Impact of the cosmic background radiation on the initial mass function of metal-poor stars

ABSTRACT We study star cluster formation at low metallicities of Z/Z⊙ = 10−4–10−1 using three-dimensional hydrodynamics simulations. Particular emphasis is put on how the stellar mass distribution is affected by the cosmic microwave background radiation (CMB), which sets the temperature floor to the...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Monthly notices of the Royal Astronomical Society 2022-07, Vol.514 (3), p.4639-4654
Hauptverfasser: Chon, Sunmyon, Ono, Haruka, Omukai, Kazuyuki, Schneider, Raffaella
Format: Artikel
Sprache:eng
Online-Zugang:Volltext bestellen
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page 4654
container_issue 3
container_start_page 4639
container_title Monthly notices of the Royal Astronomical Society
container_volume 514
creator Chon, Sunmyon
Ono, Haruka
Omukai, Kazuyuki
Schneider, Raffaella
description ABSTRACT We study star cluster formation at low metallicities of Z/Z⊙ = 10−4–10−1 using three-dimensional hydrodynamics simulations. Particular emphasis is put on how the stellar mass distribution is affected by the cosmic microwave background radiation (CMB), which sets the temperature floor to the gas. Starting from the collapse of a turbulent cloud, we follow the formation of a protostellar system resolving ∼au scale. In relatively metal-enriched cases of Z/Z⊙ ≳ 10−2, where the mass function resembles the present-day one in the absence of CMB, high-temperature CMB suppresses cloud fragmentation and reduces the number of low-mass stars, making the mass function more top-heavy than in the cases without CMB heating at z ≳ 10. In lower-metallicity cases with Z/Z⊙ ≲ 10−3, where the gas temperature is higher than the CMB value due to inefficient cooling, the CMB has only a minor impact on the mass distribution, which is top-heavy, regardless of the redshift. In cases either with a low metallicity of Z/Z⊙ ≲ 10−2 or at a high redshift z ≳ 10, the mass spectrum consists of a low-mass Salpeter-like component, peaking at 0.1 M⊙, and a top-heavy component with 10–50 M⊙, with the fraction in the latter increasing with increasing redshift. In galaxies forming at z ≳ 10, the major targets of the future instruments including JWST, CMB heating makes the stellar mass function significantly top-heavy, enhancing the number of supernova explosions by a factor of 1.4 (2.8) at z = 10 (20, respectively) compared to the prediction by Chabrier initial mass function when Z/Z⊙ = 0.1.
doi_str_mv 10.1093/mnras/stac1549
format Article
fullrecord <record><control><sourceid>oup_TOX</sourceid><recordid>TN_cdi_crossref_primary_10_1093_mnras_stac1549</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><oup_id>10.1093/mnras/stac1549</oup_id><sourcerecordid>10.1093/mnras/stac1549</sourcerecordid><originalsourceid>FETCH-LOGICAL-c339t-453e2abbaff99e45eb8dbff679b1dbcd085179419f56d2db708dc70b059890323</originalsourceid><addsrcrecordid>eNqFkL1PwzAUxC0EEqWwMntlSPscx0k8ooqPSpVYYGGJnr_A0MSR7Q7896QEZqQn3fDuTqcfIdcMVgwkX_dDxLROGTUTlTwhC8ZrUZSyrk_JAoCLom0YOycXKX0AQMXLekFet_2IOtPgaH63VIfUe00V6s-3GA6DoRGNx-zDQKc7Wvzgs8c97TEl6g6Dnp-O9jbjvhhDiHQaEdMlOXO4T_bqV5fk5f7uefNY7J4etpvbXaE5l7moBLclKoXOSWkrYVVrlHN1IxUzShtoBWtkxaQTtSmNaqA1ugEFQrYSeMmXZDX36hhSitZ1Y_Q9xq-OQXck0_2Q6f7ITIGbORAO43_eb-KoaRA</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Impact of the cosmic background radiation on the initial mass function of metal-poor stars</title><source>Oxford Journals Open Access Collection</source><creator>Chon, Sunmyon ; Ono, Haruka ; Omukai, Kazuyuki ; Schneider, Raffaella</creator><creatorcontrib>Chon, Sunmyon ; Ono, Haruka ; Omukai, Kazuyuki ; Schneider, Raffaella</creatorcontrib><description>ABSTRACT We study star cluster formation at low metallicities of Z/Z⊙ = 10−4–10−1 using three-dimensional hydrodynamics simulations. Particular emphasis is put on how the stellar mass distribution is affected by the cosmic microwave background radiation (CMB), which sets the temperature floor to the gas. Starting from the collapse of a turbulent cloud, we follow the formation of a protostellar system resolving ∼au scale. In relatively metal-enriched cases of Z/Z⊙ ≳ 10−2, where the mass function resembles the present-day one in the absence of CMB, high-temperature CMB suppresses cloud fragmentation and reduces the number of low-mass stars, making the mass function