2019A&A...628A..92F


Query : 2019A&A...628A..92F

2019A&A...628A..92F - Astronomy and Astrophysics, volume 628A, 92-92 (2019/8-1)

Constraining nuclear star cluster formation using MUSE-AO observations of the early-type galaxy FCC 47.

FAHRION K., LYUBENOVA M., VAN DE VEN G., LEAMAN R., HILKER M., MARTIN-NAVARRO I., ZHU L., ALFARO-CUELLO M., COCCATO L., CORSINI E.M., FALCON-BARROSO J., IODICE E., McDERMID R.M., SARZI M. and DE ZEEUW T.

Abstract (from CDS):


Context. Nuclear star clusters (NSCs) are found in at least 70% of all galaxies, but their formation path is still unclear. In the most common scenarios, NSCs form in-situ from the galaxy's central gas reservoir, through the merging of globular clusters (GCs), or through a combination of both.
Aims. As the scenarios pose different expectations for angular momentum and stellar population properties of the NSC in comparison to the host galaxy and the GC system, it is necessary to characterise the stellar light, NSC, and GCs simultaneously. The large NSC (reff=66pc) and rich GC system of the early-type Fornax cluster galaxy FCC 47 (NGC 1336) render this galaxy an ideal laboratory to constrain NSC formation.
Methods. Using Multi Unit Spectroscopic Explorer science verification data assisted by adaptive optics, we obtained maps for the stellar kinematics and stellar-population properties of FCC 47. We extracted the spectra of the central NSC and determined line-of-sight velocities of 24 GCs and metallicities of five. Results. The galaxy shows the following kinematically decoupled components (KDCs): a disk and a NSC. Our orbit-based dynamical Schwarzschild model revealed that the NSC is a distinct kinematic feature and it constitutes the peak of metallicity and old ages in FCC 47. The main body consists of two counter-rotating populations and is dominated by a more metal-poor population. The GC system is bimodal with a dominant metal-poor population and the total GC system mass is ∼17% of the NSC mass (∼7x108M). Conclusions. The rotation, high metallicity, and high mass of the NSC cannot be explained by GC-inspiral alone. It most likely requires additional, quickly quenched, in-situ formation. The presence of two KDCs likely are evidence of a major merger that has significantly altered the structure of FCC 47, indicating the important role of galaxy mergers in forming the complex kinematics in the galaxy-NSC system.

Abstract Copyright: © ESO 2019

Journal keyword(s): galaxies: individual: NGC 1336 - galaxies: nuclei - galaxies: kinematics and dynamics - galaxies: star clusters: general

CDS comments: Table C.1 ID1 not in SIMBAD.

Simbad objects: 29

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Number of rows : 29
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 [JPB2015] 051.6219946-35.7219579 GlC 03 26 29.2787 -35 43 19.048           ~ 2 0
2 [JPB2015] 051.6243290-35.7255972 GlC 03 26 29.8592045856 -35 43 32.466096336           ~ 2 0
3 [JPB2015] 051.6245358-35.7179755 GlC 03 26 29.8886 -35 43 04.712           ~ 2 0
4 [JPB2015] 051.6251429-35.7226409 GlC 03 26 30.0549356808 -35 43 21.832858596           ~ 2 0
5 [JPB2015] 051.6261055-35.7210342 GlC 03 26 30.2653 -35 43 15.723           ~ 2 0
6 [JPB2015] 051.6266636-35.7196305 GlC 03 26 30.3993 -35 43 10.670           ~ 2 0
7 [JPB2015] 051.6284365-35.7297971 GlC 03 26 30.8248 -35 43 47.270           ~ 2 0
8 [JPB2015] 051.6304665-35.7244222 GlC 03 26 31.3120 -35 43 27.920           ~ 2 0
9 [JPB2015] 051.6311027-35.7178949 GlC 03 26 31.4646 -35 43 04.422           ~ 2 0
10 [JPB2015] 051.6313314-35.7176640 GlC 03 26 31.5195 -35 43 03.590           ~ 2 0
11 [JPB2015] 051.6326099-35.7124987 Gl? 03 26 31.8264 -35 42 44.995           ~ 2 0
12 [JPB2015] 051.6327986-35.7125745 Gl? 03 26 31.8717 -35 42 45.268           ~ 2 0
13 [JPB2015] 051.6333399-35.7121424 GlC 03 26 32.0016 -35 42 43.713           ~ 2 0
14 NGC 1336 GiG 03 26 32.1845365512 -35 42 48.662672184   13.12   11.95   ~ 128 0
15 [JPB2015] 051.6346842-35.7122640 Gl? 03 26 32.3242 -35 42 44.150           ~ 2 0
16 [JPB2015] 051.6347768-35.7123402 GlC 03 26 32.3464 -35 42 44.425           ~ 2 0
17 [JPB2015] 051.6349555-35.7190817 GlC 03 26 32.3893 -35 43 08.694           ~ 2 0
18 [JPB2015] 051.6353013-35.7250935 GlC 03 26 32.4723 -35 43 30.337           ~ 2 0
19 [JPB2015] 051.6353780-35.7206806 GlC 03 26 32.4907 -35 43 14.450           ~ 2 0
20 [FGH2019] FCC 47-UCD1 G 03 26 32.920 -35 42 56.10           ~ 3 0
21 [JPB2015] 051.6377788-35.7216483 GlC 03 26 33.0669 -35 43 17.934           ~ 2 0
22 [JPB2015] 051.6379170-35.7288359 GlC 03 26 33.1001 -35 43 43.809           ~ 2 0
23 [JPB2015] 051.6391501-35.7170935 GlC 03 26 33.4164102960 -35 43 01.879852944           ~ 2 0
24 [JPB2015] 051.6414733-35.7197915 GlC 03 26 33.9536 -35 43 11.249           ~ 2 0
25 [JPB2015] 051.6430098-35.7222389 GlC 03 26 34.3224 -35 43 20.060           ~ 2 0
26 NGC 1399 BiC 03 38 29.083 -35 27 02.67 11.05 9.74 9.59 8.12   ~ 1557 1
27 ACO S 373 ClG 03 38 29.4 -35 27 08           ~ 1781 0
28 NGC 4365 GiG 12 24 28.228 +07 19 03.07   11.5       ~ 830 0
29 M 87 AGN 12 30 49.42338414 +12 23 28.0436859 10.16 9.59 8.63   7.49 ~ 7020 3

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2023.09.29-16:14:32

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