ALMA-IMF: III. Investigating the origin of stellar masses: Top-heavy core mass function in the W43-MM2&MM3 mini-starburst

Autores
Pouteau, Y.; Motte, F.; Nony, T.; Galván Madrid, R.; Menashchikov, A.; Bontemps, Sophie; Robitaille, J. F.; Louvet, F.; Ginsburg, A.; Herpin, F.; López Sepulcre, A.; DellâOva, P.; Gusdorf, A.; Sanhueza, P.; Stutz, A. M.; Brouillet, N.; Thomasson, B.; Armante, M.; Baug, T.; Bonfand, M.; Busquet, G.; Csengeri, T.; Cunningham, N.; Fernandez Lopez, Manuel; Liu, H. L.; Olguin, F.; Towner, A. P. M.; Bally, J.; Braine, J.; Bronfman, L.
Año de publicación
2022
Idioma
inglés
Tipo de recurso
artículo
Estado
versión publicada
Descripción
Aims. The processes that determine the stellar initial mass function (IMF) and its origin are critical unsolved problems, with profound implications for many areas of astrophysics. The W43-MM2&MM3 mini-starburst ridge hosts a rich young protocluster, from which it is possible to test the current paradigm on the IMF origin. Methods. The ALMA-IMF Large Program observed the W43-MM2&MM3 ridge, whose 1.3 mm and 3 mm ALMA 12 m array continuum images reach a ∼2500 au spatial resolution.We used both the best-sensitivity and the line-free ALMA-IMF images, reduced the noise with the multi-resolution segmentation technique MnGSeg, and derived the most complete and most robust core catalog possible. Using two different extraction software packages, getsf and GExt2D, we identified ∼200 compact sources, whose ∼100 common sources have, on average, fluxes consistent to within 30%. We filtered sources with non-negligible free-free contamination and corrected fluxes from line contamination, resulting in a W43-MM2&MM3 catalog of 205 getsf cores.With a median deconvolved FWHM size of 3400 au, core masses range from ∼0.1 M to ∼70 M⊙ and the getsf catalog is 90% complete down to 0:8 M⊙. Results. The high-mass end of the core mass function (CMF) of W43-MM2&MM3 is top-heavy compared to the canonical IMF. Fitting the cumulative CMF with a single power-law of the form N(> log M) / M⊙, we measured α = -0:95 ± 0:04, compared to the canonical α = -1:35 Salpeter IMF slope. The slope of the CMF is robust with respect to map processing, extraction software packages, and reasonable variations in the assumptions taken to estimate core masses.We explore several assumptions on how cores transfer their mass to stars (assuming a mass conversion efficiency) and subfragment (defining a core fragment mass function) to predict the IMF resulting from the W43-MM2&MM3 CMF. While core mass growth should flatten the high-mass end of the resulting IMF, core fragmentation could steepen it. Conclusions. In stark contrast to the commonly accepted paradigm, our result argues against the universality of the CMF shape. More robust functions of the star formation efficiency and core subfragmentation are required to better predict the resulting IMF, here suggested to remain top-heavy at the end of the star formation phase. If confirmed, the IMFs emerging from starburst events could inherit their top-heavy shape from their parental CMFs, challenging the IMF universality.