more top-heavy than in the cases without CMB heating at z ≳ 10. In lower-metallicity cases with Z/Z⊙ ≲ 10−3, where the gas temperature is higher than the CMB value due to inefficient cooling, the CMB has only a minor impact on the mass distribution, which is top-heavy, regardless of the redshift. In cases either with a low metallicity of Z/Z⊙ ≲ 10−2 or at a high redshift z ≳ 10, the mass spectrum consists of a low-mass Salpeter-like component, peaking at 0.1 M⊙, and a top-heavy component with 10–50 M⊙, with the fraction in the latter increasing with increasing redshift. In galaxies forming at z ≳ 10, the major targets of the future instruments including JWST, CMB heating makes the stellar mass function significantly top-heavy, enhancing the number of supernova explosions by a factor of 1.4 (2.8) at z = 10 (20, respectively) compared to the prediction by Chabrier initial mass function when Z/Z⊙ = 0.1.</description><identifier>ISSN: 0035-8711</identifier><identifier>EISSN: 1365-2966</identifier><identifier>DOI: 10.1093/mnras/stac1549</identifier><language>eng</language><publisher>Oxford University Press</publisher><ispartof>Monthly notices of the Royal Astronomical Society, 2022-07, Vol.514 (3), p.4639-4654</ispartof><rights>2022 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society 2022</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c339t-453e2abbaff99e45eb8dbff679b1dbcd085179419f56d2db708dc70b059890323</citedby><cites>FETCH-LOGICAL-c339t-453e2abbaff99e45eb8dbff679b1dbcd085179419f56d2db708dc70b059890323</cites><orcidid>0000-0001-9317-2888 ; 0000-0002-2912-3923</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,1604,27923,27924</link.rule.ids><linktorsrc>$$Uhttps://dx.doi.org/10.1093/mnras/stac1549$$EView_record_in_Oxford_University_Press$$FView_record_in_$$GOxford_University_Press</linktorsrc></links><search><creatorcontrib>Chon, Sunmyon</creatorcontrib><creatorcontrib>Ono, Haruka</creatorcontrib><creatorcontrib>Omukai, Kazuyuki</creatorcontrib><creatorcontrib>Schneider, Raffaella</creatorcontrib><title>Impact of the cosmic background radiation on the initial mass function of metal-poor stars</title><title>Monthly notices of the Royal Astronomical Society</title><description>ABSTRACT We study star cluster formation at low metallicities of Z/Z⊙ = 10−4–10−1 using three-dimensional hydrodynamics simulations. Particular emphasis is put on how the stellar mass distribution is affected by the cosmic microwave background radiation (CMB), which sets the temperature floor to the gas. Starting from the collapse of a turbulent cloud, we follow the formation of a protostellar system resolving ∼au scale. In relatively metal-enriched cases of Z/Z⊙ ≳ 10−2, where the mass function resembles the present-day one in the absence of CMB, high-temperature CMB suppresses cloud fragmentation and reduces the number of low-mass stars, making the mass function more top-heavy than in the cases without CMB heating at z ≳ 10. In lower-metallicity cases with Z/Z⊙ ≲ 10−3, where the gas temperature is higher than the CMB value due to inefficient cooling, the CMB has only a minor impact on the mass distribution, which is top-heavy, regardless of the redshift. In cases either with a low metallicity of Z/Z⊙ ≲ 10−2 or at a high redshift z ≳ 10, the mass spectrum consists of a low-mass Salpeter-like component, peaking at 0.1 M⊙, and a top-heavy component with 10–50 M⊙, with the fraction in the latter increasing with increasing redshift. In galaxies forming at z ≳ 10, the major targets of the future instruments including JWST, CMB heating makes the stellar mass function significantly top-heavy, enhancing the number of supernova explosions by a factor of 1.4 (2.8) at z = 10 (20, respectively) compared to the prediction by Chabrier initial mass function when Z/Z⊙ = 0.1.