Pub Date : 2024-03-06DOI: 10.1016/j.nds.2024.02.003
Balraj Singh , Jun Chen
Experimental nuclear spectroscopic data are compiled and evaluated for 18 known nuclides of mass 165 (Pm, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu, Hf, Ta, W, Re, Os, Ir, Pt). Detailed information is presented for each reaction and decay experiment. Combining all the available data, recommended values are provided for energies, spins and parities, and half-lives of levels, with energies, branching ratios and multipolarities of γ radiations, and characteristics of β and α radiations in radioactive decays. 165Dy, 165Ho, 165Er, 165Tm, 165Yb, 165Lu and 165Hf are among the most extensively studied nuclides via decay and high-spin gamma-ray spectroscopy measurements, followed by limited data for 165Tb, 165Ta, 165W, 165Re, and 165Os. No excited states have yet been identified in 165Sm, 165Gd, and 165Pt, while for 165Eu and 165Ir, information is available for only the g.s. and an isomer, but with no γ rays. This work supersedes earlier evaluation of A=165 nuclides by 2006Ja09.
{"title":"Nuclear Structure and Decay Data for A=165 Isobars","authors":"Balraj Singh , Jun Chen","doi":"10.1016/j.nds.2024.02.003","DOIUrl":"https://doi.org/10.1016/j.nds.2024.02.003","url":null,"abstract":"<div><p>Experimental nuclear spectroscopic data are compiled and evaluated for 18 known nuclides of mass 165 (Pm, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu, Hf, Ta, W, Re, Os, Ir, Pt). Detailed information is presented for each reaction and decay experiment. Combining all the available data, recommended values are provided for energies, spins and parities, and half-lives of levels, with energies, branching ratios and multipolarities of <em>γ</em> radiations, and characteristics of <em>β</em> and <em>α</em> radiations in radioactive decays. <sup>165</sup>Dy, <sup>165</sup>Ho, <sup>165</sup>Er, <sup>165</sup>Tm, <sup>165</sup>Yb, <sup>165</sup>Lu and <sup>165</sup>Hf are among the most extensively studied nuclides via decay and high-spin gamma-ray spectroscopy measurements, followed by limited data for <sup>165</sup>Tb, <sup>165</sup>Ta, <sup>165</sup>W, <sup>165</sup>Re, and <sup>165</sup>Os. No excited states have yet been identified in <sup>165</sup>Sm, <sup>165</sup>Gd, and <sup>165</sup>Pt, while for <sup>165</sup>Eu and <sup>165</sup>Ir, information is available for only the g.s. and an isomer, but with no <em>γ</em> rays. This work supersedes earlier evaluation of A=165 nuclides by 2006Ja09.</p></div>","PeriodicalId":49735,"journal":{"name":"Nuclear Data Sheets","volume":"194 ","pages":"Pages 460-877"},"PeriodicalIF":3.7,"publicationDate":"2024-03-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140041859","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-03-06DOI: 10.1016/S0090-3752(24)00025-5
{"title":"Nuclear Data Sheets Symbols and Abbreviations","authors":"","doi":"10.1016/S0090-3752(24)00025-5","DOIUrl":"https://doi.org/10.1016/S0090-3752(24)00025-5","url":null,"abstract":"","PeriodicalId":49735,"journal":{"name":"Nuclear Data Sheets","volume":"194 ","pages":"Page IBC"},"PeriodicalIF":3.7,"publicationDate":"2024-03-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140041860","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01DOI: 10.1016/j.nds.2024.01.006
A.S. Tamashiro , J.T. Harke , J.G. Duarte , Y. Mishnayot , S. Burcher , S.W. Padgett , P. Zhao , B.D. Pierson , N. Gharibyan , J.M. Goda , L.R. Greenwood , D.K. Hayes , J. Hutchinson , N. Harward , K. Roberts , G. Slavik , P. Yap-Chiongco , J. Walker , C.J. Palmer
Precise integral measurement of fast neutron-induced fission product yields for various actinides is of high interest for applied nuclear science. The goal of this effort is to improve uncertainties in fission product yield values of 237Np. Fission was induced in a NpO2(NO3) target using the Godiva IV critical assembly in burst mode. The irradiated sample was transferred to a high-resolution γ-ray detection setup within 50 minutes. γ-ray list mode data was collected from 50 minutes to 1 week after the irradiation. γ-ray spectroscopy was performed to analyze the time dependent γ-ray yields using an automated peak search algorithm to identify isotopes by their decay γ-ray energy and half-life. The initial activity for each isotope identified was used to calculate their fission product yield.
