Production of Sn and Sb isotopes in high-energy neutron-induced fission of natU
. The first systematic measurement of neutron-induced fission yields has been performed at the upgraded IGISOL-4 facility at the University of Jyväskylä, Finland. The fission products from high-energy neutron-induced fission of nat U were stopped in a gas cell filled with helium buffer gas, and were...
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creator | Mattera, A. Pomp, S. Lantz, M. Rakopoulos, V. Solders, A. Al-Adili, A. Penttilä, H. Moore, I. D. Rinta-Antila, S. Eronen, T. Kankainen, A. Pohjalainen, I. Gorelov, D. Canete, L. Nesterenko, D. Vilén, M. Äystö, J. |
description | .
The first systematic measurement of neutron-induced fission yields has been performed at the upgraded IGISOL-4 facility at the University of Jyväskylä, Finland. The fission products from high-energy neutron-induced fission of
nat
U were stopped in a gas cell filled with helium buffer gas, and were online separated with a dipole magnet. The isobars, with masses in the range
A
= 128-133 , were transported to a tape-implantation station and identified using
γ
-spectroscopy. We report here the relative cumulative isotopic yields of tin (
Z
= 50) and the relative independent isotopic yields of antimony (
Z
= 51) . Isomeric yield ratios were also obtained for five nuclides. The yields of tin show a staggered behaviour around
A
= 131 , not observed in the ENDF/B-VII.1 evaluation. The yields of antimony also contradict the trend from the evaluation, but are in agreement with a calculation performed using the GEF model that shows the yield increasing with mass in the range
A
= 128-133 . |
doi_str_mv | 10.1140/epja/i2018-12462-1 |
format | Article |
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The first systematic measurement of neutron-induced fission yields has been performed at the upgraded IGISOL-4 facility at the University of Jyväskylä, Finland. The fission products from high-energy neutron-induced fission of
nat
U were stopped in a gas cell filled with helium buffer gas, and were online separated with a dipole magnet. The isobars, with masses in the range
A
= 128-133 , were transported to a tape-implantation station and identified using
γ
-spectroscopy. We report here the relative cumulative isotopic yields of tin (
Z
= 50) and the relative independent isotopic yields of antimony (
Z
= 51) . Isomeric yield ratios were also obtained for five nuclides. The yields of tin show a staggered behaviour around
A
= 131 , not observed in the ENDF/B-VII.1 evaluation. The yields of antimony also contradict the trend from the evaluation, but are in agreement with a calculation performed using the GEF model that shows the yield increasing with mass in the range
A
= 128-133 .</description><identifier>ISSN: 1434-6001</identifier><identifier>EISSN: 1434-601X</identifier><identifier>DOI: 10.1140/epja/i2018-12462-1</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer Berlin Heidelberg</publisher><subject>Antimony ; Energy measurement ; Fission products ; Hadrons ; Heavy Ions ; Helium ; Implantation ; Letter ; Nuclear Fusion ; Nuclear isobars ; Nuclear Physics ; Nuclides ; Particle and Nuclear Physics ; Physics ; Physics and Astronomy ; Tin isotopes</subject><ispartof>The European physical journal. A, Hadrons and nuclei, 2018, Vol.54 (3), p.1-4, Article 33</ispartof><rights>The Author(s) 2018</rights><rights>Copyright Springer Science & Business Media 2018</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c2081-eac3318edd5379acd133bbce24041f474b76e7c4680374a7dade465085ce7f583</citedby><cites>FETCH-LOGICAL-c2081-eac3318edd5379acd133bbce24041f474b76e7c4680374a7dade465085ce7f583</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1140/epja/i2018-12462-1$$EPDF$$P50$$Gspringer$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1140/epja/i2018-12462-1$$EHTML$$P50$$Gspringer$$Hfree_for_read</linktohtml><link.rule.ids>314,776,780,27901,27902,41464,42533,51294</link.rule.ids></links><search><creatorcontrib>Mattera, A.</creatorcontrib><creatorcontrib>Pomp, S.</creatorcontrib><creatorcontrib>Lantz, M.</creatorcontrib><creatorcontrib>Rakopoulos, V.</creatorcontrib><creatorcontrib>Solders, A.</creatorcontrib><creatorcontrib>Al-Adili, A.</creatorcontrib><creatorcontrib>Penttilä, H.</creatorcontrib><creatorcontrib>Moore, I. D.</creatorcontrib><creatorcontrib>Rinta-Antila, S.</creatorcontrib><creatorcontrib>Eronen, T.</creatorcontrib><creatorcontrib>Kankainen, A.</creatorcontrib><creatorcontrib>Pohjalainen, I.</creatorcontrib><creatorcontrib>Gorelov, D.</creatorcontrib><creatorcontrib>Canete, L.</creatorcontrib><creatorcontrib>Nesterenko, D.</creatorcontrib><creatorcontrib>Vilén, M.</creatorcontrib><creatorcontrib>Äystö, J.</creatorcontrib><title>Production of Sn and Sb isotopes in high-energy neutron-induced fission of natU</title><title>The European physical journal. A, Hadrons and nuclei</title><addtitle>Eur. Phys. J. A</addtitle><description>.
