Conceptual design of the gamma-to-electron magnetic spectrometer for the National Ignition Facility
The Gamma-to-Electron Magnetic Spectrometer (GEMS) diagnostic is designed to measure the prompt γ-ray energy spectrum during high yield deuterium-tritium (DT) implosions at the National Ignition Facility (NIF). The prompt γ-ray spectrum will provide "burn-averaged" observables, including t...
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container_title | Review of scientific instruments |
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creator | Kim, Y Herrmann, H W Jorgenson, H J Barlow, D B Young, C S Stoeffl, W Casey, D Clancy, T Lopez, F E Oertel, J A Hilsabeck, T Moy, K Batha, S H |
description | The Gamma-to-Electron Magnetic Spectrometer (GEMS) diagnostic is designed to measure the prompt γ-ray energy spectrum during high yield deuterium-tritium (DT) implosions at the National Ignition Facility (NIF). The prompt γ-ray spectrum will provide "burn-averaged" observables, including total DT fusion yield, total areal density (ρR), ablator ρR, and fuel ρR. These burn-averaged observables are unique because they are essentially averaged over 4π, providing a global reference for the line-of-sight-specific measurements typical of x-ray and neutron diagnostics. The GEMS conceptual design meets the physics-based requirements: ΔE/E = 3%-5% can be achieved in the range of 2-25 MeV γ-ray energy. Minimum DT neutron yields required for 15% measurement uncertainty at low-resolution mode are: 5 × 10(14) DT-n for ablator ρR (at 0.2 g/cm(2)); 2 × 10(15) DT-n for total DT yield (at 4.2 × 10(-5) γ/n); and 1 × 10(16) DT-n for fuel ρR (at 1 g/cm(2)). |
doi_str_mv | 10.1063/1.4892900 |
format | Article |
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(LLNL), Livermore, CA (United States)</creatorcontrib><description>The Gamma-to-Electron Magnetic Spectrometer (GEMS) diagnostic is designed to measure the prompt γ-ray energy spectrum during high yield deuterium-tritium (DT) implosions at the National Ignition Facility (NIF). The prompt γ-ray spectrum will provide "burn-averaged" observables, including total DT fusion yield, total areal density (ρR), ablator ρR, and fuel ρR. These burn-averaged observables are unique because they are essentially averaged over 4π, providing a global reference for the line-of-sight-specific measurements typical of x-ray and neutron diagnostics. The GEMS conceptual design meets the physics-based requirements: ΔE/E = 3%-5% can be achieved in the range of 2-25 MeV γ-ray energy. Minimum DT neutron yields required for 15% measurement uncertainty at low-resolution mode are: 5 × 10(14) DT-n for ablator ρR (at 0.2 g/cm(2)); 2 × 10(15) DT-n for total DT yield (at 4.2 × 10(-5) γ/n); and 1 × 10(16) DT-n for fuel ρR (at 1 g/cm(2)).</description><identifier>ISSN: 0034-6748</identifier><identifier>EISSN: 1089-7623</identifier><identifier>DOI: 10.1063/1.4892900</identifier><identifier>PMID: 25430301</identifier><language>eng</language><publisher>United States: American Institute of Physics (AIP)</publisher><subject>ENGINEERING ; INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</subject><ispartof>Review of scientific instruments, 2014-11, Vol.85 (11), p.11E122-11E122</ispartof><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c413t-e20bba75f30b60154b244272d870ce29c72aa857d14bd4ad88079448f1e794c73</citedby><cites>FETCH-LOGICAL-c413t-e20bba75f30b60154b244272d870ce29c72aa857d14bd4ad88079448f1e794c73</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,780,784,885,27924,27925</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/25430301$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://www.osti.gov/servlets/purl/1414367$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Kim, Y</creatorcontrib><creatorcontrib>Herrmann, H W</creatorcontrib><creatorcontrib>Jorgenson, H J</creatorcontrib><creatorcontrib>Barlow, D B</creatorcontrib><creatorcontrib>Young, C S</creatorcontrib><creatorcontrib>Stoeffl, W</creatorcontrib><creatorcontrib>Casey, D</creatorcontrib><creatorcontrib>Clancy, T</creatorcontrib><creatorcontrib>Lopez, F E</creatorcontrib><creatorcontrib>Oertel, J A</creatorcontrib><creatorcontrib>Hilsabeck, T</creatorcontrib><creatorcontrib>Moy, K</creatorcontrib><creatorcontrib>Batha, S H</creatorcontrib><creatorcontrib>Lawrence Livermore National Lab. 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Minimum DT neutron yields required for 15% measurement uncertainty at low-resolution mode are: 5 × 10(14) DT-n for ablator ρR (at 0.2 g/cm(2)); 2 × 10(15) DT-n for total DT yield (at 4.2 × 10(-5) γ/n); and 1 × 10(16) DT-n for fuel ρR (at 1 g/cm(2)).