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The Core Mass Function in the Orion Nebula Cluster Region: What Determines the Final Stellar Masses?

Authors :
John M. Carpenter
Peter Schilke
Thushara Pillai
Fumitaka Nakamura
Álvaro Sánchez-Monge
John Bally
Andrea Isella
Shuo Kong
Jaime E. Pineda
Dariusz C. Lis
Ryohei Kawabe
Blakesley Burkhart
Doyal A. Harper
Yoshito Shimajiri
Ralf S. Klessen
Volker Ossenkopf-Okada
Rowan J. Smith
Shun Ishii
Steve Mairs
Héctor G. Arce
Takashi Tsukagoshi
Paul F. Goldsmith
How-Huan Chen
Adam Ginsberg
Hideaki Takemura
Paolo Padoan
Alyssa A. Goodman
Patricio Sanhueza
Rachel Friesen
Kazuhito Dobashi
Tomomi Shimoikura
Jens Kauffmann
Japan Society for the Promotion of Science
German Research Foundation
Ministerio de Economía y Competitividad (España)
Ministerio de Ciencia, Innovación y Universidades (España)
National Science Foundation (US)
Max Planck Society
Source :
Digital.CSIC. Repositorio Institucional del CSIC, instname, ApJL
Publication Year :
2021
Publisher :
arXiv, 2021.

Abstract

Takemura, H., et al.<br />Applying dendrogram analysis to the CARMA-NRO C18O (J = 1-0) data having an angular resolution of ∼8″, we identified 692 dense cores in the Orion Nebula Cluster region. Using this core sample, we compare the core and initial stellar mass functions in the same area to quantify the step from cores to stars. About 22% of the identified cores are gravitationally bound. The derived core mass function (CMF) for starless cores has a slope similar to Salpeter's stellar initial mass function (IMF) for the mass range above 1 M o˙, consistent with previous studies. Our CMF has a peak at a subsolar mass of ∼0.1 M o˙, which is comparable to the peak mass of the IMF derived in the same area. We also find that the current star formation rate is consistent with the picture in which stars are born only from self-gravitating starless cores. However, the cores must gain additional gas from the surroundings to reproduce the current IMF (e.g., its slope and peak mass), because the core mass cannot be accreted onto the star with 100% efficiency. Thus, the mass accretion from the surroundings may play a crucial role in determining the final stellar masses of stars.<br />P.S. was partially supported by a Grant-in-Aid for Scientific Research (KAKENHI Number 18H01259) of Japan Society for the Promotion of Science (JSPS). R.S.K. acknowledges financial support from the DFG via the collaborative research center (SFB 881, Project-ID 138713538) “The Milky Way System” (subprojects A1, B1, B2, and B8). He is also thankful for subsidies from the Heidelberg Cluster of Excellence STRUCTURES in the framework of Germanyʼs Excellence Strategy (grant EXC-2181/1-390900948) and for funding from the European Research Council (ERC) via the ERC Synergy Grant ECOGAL (grant 855130). P.P. acknowledges support by the Spanish MINECO under project AYA2017- 88754-P, and financial support from the State Agency for Research of the Spanish Ministry of Science and Innovation through the “Unit of Excellence María de Maeztu 2020-2023” award to the Institute of Cosmos Sciences (CEX2019-000918-M). V.O., A.S.M., and P.S. were supported by the Collaborative Research Centre 956, subprojects C1, A6, and C3, funded by the Deutsche Forschungsgemeinschaft (DFG), project ID 184018867. T.G.S.P. gratefully acknowledges support by the National Science Foundation under grant No. AST-2009842. J.E.P. acknowledges the support by the Max Planck Society. We thank the anonymous referee for many useful comments that have improved the presentation

Details

Database :
OpenAIRE
Journal :
Digital.CSIC. Repositorio Institucional del CSIC, instname, ApJL
Accession number :
edsair.doi.dedup.....af05abdc363c2fb7b362dc8f1f83dfbc
Full Text :
https://doi.org/10.48550/arxiv.2103.08527