The first systematic measurement of neutron-induced fission yields has been performed at the upgraded IGISOL-4 facility at the University of Jyväskylä, Finland. The fission products from high-energy neutron-induced fission of
nat
U were stopped in a gas cell filled with helium buffer gas, and were online separated with a dipole magnet. The isobars, with masses in the range
A
= 128-133 , were transported to a tape-implantation station and identified using
γ
-spectroscopy. We report here the relative cumulative isotopic yields of tin (
Z
= 50) and the relative independent isotopic yields of antimony (
Z
= 51) . Isomeric yield ratios were also obtained for five nuclides. The yields of tin show a staggered behaviour around
A
= 131 , not observed in the ENDF/B-VII.1 evaluation. The yields of antimony also contradict the trend from the evaluation, but are in agreement with a calculation performed using the GEF model that shows the yield increasing with mass in the range
A
= 128-133 .</description><subject>Antimony</subject><subject>Energy measurement</subject><subject>Fission products</subject><subject>Hadrons</subject><subject>Heavy Ions</subject><subject>Helium</subject><subject>Implantation</subject><subject>Letter</subject><subject>Nuclear Fusion</subject><subject>Nuclear isobars</subject><subject>Nuclear Physics</subject><subject>Nuclides</subject><subject>Particle and Nuclear Physics</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Tin isotopes</subject><issn>1434-6001</issn><issn>1434-601X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><sourceid>C6C</sourceid><recordid>eNp9kEtLAzEUhYMoWKt_wFXAdezNYx5dSvEFhQq14C5kJnfaFE3GZGbRf-_0ge5c3bM437nwEXLL4Z5zBRNst2biBPCScaFywfgZGXElFcuBf5z_ZuCX5CqlLQAoMc1HZPEWg-3rzgVPQ0OXnhpv6bKiLoUutJio83Tj1huGHuN6Rz32XQyeOT9gaGnjUjrB3nSra3LRmM-EN6c7Jqunx_fZC5svnl9nD3NWCyg5Q1NLyUu0NpPF1NSWS1lVNQoFijeqUFWRY1GrvARZKFNYY1HlGZRZjUWTlXJM7o67bQzfPaZOb0Mf_fBSC4BprlQG2dASx1YdQ0oRG91G92XiTnPQe3F6L04fxOmDOM0HSB6hNJT9GuPf9D_UD2zIclQ</recordid><startdate>2018</startdate><enddate>2018</enddate><creator>Mattera, A.</creator><creator>Pomp, S.</creator><creator>Lantz, M.</creator><creator>Rakopoulos, V.</creator><creator>Solders, A.</creator><creator>Al-Adili, A.</creator><creator>Penttilä, H.</creator><creator>Moore, I. D.</creator><creator>Rinta-Antila, S.</creator><creator>Eronen, T.</creator><creator>Kankainen, A.</creator><creator>Pohjalainen, I.</creator><creator>Gorelov, D.</creator><creator>Canete, L.</creator><creator>Nesterenko, D.</creator><creator>Vilén, M.</creator><creator>Äystö, J.</creator><general>Springer Berlin Heidelberg</general><general>Springer Nature B.V</general><scope>C6C</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>2018</creationdate><title>Production of Sn and Sb isotopes in high-energy neutron-induced fission of natU</title><author>Mattera, A. ; Pomp, S. ; Lantz, M. ; Rakopoulos, V. ; Solders, A. ; Al-Adili, A. ; Penttilä, H. ; Moore, I. D. ; Rinta-Antila, S. ; Eronen, T. ; Kankainen, A. ; Pohjalainen, I. ; Gorelov, D. ; Canete, L. ; Nesterenko, D. ; Vilén, M. ; Äystö, J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c2081-eac3318edd5379acd133bbce24041f474b76e7c4680374a7dade465085ce7f583</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Antimony</topic><topic>Energy measurement</topic><topic>Fission products</topic><topic>Hadrons</topic><topic>Heavy Ions</topic><topic>Helium</topic><topic>Implantation</topic><topic>Letter</topic><topic>Nuclear Fusion</topic><topic>Nuclear isobars</topic><topic>Nuclear Physics</topic><topic>Nuclides</topic><topic>Particle and Nuclear Physics</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Tin isotopes</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Mattera, A.