CARMA-NRO Orion Survey: unbiased survey of dense cores and core mass functions in Orion A
The mass distribution of dense cores is a potential key to understand the process of star formation. Applying dendrogram analysis to the CARMA-NRO Orion C\(^{18}\)O (\(J\)=1--0) data, we identify 2342 dense cores, about 22 \% of which have virial ratios smaller than 2, and can be classified as gravi...
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creator | Takemura, Hideaki Nakamura, Fumitaka Arce, Héctor G Schneider, Nicola Ossenkopf-Okada, Volker Kong, Shuo Ishii, Shun Dobashi, Kazuhito Shimoikura, Tomomi Sanhueza, Patricio Tsukagoshi, Takashi Padoan, Paolo Klessen, Ralf S Goldsmith, Paul F Burkhart, Blakesley Dariusz C Lis Álvaro Sánchez-Monge Shimajiri, Yoshito Kawabe, Ryohei |
description | The mass distribution of dense cores is a potential key to understand the process of star formation. Applying dendrogram analysis to the CARMA-NRO Orion C\(^{18}\)O (\(J\)=1--0) data, we identify 2342 dense cores, about 22 \% of which have virial ratios smaller than 2, and can be classified as gravitationally bound cores. The derived core mass function (CMF) for bound starless cores which are not associate with protostars has a slope similar to Salpeter's initial mass function (IMF) for the mass range above 1 \(M_\odot\), with a peak at \(\sim\) 0.1 \(M_\odot\). We divide the cloud into four parts based on the declination, OMC-1/2/3, OMC-4/5, L1641N/V380 Ori, and L1641C, and derive the CMFs in these regions. We find that starless cores with masses greater than 10 \(M_\odot\) exist only in OMC-1/2/3, whereas the CMFs in OMC-4/5, L1641N, and L1641C are truncated at around 5--10 \(M_\odot\). From the number ratio of bound starless cores and Class II objects in each subregion, the lifetime of bound starless cores is estimated to be 5--30 free-fall times, consistent with previous studies for other regions. In addition, we discuss core growth by mass accretion from the surrounding cloud material to explain the coincidence of peak masses between IMFs and CMFs. The mass accretion rate required for doubling the core mass within a core lifetime is larger than that of Bondi-Hoyle accretion by a factor of order 2. This implies that more dynamical accretion processes are required to grow cores. |
doi_str_mv | 10.48550/arxiv.2211.10215 |
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Applying dendrogram analysis to the CARMA-NRO Orion C\(^{18}\)O (\(J\)=1--0) data, we identify 2342 dense cores, about 22 \% of which have virial ratios smaller than 2, and can be classified as gravitationally bound cores. The derived core mass function (CMF) for bound starless cores which are not associate with protostars has a slope similar to Salpeter's initial mass function (IMF) for the mass range above 1 \(M_\odot\), with a peak at \(\sim\) 0.1 \(M_\odot\). We divide the cloud into four parts based on the declination, OMC-1/2/3, OMC-4/5, L1641N/V380 Ori, and L1641C, and derive the CMFs in these regions. We find that starless cores with masses greater than 10 \(M_\odot\) exist only in OMC-1/2/3, whereas the CMFs in OMC-4/5, L1641N, and L1641C are truncated at around 5--10 \(M_\odot\). From the number ratio of bound starless cores and Class II objects in each subregion, the lifetime of bound starless cores is estimated to be 5--30 free-fall times, consistent with previous studies for other regions. In addition, we discuss core growth by mass accretion from the surrounding cloud material to explain the coincidence of peak masses between IMFs and CMFs. The mass accretion rate required for doubling the core mass within a core lifetime is larger than that of Bondi-Hoyle accretion by a factor of order 2. This implies that more dynamical accretion processes are required to grow cores.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.2211.10215</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Declination ; Deposition ; Initial mass function ; Mass distribution ; Physics - Astrophysics of Galaxies ; Physics - Solar and Stellar Astrophysics ; Protostars ; Star & galaxy formation ; Star formation</subject><ispartof>arXiv.org, 2022-11</ispartof><rights>2022. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,784,885,27925</link.rule.ids><backlink>$$Uhttps://doi.org/10.3847/1538-4365/aca4d4$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.48550/arXiv.2211.10215$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Takemura, Hideaki</creatorcontrib><creatorcontrib>Nakamura, Fumitaka</creatorcontrib><creatorcontrib>Arce, Héctor G</creatorcontrib><creatorcontrib>Schneider, Nicola</creatorcontrib><creatorcontrib>Ossenkopf-Okada, Volker</creatorcontrib><creatorcontrib>Kong, Shuo</creatorcontrib><creatorcontrib>Ishii, Shun</creatorcontrib><creatorcontrib>Dobashi, Kazuhito</creatorcontrib><creatorcontrib>Shimoikura, Tomomi</creatorcontrib><creatorcontrib>Sanhueza, Patricio</creatorcontrib><creatorcontrib>Tsukagoshi, Takashi</creatorcontrib><creatorcontrib>Padoan, Paolo</creatorcontrib><creatorcontrib>Klessen, Ralf S</creatorcontrib><creatorcontrib>Goldsmith, Paul F</creatorcontrib><creatorcontrib>Burkhart, Blakesley</creatorcontrib><creatorcontrib>Dariusz C Lis Álvaro Sánchez-Monge</creatorcontrib><creatorcontrib>Shimajiri, Yoshito</creatorcontrib><creatorcontrib>Kawabe, Ryohei</creatorcontrib><title>CARMA-NRO