Principal-Axis Analysis of the Eddington Tensor for the Early Post-Bounce Phase of Rotational Core-Collapse Supernovae
Using full Boltzmann neutrino transport, we performed two-dimensional (2D) core-collapse supernova simulations in axisymmetry for two progenitor models with 11.2M and 15.0M both rotational and non-rotational. We employed the results obtained in the early post-bounce phase (t < 20 ms) to assess pe...
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description | Using full Boltzmann neutrino transport, we performed two-dimensional (2D) core-collapse supernova simulations in axisymmetry for two progenitor models with 11.2M and 15.0M both rotational and non-rotational. We employed the results obtained in the early post-bounce phase (t < 20 ms) to assess performance under rapid rotation of some closure relations commonly employed in the truncated moment method. We first made a comparison in 1D under spherical symmetry, though, of the Eddington factor p defined in the fluid rest frame (FR). We confirmed that the maximum entropy closure for the Fermionic distribution (MEFD) performs better than others near the proto-neutron star surface, where p < 1/3 occurs, but does not work well even in 1D when the phase space occupancy satisfies e < 0.5 together with p < 1/3, the condition known to be not represented by MEFD. For the 2D models with the rapid rotation, we employed the principal-axis analysis of the Eddington tensor. We paid particular attention to the direction of the longest principal axis. We observed in FR that it is aligned neither with the radial direction nor with the neutrino flux in 2D, particularly so in convective and/or rapidly rotating regions, the fact not accommodated in the moment method. We repeated the same analysis in the laboratory frame (LB) and found again that the direction of the longest principal axis is not well reproduced by MEFD because the interpolation between the optically thick and thin limits is not very accurate in this frame. |
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We employed the results obtained in the early post-bounce phase (t < 20 ms) to assess performance under rapid rotation of some closure relations commonly employed in the truncated moment method. We first made a comparison in 1D under spherical symmetry, though, of the Eddington factor p defined in the fluid rest frame (FR). We confirmed that the maximum entropy closure for the Fermionic distribution (MEFD) performs better than others near the proto-neutron star surface, where p < 1/3 occurs, but does not work well even in 1D when the phase space occupancy satisfies e < 0.5 together with p < 1/3, the condition known to be not represented by MEFD. For the 2D models with the rapid rotation, we employed the principal-axis analysis of the Eddington tensor. We paid particular attention to the direction of the longest principal axis. We observed in FR that it is aligned neither with the radial direction nor with the neutrino flux in 2D, particularly so in convective and/or rapidly rotating regions, the fact not accommodated in the moment method. We repeated the same analysis in the laboratory frame (LB) and found again that the direction of the longest principal axis is not well reproduced by MEFD because the interpolation between the optically thick and thin limits is not very accurate in this frame.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.2109.05846</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Angular distribution ; Approximation ; Axes (reference lines) ; Evaluation ; Fermi-Dirac statistics ; Mathematical analysis ; Maximum entropy ; Neutrinos ; Occupancy ; Physics - High Energy Astrophysical Phenomena ; Rotation ; Simulation ; Supernovae ; Tensors ; Two dimensional models</subject><ispartof>arXiv.org, 2022-05</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>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,784,885,27924</link.rule.ids><backlink>$$Uhttps://doi.org/10.48550/arXiv.2109.05846$$DView paper in arXiv$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.3847/1538-4357/ac714b$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink></links><search><creatorcontrib>Iwakami, Wakana</creatorcontrib><creatorcontrib>Harada, Akira</creatorcontrib><creatorcontrib>Nagakura, Hiroki</creatorcontrib><creatorcontrib>Akaho, Ryuichiro</creatorcontrib><creatorcontrib>Okawa, Hirotada</creatorcontrib><creatorcontrib>Furusawa, Shun</creatorcontrib><creatorcontrib>Matsufuru, Hideo</creatorcontrib><creatorcontrib>Sumiyoshi, Kohsuke</creatorcontrib><creatorcontrib>Yamada, Shoichi</creatorcontrib><title>Principal-Axis Analysis of the Eddington Tensor for the Early Post-Bounce Phase of Rotational Core-Collapse Supernovae</title><title>arXiv.org</title><description>Using full Boltzmann neutrino transport, we performed two-dimensional (2D) core-collapse supernova simulations in axisymmetry for two progenitor models with 11.2M and 15.0M both rotational and non-rotational. We employed the results obtained in the early post-bounce phase (t < 20 ms) to assess performance under rapid rotation of some closure relations commonly employed in the truncated moment method. We first made a comparison in 1D under spherical symmetry, though, of the Eddington factor p defined in the fluid rest frame (FR). We confirmed that the maximum entropy closure for the Fermionic distribution (MEFD) performs better than others near the proto-neutron star surface, where p < 1/3 occurs, but does not work well even in 1D when the phase space occupancy satisfies e < 0.5 together with p < 1/3, the condition known to be not represented by MEFD. For the 2D models with the rapid rotation, we employed the principal-axis analysis of the Eddington tensor. We paid particular attention to the direction of the longest principal axis. We observed in FR that it is aligned neither with the radial direction nor with the neutrino flux in 2D, particularly so in convective and/or rapidly rotating regions, the fact not accommodated in the moment method. We repeated the same analysis in the laboratory frame (LB) and found again that the direction of the longest principal axis is not well reproduced by MEFD because the interpolation between the optically thick and thin limits is not very accurate in this frame.