Fil: Pouteau, Y.. Universite Grenoble Alpes; Francia
Fil: Motte, F.. Universite Grenoble Alpes; Francia
Fil: Nony, T.. Universidad Nacional Autónoma de México; México
Fil: Galván Madrid, R.. Universidad Nacional Autónoma de México; México
Fil: Menashchikov, A.. Universite Paris-Saclay; . Université Paris Diderot - Paris 7; Francia
Fil: Bontemps, Sophie. Universite de Bordeaux; Francia
Fil: Robitaille, J. F.. Universite Grenoble Alpes; Francia
Fil: Louvet, F.. Universidad de Chile; Chile. Universite Grenoble Alpes; Francia
Fil: Ginsburg, A.. University of Florida; Estados Unidos
Fil: Herpin, F.. Universite de Bordeaux; Francia
Fil: López Sepulcre, A.. Iram Institut de Radioastronomie Millimétrique; Francia. Universite Grenoble Alpes; Francia
Fil: DellâOva, P.. Centre National de la Recherche Scientifique. Observatoire de Paris; Francia. Ecole Normale Supérieure; Francia
Fil: Gusdorf, A.. Ecole Normale Supérieure; Francia. Centre National de la Recherche Scientifique. Observatoire de Paris; Francia
Fil: Sanhueza, P.. National Institutes Of Natural Sciences; Japón. The Graduate University For Advanced Studies; Japón
Fil: Stutz, A. M.. Max Planck Institute For Astronomy; Alemania. Universidad de Concepción; Chile
Fil: Brouillet, N.. Universite de Bordeaux; Francia
Fil: Thomasson, B.. Universite Grenoble Alpes; Francia
Fil: Armante, M.. Centre National de la Recherche Scientifique. Observatoire de Paris; Francia. Ecole Normale Supérieure; Francia
Fil: Baug, T.. S N Bose National Centre For Basic Science; India
Fil: Bonfand, M.. Universite de Bordeaux; Francia
Fil: Busquet, G.. Universite Grenoble Alpes; Francia. Universidad de Barcelona; España
Fil: Csengeri, T.. Universite de Bordeaux; Francia
Fil: Cunningham, N.. Universite Grenoble Alpes; Francia
Fil: Fernandez Lopez, Manuel. Provincia de Buenos Aires. Gobernación. Comisión de Investigaciones Científicas. Instituto Argentino de Radioastronomía. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Instituto Argentino de Radioastronomía; Argentina
Fil: Liu, H. L.. Universidad de Concepción; Chile. Yunnan University; China
Fil: Olguin, F.. National Tsing Hua University; China
Fil: Towner, A. P. M.. University of Florida; Estados Unidos
Fil: Bally, J.. State University of Colorado at Boulder; Estados Unidos
Fil: Braine, J.. Universite de Bordeaux; Francia
Fil: Bronfman, L.. Universidad de Chile; Chile
Materia
DUST
EXTINCTION
ISM: CLOUDS
MASS FUNCTION
STARS: FORMATION
STARS: LUMINOSITY FUNCTION
STARS: MASSIVE
SUBMILLIMETER: ISM
Nivel de accesibilidad
acceso abierto
Condiciones de uso
https://creativecommons.org/licenses/by/2.5/ar/
Repositorio
CONICET Digital (CONICET)
Institución
Consejo Nacional de Investigaciones Científicas y Técnicas
OAI Identificador
oai:ri.conicet.gov.ar:11336/215644

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oai_identifier_str oai:ri.conicet.gov.ar:11336/215644
network_acronym_str CONICETDig
repository_id_str 3498
network_name_str CONICET Digital (CONICET)
spelling ALMA-IMF: III. Investigating the origin of stellar masses: Top-heavy core mass function in the W43-MM2&MM3 mini-starburstPouteau, Y.Motte, F.Nony, T.Galván Madrid, R.Menashchikov, A.Bontemps, SophieRobitaille, J. F.Louvet, F.Ginsburg, A.Herpin, F.López Sepulcre, A.DellâOva, P.Gusdorf, A.Sanhueza, P.Stutz, A. M.Brouillet, N.Thomasson, B.Armante, M.Baug, T.Bonfand, M.Busquet, G.Csengeri, T.Cunningham, N.Fernandez Lopez, ManuelLiu, H. L.Olguin, F.Towner, A. P. M.Bally, J.Braine, J.Bronfman, L.DUSTEXTINCTIONISM: CLOUDSMASS FUNCTIONSTARS: FORMATIONSTARS: LUMINOSITY FUNCTIONSTARS: MASSIVESUBMILLIMETER: ISMhttps://purl.org/becyt/ford/1.3https://purl.org/becyt/ford/1Aims. The processes that determine the stellar