2024AJ....168...33O


Query : 2024AJ....168...33O

2024AJ....168...33O - Astron. J., 168, 33 (2024/July-0)

Stellar Population near NGC 2021: Procession of Star Formation in the South Rim of Supergiant Shell LMC 4.

OU P.-S., CHAO R.-C., CHU Y.-H., HSU C.-Y. and LI C.-J.

Abstract (from CDS):

Supergiant shells (SGSs) are the largest interstellar structures where heated and enriched gas flows into the host galaxy's halo. The SGSs in the Large Magellanic Cloud (LMC) are so close that their stars can be resolved with ground-based telescopes to allow studies of star-formation history. Aiming to study the star formation history and energy budget of LMC 4, we have conducted a pilot study of the cluster NGC 2021 and the OB associations in its vicinity near the south rim of LMC 4. We use the Magellanic Cloud Photometric Survey data of the LMC to establish a methodology to examine the stellar population and assess the massive star formation history. We find a radial procession of massive star formation from the northwest part of the OB association LH79 through NGC 2021 to the OB association LH78 in the south. Using the stellar content of NGC 2021 and the assumption of Salpeter's initial mass function, we estimate that ∼4 supernovae have occurred in NGC 2021, injecting at least 4 × 1051 erg of kinetic energy into the interior of LMC 4.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Large Magellanic Cloud - Magellanic Clouds - Star formation - Stellar populations

Simbad objects: 6

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Number of rows : 6
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 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
2 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
3 NAME LMC 4 Supergiant Shell sh 05 31 33 -66 40.5           ~ 183 0
4 NGC 2011 Cl* 05 32 19 -67 31.3   10.62 10.58     ~ 74 0
5 KMHK 1059 Cl* 05 33 18.1 -67 31 20   10.28 10.19     ~ 18 0
6 NGC 2021 As* 05 33 30.170 -67 27 18.31     12.06     ~ 28 0

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