Inversely synthesizing the core mass function of high-mass star-forming regions from the canonical initial mass function

Many studies have revealed that the core mass function (CMF) in high-mass star-forming regions is top-heavy. In this work, we start from the canonical initial mass function (IMF) to inversely synthesize the observed CMFs of high-mass star formation regions, taking into account variations in multiplicity and mass conversion efficiency from core to star ( ϵ core ). To match the observed CMFs, cores of different masses should have varying ϵ core , with ϵ core increasing as the core mass decreases. However, the multiplicity fraction does not affect the synthesized CMFs. To accurately fit the high-mass end of the CMF, it is essential to determine whether the CMF shows a slope transition from the low-mass end to the high-mass one. If the CMF truly undergoes a slope transition but observational biases obscure it, leading to a combined fit with a shallower slope, this could artificially create a top-heavy CMF.

Authors

Publication Details

Journal
Astronomy and Astrophysics
Published
2025-03-01
DOI
https://doi.org/10.1051/0004-6361/202452924
Citations
1
Primary Topic
Astrophysics and Star Formation Studies
Type
article
Field-Weighted Citation Impact
1.15
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article

Inversely synthesizing the core mass function of high-mass star-forming regions from the canonical initial mass function

Pavel Kroupa, Sami Dib, Jianwen Zhou
1 citations
Astronomy and Astrophysics
Astrophysics and Star Formation Studies
1.15
article

Inversely synthesizing the core mass function of high-mass star-forming regions from the canonical initial mass function

Pavel Kroupa, Sami Dib, Jianwen Zhou
article en
1 citations

Abstract

Many studies have revealed that the core mass function (CMF) in high-mass star-forming regions is top-heavy. In this work, we start from the canonical initial mass function (IMF) to inversely synthesize the observed CMFs of high-mass star formation regions, taking into account variations in multiplicity and mass conversion efficiency from core to star ( ϵ core ). To match the observed CMFs, cores of different masses should have varying ϵ core , with ϵ core increasing as the core mass decreases. However, the multiplicity fraction does not affect the synthesized CMFs. To accurately fit the high-mass end of the CMF, it is essential to determine whether the CMF shows a slope transition from the low-mass end to the high-mass one. If the CMF truly undergoes a slope transition but observational biases obscure it, leading to a combined fit with a shallower slope, this could artificially create a top-heavy CMF.

Astronomy and AstrophysicsVol. 695
Openalex Percentile: Top 21%
Astrophysics and Star Formation Studies
1.15
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