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    Methodology of 63Cu(n,2n)62Cu Reaction Rate Measurement

    Source: Journal of Nuclear Engineering and Radiation Science:;2020:;volume( 007 ):;issue: 002::page 024503-1
    Author:
    Schulc, Martin
    ,
    Košťál, Michal
    ,
    Šimon, Jan
    ,
    Novák, Evžen
    DOI: 10.1115/1.4048236
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: This paper presents the measurement of the spectrum-averaged cross section (SACS) of 63Cu(n,2n)62Cu reaction in 252Cf spontaneous fission neutron spectrum. The SACS in the 252Cf spectrum was chosen as a validation tool since 252Cf is the only standard neutron field and 62Cu isotope is not easy to measure by gamma spectroscopy since the gamma line of interest is an annihilation peak, which is also produced by 64Cu isotope. Fortunately, contributions to the annihilation peak from these isotopes can be distinguished due to the very different half-lives. SACS was inferred from the experimental reaction rate. The SACS in the 252Cf spontaneous fission neutron field for the 63Cu(n,2n)62Cu reaction was determined as equal to (0.1763 ± 0.0077 mb). This value agrees with value (0.183 ± 0.007) × 10−3 b within uncertainty presented by W. Mannhart. However, it differs by 12.7% from IRDFF-II value, which is equal to (0.19874 ± 8.954 10−3) × 10−3 b. Furthermore, reasonable agreement is not achieved with ENDF/B-VIII.0, JEFF-3.3, CENDL-3.1, ROSFOND-2010, nor JENDL-4.0 nuclear data libraries.
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      Methodology of 63Cu(n,2n)62Cu Reaction Rate Measurement

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    contributor authorSchulc, Martin
    contributor authorKošťál, Michal
    contributor authorŠimon, Jan
    contributor authorNovák, Evžen
    date accessioned2022-02-05T21:53:17Z
    date available2022-02-05T21:53:17Z
    date copyright11/16/2020 12:00:00 AM
    date issued2020
    identifier issn2332-8983
    identifier otherners_007_02_024503.pdf
    identifier urihttp://yetl.yabesh.ir/yetl1/handle/yetl/4276522
    description abstractThis paper presents the measurement of the spectrum-averaged cross section (SACS) of 63Cu(n,2n)62Cu reaction in 252Cf spontaneous fission neutron spectrum. The SACS in the 252Cf spectrum was chosen as a validation tool since 252Cf is the only standard neutron field and 62Cu isotope is not easy to measure by gamma spectroscopy since the gamma line of interest is an annihilation peak, which is also produced by 64Cu isotope. Fortunately, contributions to the annihilation peak from these isotopes can be distinguished due to the very different half-lives. SACS was inferred from the experimental reaction rate. The SACS in the 252Cf spontaneous fission neutron field for the 63Cu(n,2n)62Cu reaction was determined as equal to (0.1763 ± 0.0077 mb). This value agrees with value (0.183 ± 0.007) × 10−3 b within uncertainty presented by W. Mannhart. However, it differs by 12.7% from IRDFF-II value, which is equal to (0.19874 ± 8.954 10−3) × 10−3 b. Furthermore, reasonable agreement is not achieved with ENDF/B-VIII.0, JEFF-3.3, CENDL-3.1, ROSFOND-2010, nor JENDL-4.0 nuclear data libraries.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleMethodology of 63Cu(n,2n)62Cu Reaction Rate Measurement
    typeJournal Paper
    journal volume7
    journal issue2
    journal titleJournal of Nuclear Engineering and Radiation Science
    identifier doi10.1115/1.4048236
    journal fristpage024503-1
    journal lastpage024503-4
    page4
    treeJournal of Nuclear Engineering and Radiation Science:;2020:;volume( 007 ):;issue: 002
    contenttypeFulltext
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