</description><subject>Angular distribution</subject><subject>Approximation</subject><subject>Axes (reference lines)</subject><subject>Evaluation</subject><subject>Fermi-Dirac statistics</subject><subject>Mathematical analysis</subject><subject>Maximum entropy</subject><subject>Neutrinos</subject><subject>Occupancy</subject><subject>Physics - High Energy Astrophysical Phenomena</subject><subject>Rotation</subject><subject>Simulation</subject><subject>Supernovae</subject><subject>Tensors</subject><subject>Two dimensional models</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>eNotkF9LwzAUxYMgOOY-gE8GfM5M8z-Ps0wnDBy695KmqeuoTU3asX17s82Hy7lwzj1cfgA8ZHjOFOf42YRjc5iTDOs55oqJGzAhlGZIMULuwCzGPcaYCEk4pxNw2ISms01vWrQ4NhEuOtOeYlp8DYedg8uqarrvwXdw67roA6zTXAwT2hPc-DigFz921sHNzkR3vvv0gxkan5pg7oNDuW9b0yfva-xd6PzBuHtwW5s2utm_TsH2dbnNV2j98faeL9bIcMJRxjJVaqm0FsJWlZYiq3WJK8ZsLQnjVLtSVdwSTW3JLONKiFKLJKaSDDM6BY_X2guUog_Njwmn4gynuMBJiadrog_-d3RxKPZ-DOn1WBAuGWdSKk7_AHA4Z3A</recordid><startdate>20220521</startdate><enddate>20220521</enddate><creator>Iwakami, Wakana</creator><creator>Harada, Akira</creator><creator>Nagakura, Hiroki</creator><creator>Akaho, Ryuichiro</creator><creator>Okawa, Hirotada</creator><creator>Furusawa, Shun</creator><creator>Matsufuru, Hideo</creator><creator>Sumiyoshi, Kohsuke</creator><creator>Yamada, Shoichi</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>20220521</creationdate><title>Principal-Axis Analysis of the Eddington Tensor for the Early Post-Bounce Phase of Rotational Core-Collapse Supernovae</title><author>Iwakami, Wakana ; Harada, Akira ; Nagakura, Hiroki ; Akaho, Ryuichiro ; Okawa, Hirotada ; Furusawa, Shun ; Matsufuru, Hideo ; Sumiyoshi, Kohsuke ; Yamada, Shoichi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a525-1418b9789966cdd9761f9b0d44cf724539eb8d5c293cb4c45866b96586ad74043</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Angular distribution</topic><topic>Approximation</topic><topic>Axes (reference lines)</topic><topic>Evaluation</topic><topic>Fermi-Dirac statistics</topic><topic>Mathematical analysis</topic><topic>Maximum entropy</topic><topic>Neutrinos</topic><topic>Occupancy</topic><topic>Physics - High Energy Astrophysical Phenomena</topic><topic>Rotation</topic><topic>Simulation</topic><topic>Supernovae</topic><topic>Tensors</topic><topic>Two dimensional models</topic><toplevel>online_resources</toplevel><creatorcontrib>Iwakami, Wakana</creatorcontrib><creatorcontrib>Harada, Akira</creatorcontrib><creatorcontrib>Nagakura, Hiroki</creatorcontrib><creatorcontrib>Akaho, Ryuichiro</creatorcontrib><creatorcontrib>Okawa, Hirotada</creatorcontrib><creatorcontrib>Furusawa, Shun</creatorcontrib><creatorcontrib>Matsufuru, Hideo</creatorcontrib><creatorcontrib>Sumiyoshi, Kohsuke</creatorcontrib><creatorcontrib>Yamada, Shoichi</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Iwakami, Wakana</au><au>Harada, Akira</au><au>Nagakura, Hiroki</au><au>Akaho, Ryuichiro</au><au>Okawa, Hirotada</au><au>Furusawa, Shun</au><au>Matsufuru, Hideo</au><au>Sumiyoshi, Kohsuke</au><au>Yamada, Shoichi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Principal-Axis Analysis of the Eddington Tensor for the Early Post-Bounce Phase of Rotational Core-Collapse Supernovae</atitle><jtitle>arXiv.org</jtitle><date>2022-05-21</date><risdate>2022</risdate><eissn>2331-8422</eissn><abstract>Using full Boltzmann neutrino transport, we performed two-dimensional (2D) core-collapse supernova simulations in axisymmetry for two progenitor models with 11.2M and 15.0M both rotational and non-rotational. We employed the results obtained in the early post-bounce phase (t < 20 ms) to assess performance under rapid rotation of some closure relations commonly employed in the truncated moment method. We first made a comparison in 1D under spherical symmetry, though, of the Eddington factor p defined in the fluid rest frame (FR). We confirmed that the maximum entropy closure for the Fermionic distribution (MEFD) performs better than others near the proto-neutron star surface, where p < 1/3 occurs, but does not work well even in 1D when the phase space occupancy satisfies e < 0.5 together with p < 1/3, the condition known to be not represented by MEFD. For the 2D models with the rapid rotation, we employed the principal-axis analysis of the Eddington tensor. We paid particular attention to the direction of the longest principal axis. We observed in FR that it is aligned neither with the radial direction nor with the neutrino flux in 2D, particularly so in convective and/or rapidly rotating regions, the fact not accommodated in the moment method. We repeated the same analysis in the laboratory frame (LB) and found again that the direction of the longest principal axis is not well reproduced by MEFD because the interpolation between the optically thick and thin limits is not very accurate in this frame.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.2109.05846</doi><oa>free_for_read</oa></addata></record> |
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subjects | Angular distribution Approximation Axes (reference lines) Evaluation Fermi-Dirac statistics Mathematical analysis Maximum entropy Neutrinos Occupancy Physics - High Energy Astrophysical Phenomena Rotation Simulation Supernovae Tensors Two dimensional models |
title | Principal-Axis Analysis of the Eddington Tensor for the Early Post-Bounce Phase of Rotational Core-Collapse Supernovae |
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