initial mass function (IMF) and its origin are critical unsolved problems, with profound implications for many areas of astrophysics. The W43-MM2&MM3 mini-starburst ridge hosts a rich young protocluster, from which it is possible to test the current paradigm on the IMF origin. Methods. The ALMA-IMF Large Program observed the W43-MM2&MM3 ridge, whose 1.3 mm and 3 mm ALMA 12 m array continuum images reach a ∼2500 au spatial resolution.We used both the best-sensitivity and the line-free ALMA-IMF images, reduced the noise with the multi-resolution segmentation technique MnGSeg, and derived the most complete and most robust core catalog possible. Using two different extraction software packages, getsf and GExt2D, we identified ∼200 compact sources, whose ∼100 common sources have, on average, fluxes consistent to within 30%. We filtered sources with non-negligible free-free contamination and corrected fluxes from line contamination, resulting in a W43-MM2&MM3 catalog of 205 getsf cores.With a median deconvolved FWHM size of 3400 au, core masses range from ∼0.1 M to ∼70 M⊙ and the getsf catalog is 90% complete down to 0:8 M⊙. Results. The high-mass end of the core mass function (CMF) of W43-MM2&MM3 is top-heavy compared to the canonical IMF. Fitting the cumulative CMF with a single power-law of the form N(> log M) / M⊙, we measured α = -0:95 ± 0:04, compared to the canonical α = -1:35 Salpeter IMF slope. The slope of the CMF is robust with respect to map processing, extraction software packages, and reasonable variations in the assumptions taken to estimate core masses.We explore several assumptions on how cores transfer their mass to stars (assuming a mass conversion efficiency) and subfragment (defining a core fragment mass function) to predict the IMF resulting from the W43-MM2&MM3 CMF. While core mass growth should flatten the high-mass end of the resulting IMF, core fragmentation could steepen it. Conclusions. In stark contrast to the commonly accepted paradigm, our result argues against the universality of the CMF shape. More robust functions of the star formation efficiency and core subfragmentation are required to better predict the resulting IMF, here suggested to remain top-heavy at the end of the star formation phase. If confirmed, the IMFs emerging from starburst events could inherit their top-heavy shape from their parental CMFs, challenging the IMF universality.Fil: Pouteau, Y.. Universite Grenoble Alpes; FranciaFil: Motte, F.. Universite Grenoble Alpes; FranciaFil: Nony, T.. Universidad Nacional Autónoma de México; MéxicoFil: Galván Madrid, R.. Universidad Nacional Autónoma de México; MéxicoFil: Menashchikov, A.. Universite Paris-Saclay; . Université Paris Diderot - Paris 7; FranciaFil: Bontemps, Sophie. Universite de Bordeaux; FranciaFil: Robitaille, J. F.. Universite Grenoble Alpes; FranciaFil: Louvet, F.. Universidad de Chile; Chile. Universite Grenoble Alpes; FranciaFil: Ginsburg, A.. University of Florida; Estados UnidosFil: Herpin, F.. Universite de Bordeaux; FranciaFil: López Sepulcre, A.. Iram Institut de Radioastronomie Millimétrique; Francia. Universite Grenoble Alpes; FranciaFil: DellâOva, P.. Centre National de la Recherche Scientifique. Observatoire de Paris; Francia. Ecole Normale Supérieure; FranciaFil: Gusdorf, A.. Ecole Normale Supérieure; Francia. Centre National de la Recherche Scientifique. Observatoire de Paris; FranciaFil: Sanhueza, P.. National Institutes Of Natural Sciences; Japón. The Graduate University For Advanced Studies; JapónFil: Stutz, A. M.. Max Planck Institute For Astronomy; Alemania. Universidad de Concepción; ChileFil: Brouillet, N.. Universite de Bordeaux; FranciaFil: Thomasson, B.. Universite Grenoble