ALMA CO Observations of Supernova Remnant N63A in the Large Magellanic Cloud: Discovery of Dense Molecular Clouds Embedded within Shock-ionized and Photoionized Nebulae
We carried out new 12CO(J = 1-0, 3-2) observations of a N63A supernova remnant (SNR) from the LMC using the Atacama Large Millimeter/submillimeter Array (ALMA) and Atacama Submillimeter Telescope Experiment. We find three giant molecular clouds toward the northeast, east, and near the center of the...
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Veröffentlicht in: | The Astrophysical journal 2019-03, Vol.873 (1), p.40 |
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creator | Sano, H. Matsumura, H. Nagaya, T. Yamane, Y. Alsaberi, R. Z. E. Filipovi, M. D. Tachihara, K. Fujii, K. Tokuda, K. Tsuge, K. Yoshiike, S. Onishi, T. Kawamura, A. Minamidani, T. Mizuno, N. Yamamoto, H. Inutsuka, S. Inoue, T. Maxted, N. Rowell, G. Sasaki, M. Fukui, Y. |
description | We carried out new 12CO(J = 1-0, 3-2) observations of a N63A supernova remnant (SNR) from the LMC using the Atacama Large Millimeter/submillimeter Array (ALMA) and Atacama Submillimeter Telescope Experiment. We find three giant molecular clouds toward the northeast, east, and near the center of the SNR. Using the ALMA data, we spatially resolved clumpy molecular clouds embedded within the optical nebulae in both the shock-ionized and photoionized lobes discovered by previous H and [S ii] observations. The total mass of the molecular clouds is ∼800 M☉ for the shock-ionized region and ∼1700 M☉ for the photoionized region. Spatially resolved X-ray spectroscopy reveals that the absorbing column densities toward the molecular clouds are ∼(1.5-6.0) × 1021 cm−2, which are ∼1.5-15 times less than the averaged interstellar proton column densities for each region. This means that the X-rays are produced not only behind the molecular clouds, but also in front of them. We conclude that the dense molecular clouds have been completely engulfed by the shock waves, but have still survived erosion owing to their high density and short interacting time. The X-ray spectrum toward the gas clumps is well explained by an absorbed power-law model or a high-temperature plasma model, in addition to thermal plasma components, implying that the shock-cloud interaction is efficiently working for both cases through the shock ionization and magnetic field amplification. If the hadronic gamma-ray is dominant in the GeV band, the total energy of the cosmic-ray protons is calculated to be ∼(0.3-1.4) × 1049 erg, with an estimated interstellar proton density of ∼190 90 cm−3, containing both the shock-ionized gas and neutral atomic hydrogen. |
doi_str_mv | 10.3847/1538-4357/ab02fd |
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Z. E. ; Filipovi, M. D. ; Tachihara, K. ; Fujii, K. ; Tokuda, K. ; Tsuge, K. ; Yoshiike, S. ; Onishi, T. ; Kawamura, A. ; Minamidani, T. ; Mizuno, N. ; Yamamoto, H. ; Inutsuka, S. ; Inoue, T. ; Maxted, N. ; Rowell, G. ; Sasaki, M. ; Fukui, Y.</creator><creatorcontrib>Sano, H. ; Matsumura, H. ; Nagaya, T. ; Yamane, Y. ; Alsaberi, R. Z. E. ; Filipovi, M. D. ; Tachihara, K. ; Fujii, K. ; Tokuda, K. ; Tsuge, K. ; Yoshiike, S. ; Onishi, T. ; Kawamura, A. ; Minamidani, T. ; Mizuno, N. ; Yamamoto, H. ; Inutsuka, S. ; Inoue, T. ; Maxted, N. ; Rowell, G. ; Sasaki, M. ; Fukui, Y.</creatorcontrib><description>We carried out new 12CO(J = 1-0, 3-2) observations of a N63A supernova remnant (SNR) from the LMC using the Atacama Large Millimeter/submillimeter Array (ALMA) and Atacama Submillimeter Telescope Experiment. We find three giant molecular clouds toward the northeast, east, and near the center of the SNR. Using the ALMA data, we spatially resolved clumpy molecular clouds embedded within the optical nebulae in both the shock-ionized and photoionized lobes discovered by previous H and [S ii] observations. The total mass of the molecular clouds is ∼800 M☉ for the shock-ionized region and ∼1700 M☉ for the photoionized region. Spatially resolved X-ray spectroscopy reveals that the