</description><issn>0035-8711</issn><issn>1365-2966</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNqFkL1PwzAUxC0EEqWwMntlSPscx0k8ooqPSpVYYGGJnr_A0MSR7Q7896QEZqQn3fDuTqcfIdcMVgwkX_dDxLROGTUTlTwhC8ZrUZSyrk_JAoCLom0YOycXKX0AQMXLekFet_2IOtPgaH63VIfUe00V6s-3GA6DoRGNx-zDQKc7Wvzgs8c97TEl6g6Dnp-O9jbjvhhDiHQaEdMlOXO4T_bqV5fk5f7uefNY7J4etpvbXaE5l7moBLclKoXOSWkrYVVrlHN1IxUzShtoBWtkxaQTtSmNaqA1ugEFQrYSeMmXZDX36hhSitZ1Y_Q9xq-OQXck0_2Q6f7ITIGbORAO43_eb-KoaRA</recordid><startdate>20220708</startdate><enddate>20220708</enddate><creator>Chon, Sunmyon</creator><creator>Ono, Haruka</creator><creator>Omukai, Kazuyuki</creator><creator>Schneider, Raffaella</creator><general>Oxford University Press</general><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0001-9317-2888</orcidid><orcidid>https://orcid.org/0000-0002-2912-3923</orcidid></search><sort><creationdate>20220708</creationdate><title>Impact of the cosmic background radiation on the initial mass function of metal-poor stars</title><author>Chon, Sunmyon ; Ono, Haruka ; Omukai, Kazuyuki ; Schneider, Raffaella</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c339t-453e2abbaff99e45eb8dbff679b1dbcd085179419f56d2db708dc70b059890323</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Chon, Sunmyon</creatorcontrib><creatorcontrib>Ono, Haruka</creatorcontrib><creatorcontrib>Omukai, Kazuyuki</creatorcontrib><creatorcontrib>Schneider, Raffaella</creatorcontrib><collection>CrossRef</collection><jtitle>Monthly notices of the Royal Astronomical Society</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Chon, Sunmyon</au><au>Ono, Haruka</au><au>Omukai, Kazuyuki</au><au>Schneider, Raffaella</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Impact of the cosmic background radiation on the initial mass function of metal-poor stars</atitle><jtitle>Monthly notices of the Royal Astronomical Society</jtitle><date>2022-07-08</date><risdate>2022</risdate><volume>514</volume><issue>3</issue><spage>4639</spage><epage>4654</epage><pages>4639-4654</pages><issn>0035-8711</issn><eissn>1365-2966</eissn><abstract>ABSTRACT We study star cluster formation at low metallicities of Z/Z⊙ = 10−4–10−1 using three-dimensional hydrodynamics simulations. Particular emphasis is put on how the stellar mass distribution is affected by the cosmic microwave background radiation (CMB), which sets the temperature floor to the gas. Starting from the collapse of a turbulent cloud, we follow the formation of a protostellar system resolving ∼au scale. In relatively metal-enriched cases of Z/Z⊙ ≳ 10−2, where the mass function resembles the present-day one in the absence of CMB, high-temperature CMB suppresses cloud fragmentation and reduces the number of low-mass stars, making the mass function more top-heavy than in the cases without CMB heating at z ≳ 10. In lower-metallicity cases with Z/Z⊙ ≲ 10−3, where the gas temperature is higher than the CMB value due to inefficient cooling, the CMB has only a minor impact on the mass distribution, which is top-heavy, regardless of the redshift. In cases either with a low metallicity of Z/Z⊙ ≲ 10−2 or at a high redshift z ≳ 10, the mass spectrum consists of a low-mass Salpeter-like component, peaking at 0.1 M⊙, and a top-heavy component with 10–50 M⊙, with the fraction in the latter increasing with increasing redshift. In galaxies forming at z ≳ 10, the major targets of the future instruments including JWST, CMB heating makes the stellar mass function significantly top-heavy, enhancing the number of supernova explosions by a factor of 1.4 (2.8) at z = 10 (20, respectively) compared to the prediction by Chabrier initial mass function when Z/Z⊙ = 0.1.</abstract><pub>Oxford University Press</pub><doi>10.1093/mnras/stac1549</doi><tpages>16</tpages><orcidid>https://orcid.org/0000-0001-9317-2888</orcidid><orcidid>https://orcid.org/0000-0002-2912-3923</orcidid></addata></record>
fulltext fulltext_linktorsrc
identifier ISSN: 0035-8711
ispartof Monthly notices of the Royal Astronomical Society, 2022-07, Vol.514 (3), p.4639-4654
issn 0035-8711
1365-2966
language eng
recordid cdi_crossref_primary_10_1093_mnras_stac1549
source Oxford Journals Open Access Collection
title Impact of the cosmic background radiation on the initial mass function of metal-poor stars
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-09T02%3A48%3A41IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-oup_TOX&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Impact%20of%20the%20cosmic%20background%20radiation%20on%20the%20initial%20mass%20function%20of%20metal-poor%20stars&rft.jtitle=Monthly%20notices%20of%20the%20Royal%20Astronomical%20Society&rft.au=Chon,%20Sunmyon&rft.date=2022-07-08&rft.volume=514&rft.issue=3&rft.spage=4639&rft.epage=4654&rft.pages=4639-4654&rft.issn=0035-8711&rft.eissn=1365-2966&rft_id=info:doi/10.1093/mnras/stac1549&rft_dat=%3Coup_TOX%3E10.1093/mnras/stac1549%3C/oup_TOX%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_id=info:pmid/&rft_oup_id=10.1093/mnras/stac1549&rfr_iscdi=true