Alpes; FranciaFil: Armante, M.. Centre National de la Recherche Scientifique. Observatoire de Paris; Francia. Ecole Normale Supérieure; FranciaFil: Baug, T.. S N Bose National Centre For Basic Science; IndiaFil: Bonfand, M.. Universite de Bordeaux; FranciaFil: Busquet, G.. Universite Grenoble Alpes; Francia. Universidad de Barcelona; EspañaFil: Csengeri, T.. Universite de Bordeaux; FranciaFil: Cunningham, N.. Universite Grenoble Alpes; FranciaFil: Fernandez Lopez, Manuel. Provincia de Buenos Aires. Gobernación. Comisión de Investigaciones Científicas. Instituto Argentino de Radioastronomía. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Instituto Argentino de Radioastronomía; ArgentinaFil: Liu, H. L.. Universidad de Concepción; Chile. Yunnan University; ChinaFil: Olguin, F.. National Tsing Hua University; ChinaFil: Towner, A. P. M.. University of Florida; Estados UnidosFil: Bally, J.. State University of Colorado at Boulder; Estados UnidosFil: Braine, J.. Universite de Bordeaux; FranciaFil: Bronfman, L.. Universidad de Chile; ChileEDP Sciences2022-08info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/215644Pouteau, Y.; Motte, F.; Nony, T.; Galván Madrid, R.; Menashchikov, A.; et al.; ALMA-IMF: III. Investigating the origin of stellar masses: Top-heavy core mass function in the W43-MM2&MM3 mini-starburst; EDP Sciences; Astronomy and Astrophysics; 664; 8-2022; 1-280004-6361CONICET DigitalCONICETenginfo:eu-repo/semantics/altIdentifier/doi/10.1051/0004-6361/202142951info:eu-repo/semantics/altIdentifier/url/https://www.aanda.org/articles/aa/full_html/2022/08/aa42951-21/aa42951-21.htmlinfo:eu-repo/semantics/altIdentifier/url/https://arxiv.org/abs/2203.03276info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2025-10-15T15:10:57Zoai:ri.conicet.gov.ar:11336/215644instacron:CONICETInstitucionalhttp://ri.conicet.gov.ar/Organismo científico-tecnológicoNo correspondehttp://ri.conicet.gov.ar/oai/requestdasensio@conicet.gov.ar; lcarlino@conicet.gov.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:34982025-10-15 15:10:57.411CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse
dc.title.none.fl_str_mv ALMA-IMF: III. Investigating the origin of stellar masses: Top-heavy core mass function in the W43-MM2&MM3 mini-starburst
title ALMA-IMF: III. Investigating the origin of stellar masses: Top-heavy core mass function in the W43-MM2&MM3 mini-starburst
spellingShingle ALMA-IMF: III. Investigating the origin of stellar masses: Top-heavy core mass function in the W43-MM2&MM3 mini-starburst
Pouteau, Y.
DUST
EXTINCTION
ISM: CLOUDS
MASS FUNCTION
STARS: FORMATION
STARS: LUMINOSITY FUNCTION
STARS: MASSIVE
SUBMILLIMETER: ISM
title_short ALMA-IMF: III. Investigating the origin of stellar masses: Top-heavy core mass function in the W43-MM2&MM3 mini-starburst
title_full ALMA-IMF: III. Investigating the origin of stellar masses: Top-heavy core mass function in the W43-MM2&MM3 mini-starburst
title_fullStr ALMA-IMF: III. Investigating the origin of stellar masses: Top-heavy core mass function in the W43-MM2&MM3 mini-starburst
title_full_unstemmed ALMA-IMF: III. Investigating the origin of stellar masses: Top-heavy core mass function in the W43-MM2&MM3 mini-starburst
title_sort ALMA-IMF: III. Investigating the origin of stellar masses: Top-heavy core mass function in the W43-MM2&MM3 mini-starburst
dc.creator.none.fl_str_mv Pouteau, Y.
Motte, F.
Nony, T.
Galván Madrid, R.
Menashchikov, A.
Bontemps, Sophie
Robitaille, J. F.
Louvet, F.
Ginsburg, A.
Herpin, F.
López Sepulcre, A.
DellâOva, P.
Gusdorf, A.
Sanhueza, P.
Stutz, A. M.
Brouillet, N.
Thomasson, B.
Armante, M.
Baug, T.
Bonfand, M.
Busquet, G.
Csengeri, T.
Cunningham, N.
Fernandez Lopez, Manuel
Liu, H. L.
