Fission yield model for astrophysical use based on the four-dimensional Langevin model
Nuclear fission is expected to play an essential role in the r-process nucleosynthesis via the fission recycling process. However, the impact of the fission recycling process on the r-process is still unclear due to the ambiguity of the fission yields for nuclei far from the beta-stability line and...
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creator | Ishizuka, Chikako Tsubakihara, Kohsuke Zhang, Xuan Kouno, Taiki Usang, Mark Chiba, Satoshi |
description | Nuclear fission is expected to play an essential role in the r-process nucleosynthesis via the fission recycling process. However, the impact of the fission recycling process on the r-process is still unclear due to the ambiguity of the fission yields for nuclei far from the beta-stability line and superheavy nuclei. Our four-dimensional Langevin model can reproduce experimental nuclear fission properties, such as fission fragment mass distributions and total kinetic energies in a systematic manner including their sudden changes due to shell structure. Then we developed a phenomenological yield model for nuclei Z=92 to 122, ranging from neutron deficient to very neutron-rich ones, by fitting the fission fragment mass yield obtained by the Langevin model with five Gaussians. We use the charge distributions for each isobar based on a parametrization which we have evaluated based on thousands of experimental data for actinides, to obtain the fission yields in the form of (Z, N) distributions. What is unique here is the sudden change of the mass distribution from a 2-peak to 1-peak structure for the region of
256
Fm, and the appearance of a 5-peak structure for superheavy nuclei predicted by the 4D Langevin calculation. |
doi_str_mv | 10.1051/epjconf/202328404013 |
format | Conference Proceeding |
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256
Fm, and the appearance of a 5-peak structure for superheavy nuclei predicted by the 4D Langevin calculation.</description><identifier>ISSN: 2100-014X</identifier><identifier>ISSN: 2101-6275</identifier><identifier>EISSN: 2100-014X</identifier><identifier>DOI: 10.1051/epjconf/202328404013</identifier><language>eng</language><publisher>Les Ulis: EDP Sciences</publisher><subject>Actinides ; Charge distribution ; Mass distribution ; Nuclear fission ; Nuclear fusion ; Nuclei ; Parameterization ; Recycling ; Shells (structural forms)</subject><ispartof>EPJ Web of conferences, 2023, Vol.284, p.4013</ispartof><rights>2023. This work is licensed under https://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c248t-ad5f914415204a6e4f7108a66fa126e82cfacee7de32240d4c6a76db8355e9df3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>309,310,314,776,780,785,786,860,23909,23910,25118,27901,27902</link.rule.ids></links><search><creatorcontrib>Ishizuka, Chikako</creatorcontrib><creatorcontrib>Tsubakihara, Kohsuke</creatorcontrib><creatorcontrib>Zhang, Xuan</creatorcontrib><creatorcontrib>Kouno, Taiki</creatorcontrib><creatorcontrib>Usang, Mark</creatorcontrib><creatorcontrib>Chiba, Satoshi</creatorcontrib><title>Fission yield model for astrophysical use based on the four-dimensional Langevin model</title><title>EPJ Web of conferences</title><description>Nuclear fission is expected to play an essential role in the r-process nucleosynthesis via the fission recycling process. However, the impact of the fission recycling process on the r-process is still unclear due to the ambiguity of the fission yields for nuclei far from the beta-stability line and superheavy nuclei. Our four-dimensional Langevin model can reproduce experimental nuclear fission properties, such as fission fragment mass distributions and total kinetic energies in a systematic manner including their sudden changes due to shell structure. Then we developed a phenomenological yield model for nuclei Z=92 to 122, ranging from neutron deficient to very neutron-rich ones, by fitting the fission fragment mass yield obtained by the Langevin model with five Gaussians. We use the charge distributions for each isobar based on a parametrization which we have evaluated based on thousands of experimental data for actinides, to obtain the fission yields in the form of (Z, N) distributions. What is unique here is the sudden change of the mass distribution from a 2-peak to 1-peak structure for the region of
256