</creatorcontrib><creatorcontrib>Pomp, S.</creatorcontrib><creatorcontrib>Lantz, M.</creatorcontrib><creatorcontrib>Rakopoulos, V.</creatorcontrib><creatorcontrib>Solders, A.</creatorcontrib><creatorcontrib>Al-Adili, A.</creatorcontrib><creatorcontrib>Penttilä, H.</creatorcontrib><creatorcontrib>Moore, I. D.</creatorcontrib><creatorcontrib>Rinta-Antila, S.</creatorcontrib><creatorcontrib>Eronen, T.</creatorcontrib><creatorcontrib>Kankainen, A.</creatorcontrib><creatorcontrib>Pohjalainen, I.</creatorcontrib><creatorcontrib>Gorelov, D.</creatorcontrib><creatorcontrib>Canete, L.</creatorcontrib><creatorcontrib>Nesterenko, D.</creatorcontrib><creatorcontrib>Vilén, M.</creatorcontrib><creatorcontrib>Äystö, J.</creatorcontrib><collection>Springer Nature OA Free Journals</collection><collection>CrossRef</collection><jtitle>The European physical journal. A, Hadrons and nuclei</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Mattera, A.</au><au>Pomp, S.</au><au>Lantz, M.</au><au>Rakopoulos, V.</au><au>Solders, A.</au><au>Al-Adili, A.</au><au>Penttilä, H.</au><au>Moore, I. D.</au><au>Rinta-Antila, S.</au><au>Eronen, T.</au><au>Kankainen, A.</au><au>Pohjalainen, I.</au><au>Gorelov, D.</au><au>Canete, L.</au><au>Nesterenko, D.</au><au>Vilén, M.</au><au>Äystö, J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Production of Sn and Sb isotopes in high-energy neutron-induced fission of natU</atitle><jtitle>The European physical journal. A, Hadrons and nuclei</jtitle><stitle>Eur. Phys. J. A</stitle><date>2018</date><risdate>2018</risdate><volume>54</volume><issue>3</issue><spage>1</spage><epage>4</epage><pages>1-4</pages><artnum>33</artnum><issn>1434-6001</issn><eissn>1434-601X</eissn><abstract>.
The first systematic measurement of neutron-induced fission yields has been performed at the upgraded IGISOL-4 facility at the University of Jyväskylä, Finland. The fission products from high-energy neutron-induced fission of
nat
U were stopped in a gas cell filled with helium buffer gas, and were online separated with a dipole magnet. The isobars, with masses in the range
A
= 128-133 , were transported to a tape-implantation station and identified using
γ
-spectroscopy. We report here the relative cumulative isotopic yields of tin (
Z
= 50) and the relative independent isotopic yields of antimony (
Z
= 51) . Isomeric yield ratios were also obtained for five nuclides. The yields of tin show a staggered behaviour around
A
= 131 , not observed in the ENDF/B-VII.1 evaluation. The yields of antimony also contradict the trend from the evaluation, but are in agreement with a calculation performed using the GEF model that shows the yield increasing with mass in the range
A
= 128-133 .</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1140/epja/i2018-12462-1</doi><tpages>4</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Antimony Energy measurement Fission products Hadrons Heavy Ions Helium Implantation Letter Nuclear Fusion Nuclear isobars Nuclear Physics Nuclides Particle and Nuclear Physics Physics Physics and Astronomy Tin isotopes |
title | Production of Sn and Sb isotopes in high-energy neutron-induced fission of natU |
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