absorbing column densities toward the molecular clouds are ∼(1.5-6.0) × 1021 cm−2, which are ∼1.5-15 times less than the averaged interstellar proton column densities for each region. This means that the X-rays are produced not only behind the molecular clouds, but also in front of them. We conclude that the dense molecular clouds have been completely engulfed by the shock waves, but have still survived erosion owing to their high density and short interacting time. The X-ray spectrum toward the gas clumps is well explained by an absorbed power-law model or a high-temperature plasma model, in addition to thermal plasma components, implying that the shock-cloud interaction is efficiently working for both cases through the shock ionization and magnetic field amplification. If the hadronic gamma-ray is dominant in the GeV band, the total energy of the cosmic-ray protons is calculated to be ∼(0.3-1.4) × 1049 erg, with an estimated interstellar proton density of ∼190 90 cm−3, containing both the shock-ionized gas and neutral atomic hydrogen.</description><identifier>ISSN: 0004-637X</identifier><identifier>EISSN: 1538-4357</identifier><identifier>DOI: 10.3847/1538-4357/ab02fd</identifier><language>eng</language><publisher>Philadelphia: The American Astronomical Society</publisher><subject>Astrophysics ; Cloud interaction ; Clouds ; Clumps ; Cosmic ray protons ; Cosmic rays ; Gamma rays ; High temperature plasmas ; Hydrogen ; Interstellar ; Ionization ; ISM: clouds ; ISM: individual objects (LHA 120-N 63A) ; ISM: supernova remnants ; Magellanic clouds ; Magnetic fields ; Molecular clouds ; Nebulae ; Photoionization ; photon-dominated region (PDR) ; Power law ; Proton density (concentration) ; Radio telescopes ; Shock waves ; Spectroscopy ; Supernova ; Supernova remnants ; Thermal plasmas ; X-ray spectra ; X-ray spectroscopy ; X-rays</subject><ispartof>The Astrophysical journal, 2019-03, Vol.873 (1), p.40</ispartof><rights>2019. The American Astronomical Society. All rights reserved.</rights><rights>Copyright IOP Publishing Mar 01, 2019</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c460t-61fea08cbf3a0296af68c34c60748accc0ee9e3509e0fe2ab2ceaa83948d6ee33</citedby><cites>FETCH-LOGICAL-c460t-61fea08cbf3a0296af68c34c60748accc0ee9e3509e0fe2ab2ceaa83948d6ee33</cites><orcidid>0000-0002-4990-9288 ; 0000-0002-2062-1600 ; 0000-0003-4366-6518 ; 0000-0001-7813-0380 ; 0000-0002-2458-7876 ; 0000-0001-5609-7372 ; 0000-0003-2762-8378 ; 0000-0001-6533-224X ; 0000-0001-9778-6692 ; 0000-0002-9516-1581 ; 0000-0001-8296-7482 ; 0000-0003-2062-5692 ; 0000-0002-1411-5410 ; 0000-0002-2794-4840 ; 0000-0001-5302-1866</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.3847/1538-4357/ab02fd/pdf$$EPDF$$P50$$Giop$$H</linktopdf><link.rule.ids>314,780,784,27924,27925,38890,53867</link.rule.ids><linktorsrc>$$Uhttps://iopscience.iop.org/article/10.3847/1538-4357/ab02fd$$EView_record_in_IOP_Publishing$$FView_record_in_$$GIOP_Publishing</linktorsrc></links><search><creatorcontrib>Sano, H.</creatorcontrib><creatorcontrib>Matsumura, H.</creatorcontrib><creatorcontrib>Nagaya, T.</creatorcontrib><creatorcontrib>Yamane, Y.</creatorcontrib><creatorcontrib>Alsaberi, R. Z. E.</creatorcontrib><creatorcontrib>Filipovi, M. D.</creatorcontrib><creatorcontrib>Tachihara, K.</creatorcontrib><creatorcontrib>Fujii, K.</creatorcontrib><creatorcontrib>Tokuda, K.</creatorcontrib><creatorcontrib>Tsuge, K.</creatorcontrib><creatorcontrib>Yoshiike, S.</creatorcontrib><creatorcontrib>Onishi, T.</creatorcontrib><creatorcontrib>Kawamura, A.</creatorcontrib><creatorcontrib>Minamidani, T.</creatorcontrib><creatorcontrib>Mizuno, N.</creatorcontrib><creatorcontrib>Yamamoto, H.</creatorcontrib><creatorcontrib>Inutsuka, S.</creatorcontrib><creatorcontrib>Inoue, T.</creatorcontrib><creatorcontrib>Maxted, N.</creatorcontrib><creatorcontrib>Rowell, G.</creatorcontrib><creatorcontrib>Sasaki, M.</creatorcontrib><creatorcontrib>Fukui, Y.