Orion Survey: unbiased survey of dense cores and core mass functions in Orion A</title><title>arXiv.org</title><description>The mass distribution of dense cores is a potential key to understand the process of star formation. Applying dendrogram analysis to the CARMA-NRO Orion C\(^{18}\)O (\(J\)=1--0) data, we identify 2342 dense cores, about 22 \% of which have virial ratios smaller than 2, and can be classified as gravitationally bound cores. The derived core mass function (CMF) for bound starless cores which are not associate with protostars has a slope similar to Salpeter's initial mass function (IMF) for the mass range above 1 \(M_\odot\), with a peak at \(\sim\) 0.1 \(M_\odot\). We divide the cloud into four parts based on the declination, OMC-1/2/3, OMC-4/5, L1641N/V380 Ori, and L1641C, and derive the CMFs in these regions. We find that starless cores with masses greater than 10 \(M_\odot\) exist only in OMC-1/2/3, whereas the CMFs in OMC-4/5, L1641N, and L1641C are truncated at around 5--10 \(M_\odot\). From the number ratio of bound starless cores and Class II objects in each subregion, the lifetime of bound starless cores is estimated to be 5--30 free-fall times, consistent with previous studies for other regions. In addition, we discuss core growth by mass accretion from the surrounding cloud material to explain the coincidence of peak masses between IMFs and CMFs. The mass accretion rate required for doubling the core mass within a core lifetime is larger than that of Bondi-Hoyle accretion by a factor of order 2. This implies that more dynamical accretion processes are required to grow cores.</description><subject>Declination</subject><subject>Deposition</subject><subject>Initial mass function</subject><subject>Mass distribution</subject><subject>Physics - Astrophysics of Galaxies</subject><subject>Physics - Solar and Stellar Astrophysics</subject><subject>Protostars</subject><subject>Star & galaxy formation</subject><subject>Star formation</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GOX</sourceid><recordid>eNotj8FKw0AQhhdBsNQ-gCcXPKfOzu5mE2-hqBWqhdqLpzDNbiDFbupuU-zbG9OeZhi-_2c-xu4ETFWmNTxS-G2OU0QhpgJQ6Cs2QilFkinEGzaJcQsAmBrUWo7Y16xYvRfJx2rJl6FpPf_swtGdnnjnNw1FZ3kcDrytuXU-Ol61wUVO3g4b31GMvO58dejTkTf-0lPcsuuavqObXOaYrV-e17N5sli-vs2KRUK51kmVV6rSRtZkU5sSihoqa3JymsioVFqrrFZObFIt0CoE0A4dGA0uzakHxuz-XDt4l_vQ7Cicyn__cvDviYczsQ_tT-fiody2XfD9TyUamRlACZn8A9EuXFg</recordid><startdate>20221121</startdate><enddate>20221121</enddate><creator>Takemura, Hideaki</creator><creator>Nakamura, Fumitaka</creator><creator>Arce, Héctor G</creator><creator>Schneider, Nicola</creator><creator>Ossenkopf-Okada, Volker</creator><creator>Kong, Shuo</creator><creator>Ishii, Shun</creator><creator>Dobashi, Kazuhito</creator><creator>Shimoikura, Tomomi</creator><creator>Sanhueza, Patricio</creator><creator>Tsukagoshi, Takashi</creator><creator>Padoan, Paolo</creator><creator>Klessen, Ralf S</creator><creator>Goldsmith, Paul F</creator><creator>Burkhart, Blakesley</creator><creator>Dariusz C Lis Álvaro Sánchez-Monge</creator><creator>Shimajiri, Yoshito</creator><creator>Kawabe, Ryohei</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20221121</creationdate><title>CARMA-NRO Orion Survey: unbiased survey of dense cores and core mass functions in Orion A</title><author>Takemura, Hideaki ; 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Applying dendrogram analysis to the CARMA-NRO Orion C\(^{18}\)O (\(J\)=1--0) data, we identify 2342 dense cores, about 22 \% of which have virial ratios smaller than 2, and can be classified as gravitationally bound cores. The derived core mass function (CMF) for bound starless cores which are not associate with protostars has a slope similar to Salpeter's initial mass function (IMF) for the mass range above 1 \(M_\odot\), with a peak at \(\sim\) 0.1 \(M_\odot\). We divide the cloud into four parts based on the declination, OMC-1/2/3, OMC-4/5, L1641N/V380 Ori, and L1641C, and derive the CMFs in these regions. We find that starless cores with masses greater than 10 \(M_\odot\) exist only in OMC-1/2/3, whereas the CMFs in OMC-4/5, L1641N, and L1641C are truncated at around 5--10 \(M_\odot\). From the number ratio of bound starless cores and Class II objects in each subregion, the lifetime of bound starless cores is estimated to be 5--30 free-fall times, consistent with previous studies for other regions. In addition, we discuss core growth by mass accretion from the surrounding cloud material to explain the coincidence of peak masses between IMFs and CMFs. The mass accretion rate required for doubling the core mass within a core lifetime is larger than that of Bondi-Hoyle accretion by a factor of order 2. This implies that more dynamical accretion processes are required to grow cores.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.2211.10215</doi><oa>free_for_read</oa></addata></record> |
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subjects | Declination Deposition Initial mass function Mass distribution Physics - Astrophysics of Galaxies Physics - Solar and Stellar Astrophysics Protostars Star & galaxy formation Star formation |
title | CARMA-NRO Orion Survey: unbiased survey of dense cores and core mass functions in Orion A |
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