{"title":"237Np Fission Spectrum Cumulative Fission Product Yield Measurement Using Godiva IV Critical Assembly","authors":"A.S. Tamashiro , J.T. Harke , J.G. Duarte , Y. Mishnayot , S. Burcher , S.W. Padgett , P. Zhao , B.D. Pierson , N. Gharibyan , J.M. Goda , L.R. Greenwood , D.K. Hayes , J. Hutchinson , N. Harward , K. Roberts , G. Slavik , P. Yap-Chiongco , J. Walker , C.J. Palmer","doi":"10.1016/j.nds.2024.01.006","DOIUrl":"https://doi.org/10.1016/j.nds.2024.01.006","url":null,"abstract":"<div><p>Precise integral measurement of fast neutron-induced fission product yields for various actinides is of high interest for applied nuclear science. The goal of this effort is to improve uncertainties in fission product yield values of <sup>237</sup>Np. Fission was induced in a NpO<sub>2</sub>(NO<sub>3</sub>) target using the Godiva IV critical assembly in burst mode. The irradiated sample was transferred to a high-resolution <em>γ</em>-ray detection setup within 50 minutes. <em>γ</em>-ray list mode data was collected from 50 minutes to 1 week after the irradiation. <em>γ</em>-ray spectroscopy was performed to analyze the time dependent <em>γ</em>-ray yields using an automated peak search algorithm to identify isotopes by their decay <em>γ</em>-ray energy and half-life. The initial activity for each isotope identified was used to calculate their fission product yield.</p></div>","PeriodicalId":49735,"journal":{"name":"Nuclear Data Sheets","volume":"193 ","pages":"Pages 131-152"},"PeriodicalIF":3.7,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0090375224000073/pdf?md5=ed12f84a6f8a7bd329cdfde1f5e9279c&pid=1-s2.0-S0090375224000073-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139693887","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01DOI: 10.1016/j.nds.2024.01.002
S. Pommé , H. Stroh , J. Paepen
The half-life of 22Na has been determined through 523 activity measurements over 14.5 years with a re-entrant ionisation chamber in a temperature-stabilised room. The data were selected and aggregated from in total 127 830 ionisation current measurements with a reproducibility of the order of 0.065 % standard deviation. The ionisation current was collected over an air capacitor and measured as a change of voltage over time, which warrants excellent linearity with activity throughout the experiment. The residuals to an exponential decay curve show a distinct annual cycle of 0.0055 (5) % amplitude, which reduces to 0.0012 (5) % after compensation for a correlation with ambient humidity. The data confirm the validity of the exponential-decay law, in absence of cyclic perturbations at daily, monthly, and multi-annual scale at the level of 0.0005 % standard deviation. The 22Na half-life value obtained in this study is 950.68 (12) d or 2.60290 (34) a, with a relative standard uncertainty of 0.013 %. This value is consistent with the mean value of other measurement results in the literature, although the latter have an issue with incomplete uncertainty budgets. Owing to the high statistical accuracy and conservative uncertainty estimate of systematic errors, the result obtained in this work can be recommended as a reliable reference value.