</creatorcontrib><title>ALMA CO Observations of Supernova Remnant N63A in the Large Magellanic Cloud: Discovery of Dense Molecular Clouds Embedded within Shock-ionized and Photoionized Nebulae</title><title>The Astrophysical journal</title><addtitle>APJ</addtitle><addtitle>Astrophys. J</addtitle><description>We carried out new 12CO(J = 1-0, 3-2) observations of a N63A supernova remnant (SNR) from the LMC using the Atacama Large Millimeter/submillimeter Array (ALMA) and Atacama Submillimeter Telescope Experiment. We find three giant molecular clouds toward the northeast, east, and near the center of the SNR. Using the ALMA data, we spatially resolved clumpy molecular clouds embedded within the optical nebulae in both the shock-ionized and photoionized lobes discovered by previous H and [S ii] observations. The total mass of the molecular clouds is ∼800 M☉ for the shock-ionized region and ∼1700 M☉ for the photoionized region. Spatially resolved X-ray spectroscopy reveals that the absorbing column densities toward the molecular clouds are ∼(1.5-6.0) × 1021 cm−2, which are ∼1.5-15 times less than the averaged interstellar proton column densities for each region. This means that the X-rays are produced not only behind the molecular clouds, but also in front of them. We conclude that the dense molecular clouds have been completely engulfed by the shock waves, but have still survived erosion owing to their high density and short interacting time. The X-ray spectrum toward the gas clumps is well explained by an absorbed power-law model or a high-temperature plasma model, in addition to thermal plasma components, implying that the shock-cloud interaction is efficiently working for both cases through the shock ionization and magnetic field amplification. If the hadronic gamma-ray is dominant in the GeV band, the total energy of the cosmic-ray protons is calculated to be ∼(0.3-1.4) × 1049 erg, with an estimated interstellar proton density of ∼190 90 cm−3, containing both the shock-ionized gas and neutral atomic hydrogen.</description><subject>Astrophysics</subject><subject>Cloud interaction</subject><subject>Clouds</subject><subject>Clumps</subject><subject>Cosmic ray protons</subject><subject>Cosmic rays</subject><subject>Gamma rays</subject><subject>High temperature plasmas</subject><subject>Hydrogen</subject><subject>Interstellar</subject><subject>Ionization</subject><subject>ISM: clouds</subject><subject>ISM: individual objects (LHA 120-N 63A)</subject><subject>ISM: supernova remnants</subject><subject>Magellanic clouds</subject><subject>Magnetic fields</subject><subject>Molecular clouds</subject><subject>Nebulae</subject><subject>Photoionization</subject><subject>photon-dominated region (PDR)</subject><subject>Power law</subject><subject>Proton density (concentration)</subject><subject>Radio telescopes</subject><subject>Shock waves</subject><subject>Spectroscopy</subject><subject>Supernova</subject><subject>Supernova remnants</subject><subject>Thermal plasmas</subject><subject>X-ray spectra</subject><subject>X-ray spectroscopy</subject><subject>X-rays</subject><issn>0004-637X</issn><issn>1538-4357</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><recordid>eNp1kUtPwzAQhC0EEqVw52iJK6FunDgJt6otD6kPREHiFm2cTZuS2sVOisov4meSKDxOnFY7-mZWmiXkvM-ueOgFvb7PQ8fjftCDhLlZekA6v9Ih6TDGPEfw4OWYnFi7blY3ijrkczCZDuhwTueJRbODMtfKUp3RRbVFo_QO6CNuFKiSzgQf0FzRcoV0AmaJdApLLApQuaTDQlfpNR3lVuodmn0TMUJla0gXKKsCTMtYOt4kmKaY0ve8XNV5i5WWr059N_-oRVApfVjpUv8IM0xqN56SowwKi2ffs0ueb8ZPwztnMr-9Hw4mjvQEKx3RzxBYKJOMA3MjAZkIJfekYIEXgpSSIUbIfRYhy9CFxJUIEPLIC1OByHmXXLS5W6PfKrRlvNaVUfXJ2OXCDzmPmKgp1lLSaGsNZvHW5Bsw-7jP4uYfcVN-3JQft_-oLZetJdfbv8x_8S8SrI6x</recordid><startdate>20190301</startdate><enddate>20190301</enddate><creator>Sano, H.</creator><creator>Matsumura, H.</creator><creator>Nagaya, T.</creator><creator>Yamane, Y.</creator><creator>Alsaberi, R. 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Z. E.</au><au>Filipovi, M. D.</au><au>Tachihara, K.</au><au>Fujii, K.</au><au>Tokuda, K.</au><au>Tsuge, K.</au><au>Yoshiike, S.</au><au>Onishi, T.</au><au>Kawamura, A.</au><au>Minamidani, T.</au><au>Mizuno, N.</au><au>Yamamoto, H.</au><au>Inutsuka, S.