Fm, and the appearance of a 5-peak structure for superheavy nuclei predicted by the 4D Langevin calculation.</description><subject>Actinides</subject><subject>Charge distribution</subject><subject>Mass distribution</subject><subject>Nuclear fission</subject><subject>Nuclear fusion</subject><subject>Nuclei</subject><subject>Parameterization</subject><subject>Recycling</subject><subject>Shells (structural forms)</subject><issn>2100-014X</issn><issn>2101-6275</issn><issn>2100-014X</issn><fulltext>true</fulltext><rsrctype>conference_proceeding</rsrctype><creationdate>2023</creationdate><recordtype>conference_proceeding</recordtype><sourceid>BENPR</sourceid><recordid>eNpNkE1LAzEQhoMoWGr_gYeA57X57u5RilWh4EXFW0iTiU3ZbtZkV-i_N6U9dC4zh2deXh6E7il5pETSOfQ7Gzs_Z4RxVgsiCOVXaMIoIRWh4vv64r5Fs5x3pAxvGi7VBH2tQs4hdvgQoHV4Hx202MeETR5S7LeHHKxp8ZgBb0wGhws6bKEgY6pc2EN3_C7E2nQ_8Be6U8QduvGmzTA77yn6XD1_LF-r9fvL2_JpXVkm6qEyTvqGCkElI8IoEH5BSW2U8oYyBTWz3liAhQPOmCBOWGUWym1qLiU0zvMpejjl9in-jpAHvSvFSp-sWc0oFw1jslDiRNkUc07gdZ_C3qSDpkQfJeqzRH0pkf8D6TVnfg</recordid><startdate>20230101</startdate><enddate>20230101</enddate><creator>Ishizuka, Chikako</creator><creator>Tsubakihara, Kohsuke</creator><creator>Zhang, Xuan</creator><creator>Kouno, Taiki</creator><creator>Usang, Mark</creator><creator>Chiba, Satoshi</creator><general>EDP Sciences</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FE</scope><scope>8FG</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>P5Z</scope><scope>P62</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope></search><sort><creationdate>20230101</creationdate><title>Fission yield model for astrophysical use based on the four-dimensional Langevin model</title><author>Ishizuka, Chikako ; Tsubakihara, Kohsuke ; Zhang, Xuan ; Kouno, Taiki ; Usang, Mark ; Chiba, Satoshi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c248t-ad5f914415204a6e4f7108a66fa126e82cfacee7de32240d4c6a76db8355e9df3</frbrgroupid><rsrctype>conference_proceedings</rsrctype><prefilter>conference_proceedings</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Actinides</topic><topic>Charge distribution</topic><topic>Mass distribution</topic><topic>Nuclear fission</topic><topic>Nuclear fusion</topic><topic>Nuclei</topic><topic>Parameterization</topic><topic>Recycling</topic><topic>Shells (structural forms)</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ishizuka, Chikako</creatorcontrib><creatorcontrib>Tsubakihara, Kohsuke</creatorcontrib><creatorcontrib>Zhang, Xuan</creatorcontrib><creatorcontrib>Kouno, Taiki</creatorcontrib><creatorcontrib>Usang, Mark</creatorcontrib><creatorcontrib>Chiba, Satoshi</creatorcontrib><collection>CrossRef</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection (ProQuest)</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>Advanced Technologies & Aerospace Database</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</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></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ishizuka, Chikako</au><au>Tsubakihara, Kohsuke</au><au>Zhang, Xuan</au><au>Kouno, Taiki</au><au>Usang, Mark</au><au>Chiba, Satoshi</au><format>book</format><genre>proceeding</genre><ristype>CONF</ristype><atitle>Fission yield model for astrophysical use based on the four-dimensional Langevin model</atitle><btitle>EPJ Web of conferences</btitle><date>2023-01-01</date><risdate>2023</risdate><volume>284</volume><spage>4013</spage><pages>4013-</pages><issn>2100-014X</issn><issn>2101-6275</issn><eissn>2100-014X</eissn><abstract>Nuclear fission is expected to play an essential role in the r-process nucleosynthesis via the fission recycling process. However, the impact of the fission recycling process on the r-process is still unclear due to the ambiguity of the fission yields for nuclei far from the beta-stability line and superheavy nuclei. Our four-dimensional Langevin model can reproduce experimental nuclear fission properties, such as fission fragment mass distributions and total kinetic energies in a systematic manner including their sudden changes due to shell structure. Then we developed a phenomenological yield model for nuclei Z=92 to 122, ranging from neutron deficient to very neutron-rich ones, by fitting the fission fragment mass yield obtained by the Langevin model with five Gaussians. We use the charge distributions for each isobar based on a parametrization which we have evaluated based on thousands of experimental data for actinides, to obtain the fission yields in the form of (Z, N) distributions. What is unique here is the sudden change of the mass distribution from a 2-peak to 1-peak structure for the region of
256
Fm, and the appearance of a 5-peak structure for superheavy nuclei predicted by the 4D Langevin calculation.</abstract><cop>Les Ulis</cop><pub>EDP Sciences</pub><doi>10.1051/epjconf/202328404013</doi><oa>free_for_read</oa></addata></record> |
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subjects | Actinides Charge distribution Mass distribution Nuclear fission Nuclear fusion Nuclei Parameterization Recycling Shells (structural forms) |
title | Fission yield model for astrophysical use based on the four-dimensional Langevin model |
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