Olguin, F.
Towner, A. P. M.
Bally, J.
Braine, J.
Bronfman, L.
author Pouteau, Y.
author_facet Pouteau, Y.
Motte, F.
Nony, T.
Galván Madrid, R.
Menashchikov, A.
Bontemps, Sophie
Robitaille, J. F.
Louvet, F.
Ginsburg, A.
Herpin, F.
López Sepulcre, A.
DellâOva, P.
Gusdorf, A.
Sanhueza, P.
Stutz, A. M.
Brouillet, N.
Thomasson, B.
Armante, M.
Baug, T.
Bonfand, M.
Busquet, G.
Csengeri, T.
Cunningham, N.
Fernandez Lopez, Manuel
Liu, H. L.
Olguin, F.
Towner, A. P. M.
Bally, J.
Braine, J.
Bronfman, L.
author_role author
author2 Motte, F.
Nony, T.
Galván Madrid, R.
Menashchikov, A.
Bontemps, Sophie
Robitaille, J. F.
Louvet, F.
Ginsburg, A.
Herpin, F.
López Sepulcre, A.
DellâOva, P.
Gusdorf, A.
Sanhueza, P.
Stutz, A. M.
Brouillet, N.
Thomasson, B.
Armante, M.
Baug, T.
Bonfand, M.
Busquet, G.
Csengeri, T.
Cunningham, N.
Fernandez Lopez, Manuel
Liu, H. L.
Olguin, F.
Towner, A. P. M.
Bally, J.
Braine, J.
Bronfman, L.
author2_role author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
author
dc.subject.none.fl_str_mv DUST
EXTINCTION
ISM: CLOUDS
MASS FUNCTION
STARS: FORMATION
STARS: LUMINOSITY FUNCTION
STARS: MASSIVE
SUBMILLIMETER: ISM
topic DUST
EXTINCTION
ISM: CLOUDS
MASS FUNCTION
STARS: FORMATION
STARS: LUMINOSITY FUNCTION
STARS: MASSIVE
SUBMILLIMETER: ISM
purl_subject.fl_str_mv https://purl.org/becyt/ford/1.3
https://purl.org/becyt/ford/1
dc.description.none.fl_txt_mv Aims. The processes that determine the stellar initial mass function (IMF) and its origin are critical unsolved problems, with profound implications for many areas of astrophysics. The W43-MM2&MM3 mini-starburst ridge hosts a rich young protocluster, from which it is possible to test the current paradigm on the IMF origin. Methods. The ALMA-IMF Large Program observed the W43-MM2&MM3 ridge, whose 1.3 mm and 3 mm ALMA 12 m array continuum images reach a ∼2500 au spatial resolution.We used both the best-sensitivity and the line-free ALMA-IMF images, reduced the noise with the multi-resolution segmentation technique MnGSeg, and derived the most complete and most robust core catalog possible. Using two different extraction software packages, getsf and GExt2D, we identified ∼200 compact sources, whose ∼100 common sources have, on average, fluxes consistent to within 30%. We filtered sources with non-negligible free-free contamination and corrected fluxes from line contamination, resulting in a W43-MM2&MM3 catalog of 205 getsf cores.With a median deconvolved FWHM size of 3400 au, core masses range from ∼0.1 M to ∼70 M⊙ and the getsf catalog is 90% complete down to 0:8 M⊙. Results. The high-mass end of the core mass function (CMF) of W43-MM2&MM3 is top-heavy compared to the canonical IMF. Fitting the cumulative CMF with a single power-law of the form N(> log M) / M⊙, we measured α = -0:95 ± 0:04, compared to the canonical α = -1:35 Salpeter IMF slope. The slope of the CMF is robust with respect to map processing, extraction software packages, and reasonable variations in the assumptions taken to estimate core masses.We explore several assumptions on how cores transfer their mass to stars (assuming a mass conversion efficiency) and subfragment (defining a core fragment mass function) to predict the IMF resulting from the W43-MM2&MM3 CMF. While core mass growth should flatten the high-mass end of the resulting IMF, core fragmentation could steepen it. Conclusions. In stark contrast to the commonly accepted paradigm, our result argues against the universality of the CMF shape. More robust functions of the star formation efficiency and core subfragmentation are required to better predict the resulting IMF, here suggested to remain top-heavy at the end of the star formation phase. If confirmed, the IMFs emerging from starburst events could inherit their top-heavy shape from their parental CMFs, challenging the IMF universality.