</description><subject>ENGINEERING</subject><subject>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</subject><issn>0034-6748</issn><issn>1089-7623</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><recordid>eNo9kMtOwzAQRS0EoqWw4AdQxAoWKX4ldpaoolCpgg2sLceZpEaJHWJ30b8nfcBs7mh0dDU6CN0SPCc4Z09kzmVBC4zP0JRgWaQip-wcTTFmPM0FlxN0FcI3Hicj5BJNaMYZZphMkVl4Z6CPW90mFQTbuMTXSdxA0uiu02n0KbRg4uBd0unGQbQmCf3h0kGEIan9cODfdbTejTWrxtn9miy1sa2Nu2t0Ues2wM0pZ-hr-fK5eEvXH6-rxfM6NZywmALFZalFVjNc5phkvKScU0ErKbABWhhBtZaZqAgvK64rKbEoOJc1gTGNYDN0f-z1IVoVjI1gNsY7N36rCCec5Xvo4Qj1g__ZQoiqs8FA22oHfhsUyamUohCj1xl6PKJm8CEMUKt-sJ0edopgtReviDqJH9m7U-227KD6J_9Ms1_W9Xx6</recordid><startdate>20141101</startdate><enddate>20141101</enddate><creator>Kim, Y</creator><creator>Herrmann, H W</creator><creator>Jorgenson, H J</creator><creator>Barlow, D B</creator><creator>Young, C S</creator><creator>Stoeffl, W</creator><creator>Casey, D</creator><creator>Clancy, T</creator><creator>Lopez, F E</creator><creator>Oertel, J A</creator><creator>Hilsabeck, T</creator><creator>Moy, K</creator><creator>Batha, S H</creator><general>American Institute of Physics (AIP)</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>OIOZB</scope><scope>OTOTI</scope></search><sort><creationdate>20141101</creationdate><title>Conceptual design of the gamma-to-electron magnetic spectrometer for the National Ignition Facility</title><author>Kim, Y ; Herrmann, H W ; Jorgenson, H J ; Barlow, D B ; Young, C S ; Stoeffl, W ; Casey, D ; Clancy, T ; Lopez, F E ; Oertel, J A ; Hilsabeck, T ; Moy, K ; Batha, S H</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c413t-e20bba75f30b60154b244272d870ce29c72aa857d14bd4ad88079448f1e794c73</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>ENGINEERING</topic><topic>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kim, Y</creatorcontrib><creatorcontrib>Herrmann, H W</creatorcontrib><creatorcontrib>Jorgenson, H J</creatorcontrib><creatorcontrib>Barlow, D B</creatorcontrib><creatorcontrib>Young, C S</creatorcontrib><creatorcontrib>Stoeffl, W</creatorcontrib><creatorcontrib>Casey, D</creatorcontrib><creatorcontrib>Clancy, T</creatorcontrib><creatorcontrib>Lopez, F E</creatorcontrib><creatorcontrib>Oertel, J A</creatorcontrib><creatorcontrib>Hilsabeck, T</creatorcontrib><creatorcontrib>Moy, K</creatorcontrib><creatorcontrib>Batha, S H</creatorcontrib><creatorcontrib>Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>Review of scientific instruments</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kim, Y</au><au>Herrmann, H W</au><au>Jorgenson, H J</au><au>Barlow, D B</au><au>Young, C S</au><au>Stoeffl, W</au><au>Casey, D</au><au>Clancy, T</au><au>Lopez, F E</au><au>Oertel, J A</au><au>Hilsabeck, T</au><au>Moy, K</au><au>Batha, S H</au><aucorp>Lawrence Livermore National Lab. (LLNL), Livermore, CA (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Conceptual design of the gamma-to-electron magnetic spectrometer for the National Ignition Facility</atitle><jtitle>Review of scientific instruments</jtitle><addtitle>Rev Sci Instrum</addtitle><date>2014-11-01</date><risdate>2014</risdate><volume>85</volume><issue>11</issue><spage>11E122</spage><epage>11E122</epage><pages>11E122-11E122</pages><issn>0034-6748</issn><eissn>1089-7623</eissn><abstract>The Gamma-to-Electron Magnetic Spectrometer (GEMS) diagnostic is designed to measure the prompt γ-ray energy spectrum during high yield deuterium-tritium (DT) implosions at the National Ignition Facility (NIF). The prompt γ-ray spectrum will provide "burn-averaged" observables, including total DT fusion yield, total areal density (ρR), ablator ρR, and fuel ρR. These burn-averaged observables are unique because they are essentially averaged over 4π, providing a global reference for the line-of-sight-specific measurements typical of x-ray and neutron diagnostics. The GEMS conceptual design meets the physics-based requirements: ΔE/E = 3%-5% can be achieved in the range of 2-25 MeV γ-ray energy. Minimum DT neutron yields required for 15% measurement uncertainty at low-resolution mode are: 5 × 10(14) DT-n for ablator ρR (at 0.2 g/cm(2)); 2 × 10(15) DT-n for total DT yield (at 4.2 × 10(-5) γ/n); and 1 × 10(16) DT-n for fuel ρR (at 1 g/cm(2)).</abstract><cop>United States</cop><pub>American Institute of Physics (AIP)</pub><pmid>25430301</pmid><doi>10.1063/1.4892900</doi><oa>free_for_read</oa></addata></record> |
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title | Conceptual design of the gamma-to-electron magnetic spectrometer for the National Ignition Facility |
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