{"title":"Measurement of the 22Na half-life and evidence supporting the exponential-decay law","authors":"S. Pommé , H. Stroh , J. Paepen","doi":"10.1016/j.nds.2024.01.002","DOIUrl":"https://doi.org/10.1016/j.nds.2024.01.002","url":null,"abstract":"<div><p>The half-life of <sup>22</sup>Na has been determined through 523 activity measurements over 14.5 years with a re-entrant ionisation chamber in a temperature-stabilised room. The data were selected and aggregated from in total 127 830 ionisation current measurements with a reproducibility of the order of 0.065<!--> <!-->% standard deviation. The ionisation current was collected over an air capacitor and measured as a change of voltage over time, which warrants excellent linearity with activity throughout the experiment. The residuals to an exponential decay curve show a distinct annual cycle of 0.0055 (5)<!--> <!-->% amplitude, which reduces to 0.0012 (5)<!--> <!-->% after compensation for a correlation with ambient humidity. The data confirm the validity of the exponential-decay law, in absence of cyclic perturbations at daily, monthly, and multi-annual scale at the level of 0.0005<!--> <!-->% standard deviation. The <sup>22</sup>Na half-life value obtained in this study is 950.68 (12) d or 2.60290 (34) a, with a relative standard uncertainty of 0.013<!--> <!-->%. This value is consistent with the mean value of other measurement results in the literature, although the latter have an issue with incomplete uncertainty budgets. Owing to the high statistical accuracy and conservative uncertainty estimate of systematic errors, the result obtained in this work can be recommended as a reliable reference value.</p></div>","PeriodicalId":49735,"journal":{"name":"Nuclear Data Sheets","volume":"193 ","pages":"Pages 79-87"},"PeriodicalIF":3.7,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0090375224000024/pdf?md5=7dc354d98673d4d756cda9b73dfc3296&pid=1-s2.0-S0090375224000024-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139694293","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01DOI: 10.1016/j.nds.2024.01.007
A.S. Tamashiro , J.T. Harke , J.G. Duarte , Y. Mishnayot , S.W. Padgett , G. Slavik , S. Burcher , N. Harward , N. Gharibyan , R.A. Henderson , L.R. Greenwood , B.D. Pierson , J.M. Goda , J.A. Bounds , D.K. Hayes , C.J. Palmer
Precise integral measurement of fast neutron-induced fission product yields for various actinides is of high interest for applied nuclear science. The goal of this effort is to improve uncertainties in fission product yield values of 239Pu. Fission was induced in a pure 239Pu () target using the Godiva IV critical assembly in burst mode. The irradiated sample was transferred to a high-resolution γ-ray detector within 45 minutes. γ-ray list mode data was collected from 45 minutes to 1 week after the irradiation. γ-ray spectroscopy was performed to analyze the time dependent γ-ray yields using an automated peak search algorithm to identify isotopes by their decay γ-ray energy and half-life. The initial activity for each isotope identified was used to calculate their fission product yield.
{"title":"239Pu Fission Spectrum Cumulative Fission Product Yield Measurement Using Godiva IV Critical Assembly","authors":"A.S. Tamashiro , J.T. Harke , J.G. Duarte , Y. Mishnayot , S.W. Padgett , G. Slavik , S. Burcher , N. Harward , N. Gharibyan , R.A. Henderson , L.R. Greenwood , B.D. Pierson , J.M. Goda , J.A. Bounds , D.K. Hayes , C.J. Palmer","doi":"10.1016/j.nds.2024.01.007","DOIUrl":"https://doi.org/10.1016/j.nds.2024.01.007","url":null,"abstract":"<div><p>Precise integral measurement of fast neutron-induced fission product yields for various actinides is of high interest for applied nuclear science. The goal of this effort is to improve uncertainties in fission product yield values of <sup>239</sup>Pu. Fission was induced in a pure <sup>239</sup>Pu (<span><math><mo>></mo><mn>99</mn><mspace></mspace><mtext>%</mtext></math></span>) target using the Godiva IV critical assembly in burst mode. The irradiated sample was transferred to a high-resolution <em>γ</em>-ray detector within 45 minutes. <em>γ</em>-ray list mode data was collected from 45 minutes to 1 week after the irradiation. <em>γ</em>-ray spectroscopy was performed to analyze the time dependent <em>γ</em>-ray yields using an automated peak search algorithm to identify isotopes by their decay <em>γ</em>-ray energy and half-life. The initial activity for each isotope identified was used to calculate their fission product yield.</p></div>","PeriodicalId":49735,"journal":{"name":"Nuclear Data Sheets","volume":"193 ","pages":"Pages 153-177"},"PeriodicalIF":3.7,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0090375224000085/pdf?md5=cedfbab82dee9f192ea7bc09fad0812d&pid=1-s2.0-S0090375224000085-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139693888","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01DOI: 10.1016/j.nds.2024.01.003
T.J. Gray , J.M. Allmond , L.G. Evans , B.D. Roach , T.T. King , B.C. Rasco
The absolute γ-ray branching ratios (emission probabilities) for 19 prominent peaks in the α decay of 233U are reported with energies ranging from 97 to 366 keV. The branching ratios were obtained from α-γ coincidence measurements, normalized to the α singles. The high-purity 233U material () was separated from its decay products before preparation of a 4.74- uranyl nitrate foil with a 6-mm diameter. This is the first report on the absolute normalization of the branching ratios since 1984 and it is the only measure by α-γ coincidences, where the ratio removes several potential systematic biases. Overall, the results are consistent with the adopted literature and they validate the quantities most relevant to the non-destructive assay of fissile 233U material, which is relevant to the thorium fuel cycle and associated safeguards.
