO and Spitzer. The starburst ring is clearly detected at MIR wavelengths at the location of the dust-extincted, dark ring seen in HST observations. This ``ring'', however, is a rather complex annular region of more than 100 parsec width. We find a large fraction of diffuse [NeII] and PAH emission in the central region that is not associated with the MIR peaks on spatial scales of ∼30pc. We do not detect MIR emission from the nucleus of NGC7552, which is very prominent at optical and NIR continuum wavelengths. However, we have identified nine unresolved MIR peaks within the ring. The average extinction of these peaks is AV=7.4 and their total infrared luminosity is LIR=2.1x1010L☉. The properties of these peaks are typical for MIR-selected massive clusters found in other galaxies. The ages of the MIR-selected clusters are in the range of 5.9±0.3Myr. The age spread among the clusters of 0.8Myr is small compared to the travel time of ∼5.6Myr for half an orbit within the starburst ring. We find no strong evidence for a scenario where the continuous inflow of gas leads to the ongoing formation of massive clusters at the contact points between galactic bar and starburst ring. Instead, it appears more likely that the gas density build up more gradually over larger ring segments, and that the local physical conditions govern cluster formation. We note that the fundamental limitation on the accurate derivation of cluster age, mass and initial mass function slope is the lack of higher angular resolution. Resolving the highly embedded, massive clusters requires milli-arcsecond resolution at infrared wavelengths, which will be provided by the next generation of instruments on extremely large telescopes (ELTs).

Abstract Copyright: ∼

Journal keyword(s): ISM: kinematics and dynamics - HII regions - galaxies: nuclei - galaxies: starburst - galaxies: star clusters: general - infrared: ISM

VizieR on-line data: <Available at CDS (J/A+A/543/A61): list.dat fits/*>

Nomenclature: Table 2 : [BMS2012] MN (Nos 1-9)

Simbad objects: 43

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Number of rows : 43
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 M 33 GiG 01 33 50.8965749232 +30 39 36.630403128 6.17 6.27 5.72     ~ 6226 1
2 NGC 613 AGN 01 34 18.235 -29 25 06.56   10.77 12.71 9.50 10.6 ~ 446 3
3 NGC 604 HII 01 34 32.1 +30 47 01           ~ 608 0
4 NGC 1365 Sy1 03 33 36.458 -36 08 26.37 10.48 10.08 9.63 8.79 9.7 ~ 1987 2
5 [GAP2005] NGC 1365 M5 Rad 03 33 36.55 -36 08 13.8           ~ 17 0
6 [GAP2005] NGC 1365 M6 Rad 03 33 36.750 -36 08 17.54           ~ 16 0
7 NGC 1343 AG? 03 37 49.7256129120 +72 34 16.612030092   14.1       ~ 77 1
8 NGC 1530 AG? 04 23 27.102 +75 17 44.05   13.40       ~ 287 1
9 NGC 1614 Sy1 04 34 00.027 -08 34 44.57   14.66 13.99     ~ 697 1
10 HD 35165 Be* 05 21 16.8603281544 -34 20 42.173559132 5.24 5.90 6.09 6.12 6.26 B3IVe 79 0
11 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
12 RMC 136 Cl* 05 38 42.396 -69 06 03.36   5.81 5.40     ~ 2236 2
13 UGCA 116 AGN 05 55 42.645 +03 23 32.23 10.74 11.68 11.46   11.82 ~ 561 0
14 NGC 2444 AG? 07 46 53.0555407896 +39 01 55.100891208   13.1       ~ 110 1
15 LEDA 3129223 G 07 46 53.081 +39 00 52.52           ~ 4 0
16 [BAB2009] F PoG 07 46 53.970 +39 01 06.25           ~ 2 0
17 NGC 2445 GiP 07 46 55.1013582528 +39 00 54.455374152   13.1       ~ 71 0
18 [BBA2008] Region 2 PoG 09 55 50.63 +69 40 45.6           ~ 2 0
19 M 82 AGN 09 55 52.430 +69 40 46.93 9.61 9.30 8.41     ~ 6156 6
20 [BBA2008] Region 3 PoG 09 55 52.740 +69 40 58.60           ~ 2 0
21 NGC 3603 OpC 11 14 57.9 -61 14 32           ~ 1136 1
22 NGC 4038 EmG 12 01 53.002 -18 52 03.32   10.91   9.74 11.0 ~ 1364 1
23 NAME Antennae IG 12 01 53.170 -18 52 37.92           ~ 1749 0
24 [NU2000] 3 5 Rad 12 01 54.71 -18 52 51.4           ~ 4 0
25 [BCE2005] 157 Cl* 12 01 54.89 -18 53 04.9     23.5     ~ 23 0
26 M 100 AGN 12 22 54.9299993592 +15 49 20.296257960 10.04 10.05 9.35     ~ 1963 2
27 NGC 5223 rG 13 34 25.2195138072 +34 41 25.536446520   14.4       ~ 48 0
28 NGC 5253 rG 13 39 55.990 -31 38 24.11 11.48 10.94 10.49 10.33 13.47 ~ 1421 4
29 * alf Gru PM* 22 08 13.98473 -46 57 39.5078 1.11 1.58 1.71 1.75 1.83 B6V 311 0
30 * tau Aqr * 22 49 35.5009802675 -13 35 33.462758173 7.51 5.57 3.98 2.79 1.84 M0III 88 0
31 * alf Peg PM* 23 04 45.65345 +15 12 18.9617 2.38 2.44 2.48 2.47 2.50 A0IV 367 0
32 * iot Gru SB* 23 10 21.5282650093 -45 14 48.154088232   4.877 3.877     K1III 82 0
33 [BMS2012] M5 SFR 23 16 10.48 -42 35 02.3           ~ 2 0
34 [BMS2012] M6 SFR 23 16 10.49 -42 35 06.1           ~ 2 0
35 [BMS2012] M4 SFR 23 16 10.56 -42 35 01.8           ~ 2 0
36 [BMS2012] M3 SFR 23 16 10.57 -42 35 02.6           ~ 2 0
37 NGC 7552 Sy1 23 16 10.66 -42 35 04.7 11.34 11.22 10.57 10.08 11.1 ~ 574 3
38 [BMS2012] M2 SFR 23 16 10.67 -42 35 01.8           ~ 2 0
39 [BMS2012] M1 SFR 23 16 10.74 -42 35 01.6           ~ 2 0
40 [BMS2012] M9 SFR 23 16 10.84 -42 35 03.4           ~ 2 0
41 [BMS2012] M7 SFR 23 16 10.85 -42 35 06.7           ~ 2 0
42 [BMS2012] M8 SFR 23 16 10.94 -42 35 04.8           ~ 2 0
43 [ATB2004] C2 Cl* ~ ~           ~ 8 0

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