</au><au>Inoue, T.</au><au>Maxted, N.</au><au>Rowell, G.</au><au>Sasaki, M.</au><au>Fukui, Y.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>ALMA CO Observations of Supernova Remnant N63A in the Large Magellanic Cloud: Discovery of Dense Molecular Clouds Embedded within Shock-ionized and Photoionized Nebulae</atitle><jtitle>The Astrophysical journal</jtitle><stitle>APJ</stitle><addtitle>Astrophys. J</addtitle><date>2019-03-01</date><risdate>2019</risdate><volume>873</volume><issue>1</issue><spage>40</spage><pages>40-</pages><issn>0004-637X</issn><eissn>1538-4357</eissn><abstract>We carried out new 12CO(J = 1-0, 3-2) observations of a N63A supernova remnant (SNR) from the LMC using the Atacama Large Millimeter/submillimeter Array (ALMA) and Atacama Submillimeter Telescope Experiment. We find three giant molecular clouds toward the northeast, east, and near the center of the SNR. Using the ALMA data, we spatially resolved clumpy molecular clouds embedded within the optical nebulae in both the shock-ionized and photoionized lobes discovered by previous H and [S ii] observations. The total mass of the molecular clouds is ∼800 M☉ for the shock-ionized region and ∼1700 M☉ for the photoionized region. Spatially resolved X-ray spectroscopy reveals that the absorbing column densities toward the molecular clouds are ∼(1.5-6.0) × 1021 cm−2, which are ∼1.5-15 times less than the averaged interstellar proton column densities for each region. This means that the X-rays are produced not only behind the molecular clouds, but also in front of them. We conclude that the dense molecular clouds have been completely engulfed by the shock waves, but have still survived erosion owing to their high density and short interacting time. The X-ray spectrum toward the gas clumps is well explained by an absorbed power-law model or a high-temperature plasma model, in addition to thermal plasma components, implying that the shock-cloud interaction is efficiently working for both cases through the shock ionization and magnetic field amplification. If the hadronic gamma-ray is dominant in the GeV band, the total energy of the cosmic-ray protons is calculated to be ∼(0.3-1.4) × 1049 erg, with an estimated interstellar proton density of ∼190 90 cm−3, containing both the shock-ionized gas and neutral atomic hydrogen.</abstract><cop>Philadelphia</cop><pub>The American Astronomical Society</pub><doi>10.3847/1538-4357/ab02fd</doi><tpages>14</tpages><orcidid>https://orcid.org/0000-0002-4990-9288</orcidid><orcidid>https://orcid.org/0000-0002-2062-1600</orcidid><orcidid>https://orcid.org/0000-0003-4366-6518</orcidid><orcidid>https://orcid.org/0000-0001-7813-0380</orcidid><orcidid>https://orcid.org/0000-0002-2458-7876</orcidid><orcidid>https://orcid.org/0000-0001-5609-7372</orcidid><orcidid>https://orcid.org/0000-0003-2762-8378</orcidid><orcidid>https://orcid.org/0000-0001-6533-224X</orcidid><orcidid>https://orcid.org/0000-0001-9778-6692</orcidid><orcidid>https://orcid.org/0000-0002-9516-1581</orcidid><orcidid>https://orcid.org/0000-0001-8296-7482</orcidid><orcidid>https://orcid.org/0000-0003-2062-5692</orcidid><orcidid>https://orcid.org/0000-0002-1411-5410</orcidid><orcidid>https://orcid.org/0000-0002-2794-4840</orcidid><orcidid>https://orcid.org/0000-0001-5302-1866</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Astrophysics Cloud interaction Clouds Clumps Cosmic ray protons Cosmic rays Gamma rays High temperature plasmas Hydrogen Interstellar Ionization ISM: clouds ISM: individual objects (LHA 120-N 63A) ISM: supernova remnants Magellanic clouds Magnetic fields Molecular clouds Nebulae Photoionization photon-dominated region (PDR) Power law Proton density (concentration) Radio telescopes Shock waves Spectroscopy Supernova Supernova remnants Thermal plasmas X-ray spectra X-ray spectroscopy X-rays |
title | ALMA CO Observations of Supernova Remnant N63A in the Large Magellanic Cloud: Discovery of Dense Molecular Clouds Embedded within Shock-ionized and Photoionized Nebulae |
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