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

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  • معلومة اضافية
    • Contributors:
      Institut de Planétologie et d'Astrophysique de Grenoble (IPAG); Centre National d'Études Spatiales Toulouse (CNES)-Centre National de la Recherche Scientifique (CNRS)-Observatoire des Sciences de l'Univers de Grenoble (OSUG ); Institut national des sciences de l'Univers (INSU - CNRS)-Université Savoie Mont Blanc (USMB Université de Savoie Université de Chambéry )-Centre National de la Recherche Scientifique (CNRS)-Institut National de Recherche pour l’Agriculture, l’Alimentation et l’Environnement (INRAE)-Université Grenoble Alpes (UGA)-Météo-France-Institut national des sciences de l'Univers (INSU - CNRS)-Université Savoie Mont Blanc (USMB Université de Savoie Université de Chambéry )-Centre National de la Recherche Scientifique (CNRS)-Institut National de Recherche pour l’Agriculture, l’Alimentation et l’Environnement (INRAE)-Université Grenoble Alpes (UGA)-Météo-France; Instituto de Radioastronomía y Astrofísica Mexico (IRyA); Universidad Nacional Autónoma de México = National Autonomous University of Mexico (UNAM); Astrophysique Interprétation Modélisation (AIM (UMR_7158 / UMR_E_9005 / UM_112)); Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Université Paris Cité (UPCité); Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU); Université Paris-Saclay-Direction de Recherche Fondamentale (CEA) (DRF (CEA)); Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA); Laboratoire d'Astrophysique de Bordeaux Pessac (LAB); Université de Bordeaux (UB)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National de la Recherche Scientifique (CNRS); Universidad de Chile = University of Chile Santiago (UCHILE); University of Florida Gainesville (UF); Institut de RadioAstronomie Millimétrique (IRAM); Centre National de la Recherche Scientifique (CNRS); Astrophysique; Laboratoire de physique de l'ENS - ENS Paris (LPENS); Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS)-Université Paris Cité (UPCité)-Département de Physique de l'ENS-PSL; École normale supérieure - Paris (ENS-PSL); Université Paris Sciences et Lettres (PSL)-Université Paris Sciences et Lettres (PSL)-École normale supérieure - Paris (ENS-PSL); Université Paris Sciences et Lettres (PSL)-Université Paris Sciences et Lettres (PSL)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS)-Université Paris Cité (UPCité)-Département de Physique de l'ENS-PSL; Université Paris Sciences et Lettres (PSL)-Université Paris Sciences et Lettres (PSL); Laboratoire d'Etude du Rayonnement et de la Matière en Astrophysique et Atmosphères = Laboratory for Studies of Radiation and Matter in Astrophysics and Atmospheres (LERMA); Université Paris Sciences et Lettres (PSL)-Université Paris Sciences et Lettres (PSL)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire de Paris; Université Paris Sciences et Lettres (PSL)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS)-CY Cergy Paris Université (CY); National Astronomical Observatory of Japan (NAOJ); Graduate University for Advanced Studies Hayama (SOKENDAI); Universidad de Concepción - University of Concepcion Chile; Max Planck Institute for Astronomy (MPIA); S. N. Bose National Centre for Basic Sciences; Institut de Ciencies del Cosmos (ICCUB); Universitat de Barcelona (UB); Instituto Argentino de Radioastronomia (IAR); Consejo Nacional de Investigaciones Científicas y Técnicas Buenos Aires (CONICET)-Science and Technology Center Mendoza, Argentina (CCT)-Comision de Investigaciones Cientificas de la Provincia de BsAs (CICPBA); Yunnan University; National Tsing Hua University Hsinchu (NTHU); Department of Astrophysical and Planetary Sciences Boulder; University of Colorado Boulder; Universitat de València (UV); Shanghai Astronomical Observatory Shanghai (SHAO); Chinese Academy of Sciences Beijing (CAS); Max Planck Institute for Radio Astronomy; University of Connecticut (UCONN); School of Physics and Astronomy Cardiff; Cardiff University; ANR-16-CE92-0035,GENESIS,GENeration et Evolution des Structures du milieu InterStellaire(2016); ANR-20-CE31-0009,COSMHIC,L'origine de la masse des étoiles dans des nuages hiérarchiques en effondrement(2020)
    • بيانات النشر:
      HAL CCSD
      EDP Sciences
    • الموضوع:
      2022
    • Collection:
      Université Savoie Mont Blanc: HAL
    • نبذة مختصرة :
      International audience ; 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) ∝ Mα, 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 ...
    • Relation:
      hal-03746157; https://hal.science/hal-03746157; https://hal.science/hal-03746157/document; https://hal.science/hal-03746157/file/aa42951-21.pdf
    • الرقم المعرف:
      10.1051/0004-6361/202142951
    • الدخول الالكتروني :
      https://hal.science/hal-03746157
      https://hal.science/hal-03746157/document
      https://hal.science/hal-03746157/file/aa42951-21.pdf
      https://doi.org/10.1051/0004-6361/202142951
    • Rights:
      info:eu-repo/semantics/OpenAccess
    • الرقم المعرف:
      edsbas.FA583EEA