Fil: Pouteau, Y.. Universite Grenoble Alpes; Francia
Fil: Motte, F.. Universite Grenoble Alpes; Francia
Fil: Nony, T.. Universidad Nacional Autónoma de México; México
Fil: Galván Madrid, R.. Universidad Nacional Autónoma de México; México
Fil: Menashchikov, A.. Universite Paris-Saclay; . Université Paris Diderot - Paris 7; Francia
Fil: Bontemps, Sophie. Universite de Bordeaux; Francia
Fil: Robitaille, J. F.. Universite Grenoble Alpes; Francia
Fil: Louvet, F.. Universidad de Chile; Chile. Universite Grenoble Alpes; Francia
Fil: Ginsburg, A.. University of Florida; Estados Unidos
Fil: Herpin, F.. Universite de Bordeaux; Francia
Fil: López Sepulcre, A.. Iram Institut de Radioastronomie Millimétrique; Francia. Universite Grenoble Alpes; Francia
Fil: DellâOva, P.. Centre National de la Recherche Scientifique. Observatoire de Paris; Francia. Ecole Normale Supérieure; Francia
Fil: Gusdorf, A.. Ecole Normale Supérieure; Francia. Centre National de la Recherche Scientifique. Observatoire de Paris; Francia
Fil: Sanhueza, P.. National Institutes Of Natural Sciences; Japón. The Graduate University For Advanced Studies; Japón
Fil: Stutz, A. M.. Max Planck Institute For Astronomy; Alemania. Universidad de Concepción; Chile
Fil: Brouillet, N.. Universite de Bordeaux; Francia
Fil: Thomasson, B.. Universite Grenoble Alpes; Francia
Fil: Armante, M.. Centre National de la Recherche Scientifique. Observatoire de Paris; Francia. Ecole Normale Supérieure; Francia
Fil: Baug, T.. S N Bose National Centre For Basic Science; India
Fil: Bonfand, M.. Universite de Bordeaux; Francia
Fil: Busquet, G.. Universite Grenoble Alpes; Francia. Universidad de Barcelona; España
Fil: Csengeri, T.. Universite de Bordeaux; Francia
Fil: Cunningham, N.. Universite Grenoble Alpes; Francia
Fil: Fernandez Lopez, Manuel. Provincia de Buenos Aires. Gobernación. Comisión de Investigaciones Científicas. Instituto Argentino de Radioastronomía. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Instituto Argentino de Radioastronomía; Argentina
Fil: Liu, H. L.. Universidad de Concepción; Chile. Yunnan University; China
Fil: Olguin, F.. National Tsing Hua University; China
Fil: Towner, A. P. M.. University of Florida; Estados Unidos
Fil: Bally, J.. State University of Colorado at Boulder; Estados Unidos
Fil: Braine, J.. Universite de Bordeaux; Francia
Fil: Bronfman, L.. Universidad de Chile; Chile
description Aims. The processes that determine the stellar initial mass function (IMF) and its origin are critical unsolved problems, with profound implications for many areas of astrophysics. The W43-MM2&MM3 mini-starburst ridge hosts a rich young protocluster, from which it is possible to test the current paradigm on the IMF origin. Methods. The ALMA-IMF Large Program observed the W43-MM2&MM3 ridge, whose 1.3 mm and 3 mm ALMA 12 m array continuum images reach a ∼2500 au spatial resolution.We used both the best-sensitivity and the line-free ALMA-IMF images, reduced the noise with the multi-resolution segmentation technique MnGSeg, and derived the most complete and most robust core catalog possible. Using two different extraction software packages, getsf and GExt2D, we identified ∼200 compact sources, whose ∼100 common sources have, on average, fluxes consistent to within 30%. We filtered sources with non-negligible free-free contamination and corrected fluxes from line contamination, resulting in a W43-MM2&MM3 catalog of 205 getsf cores.With a median deconvolved FWHM size of 3400 au, core masses range from ∼0.1 M to ∼70 M⊙ and the getsf catalog is 90% complete down to 0:8 M⊙. Results. The high-mass end of the core mass function (CMF) of W43-MM2&MM3 is top-heavy compared to the canonical IMF. Fitting the cumulative CMF with a single power-law of the form N(> log M) / M⊙, we measured α = -0:95 ± 0:04, compared to the canonical α = -1:35 Salpeter IMF slope. The slope of the CMF is robust with respect to map processing, extraction software packages, and reasonable variations in the assumptions taken to estimate core masses.We explore several assumptions on how cores transfer their mass to stars (assuming a mass conversion efficiency) and subfragment (defining a core fragment mass function) to predict the IMF resulting from the W43-MM2&MM3 CMF. While core mass growth should flatten the high-mass end of the resulting IMF, core fragmentation could steepen it. Conclusions. In stark contrast to the commonly accepted paradigm, our result argues against the universality of the CMF shape. More robust functions of the star formation efficiency and core subfragmentation are required to better predict the resulting IMF, here suggested to remain top-heavy at the end of the star formation phase. If confirmed, the IMFs emerging from starburst events could inherit their top-heavy shape from their parental CMFs, challenging the IMF universality.
publishDate 2022
dc.date.none.fl_str_mv 2022-08
dc.type.none.fl_str_mv info:eu-repo/semantics/article
info:eu-repo/semantics/publishedVersion
http://purl.org/coar/resource_type/c_6501
info:ar-repo/semantics/articulo
format article
status_str publishedVersion
dc.identifier.none.fl_str_mv http://hdl.handle.net/11336/215644
Pouteau, Y.; Motte, F.; Nony, T.; Galván Madrid, R.; Menashchikov, A.; et al.; ALMA-IMF: III. Investigating the origin of stellar masses: Top-heavy core mass function in the W43-MM2&MM3 mini-starburst; EDP Sciences; Astronomy and Astrophysics; 664; 8-2022; 1-28
0004-6361
CONICET Digital
CONICET
url http://hdl.handle.net/11336/215644
identifier_str_mv Pouteau, Y.; Motte, F.; Nony, T.; Galván Madrid, R.; Menashchikov, A.; et al.; ALMA-IMF: III. Investigating the origin of stellar masses: Top-heavy core mass function in the W43-MM2&MM3 mini-starburst; EDP Sciences; Astronomy and Astrophysics; 664; 8-2022; 1-28
0004-6361
CONICET Digital
CONICET
dc.language.none.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv info:eu-repo/semantics/altIdentifier/doi/10.1051/0004-6361/202142951
info:eu-repo/semantics/altIdentifier/url/https://www.aanda.org/articles/aa/full_html/2022/08/aa42951-21/aa42951-21.html
info:eu-repo/semantics/altIdentifier/url/https://arxiv.org/abs/2203.03276
dc.rights.none.fl_str_mv info:eu-repo/semantics/openAccess
https://creativecommons.org/licenses/by/2.5/ar/
eu_rights_str_mv openAccess
rights_invalid_str_mv https://creativecommons.org/licenses/by/2.5/ar/
dc.format.none.fl_str_mv application/pdf
application/pdf
dc.publisher.none.fl_str_mv EDP Sciences
publisher.none.fl_str_mv EDP Sciences
dc.source.none.fl_str_mv reponame:CONICET Digital (CONICET)
instname:Consejo Nacional de Investigaciones Científicas y Técnicas
reponame_str CONICET Digital (CONICET)
collection CONICET Digital (CONICET)
instname_str Consejo Nacional de Investigaciones Científicas y Técnicas
repository.name.fl_str_mv CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicas
repository.mail.fl_str_mv dasensio@conicet.gov.ar; lcarlino@conicet.gov.ar
_version_ 1846083257841483776
score 13.22299