{"title":"Absolute Branching Ratios of Prominent γ Rays Following α Decay of 233U","authors":"T.J. Gray , J.M. Allmond , L.G. Evans , B.D. Roach , T.T. King , B.C. Rasco","doi":"10.1016/j.nds.2024.01.003","DOIUrl":"https://doi.org/10.1016/j.nds.2024.01.003","url":null,"abstract":"<div><p>The absolute <em>γ</em>-ray branching ratios (emission probabilities) for 19 prominent peaks in the <em>α</em> decay of <sup>233</sup>U are reported with energies ranging from 97 to 366 keV. The branching ratios were obtained from <em>α</em>-<em>γ</em> coincidence measurements, normalized to the <em>α</em> singles. The high-purity <sup>233</sup>U material (<span><math><mo>></mo><mn>99.98</mn><mtext>%</mtext></math></span>) was separated from its decay products before preparation of a 4.74-<span><math><mtext>mg</mtext><mo>/</mo><msup><mrow><mtext>cm</mtext></mrow><mrow><mn>2</mn></mrow></msup></math></span> uranyl nitrate foil with a 6-mm diameter. This is the first report on the absolute normalization of the branching ratios since 1984 and it is the only measure by <em>α</em>-<em>γ</em> coincidences, where the <span><math><mi>α</mi><mtext>-</mtext><mi>γ</mi><mo>/</mo><mi>α</mi></math></span> ratio removes several potential systematic biases. Overall, the results are consistent with the adopted literature and they validate the quantities most relevant to the non-destructive assay of fissile <sup>233</sup>U material, which is relevant to the thorium fuel cycle and associated safeguards.</p></div>","PeriodicalId":49735,"journal":{"name":"Nuclear Data Sheets","volume":"193 ","pages":"Pages 88-94"},"PeriodicalIF":3.7,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0090375224000048/pdf?md5=fa7981ffc39bc68abb366419e8cc2a62&pid=1-s2.0-S0090375224000048-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139694294","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01DOI: 10.1016/S0090-3752(24)00014-0
{"title":"Nuclear Data Sheets Symbols and Abbreviations","authors":"","doi":"10.1016/S0090-3752(24)00014-0","DOIUrl":"https://doi.org/10.1016/S0090-3752(24)00014-0","url":null,"abstract":"","PeriodicalId":49735,"journal":{"name":"Nuclear Data Sheets","volume":"193 ","pages":"Page IBC"},"PeriodicalIF":3.7,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0090375224000140/pdfft?md5=74c86dfaecc2b81ec203e0cd0f5760b5&pid=1-s2.0-S0090375224000140-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139693889","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01DOI: 10.1016/j.nds.2024.01.001
G. Schnabel , D.L. Aldama , T. Bohm , U. Fischer , S. Kunieda , A. Trkov , C. Konno , R. Capote , A.J. Koning , S. Breidokaite , T. Eade , M. Fabbri , D. Flammini , L. Isolan , I. Kodeli , M. Košťál , S. Kwon , D. Laghi , D. Leichtle , S. Nakayama , A. Žohar
The Fusion Evaluated Nuclear Data Library (FENDL) is a comprehensive and validated collection of nuclear cross section data coordinated by the International Atomic Energy Agency (IAEA) Nuclear Data Section (NDS). FENDL assembles the best nuclear data for fusion applications selected from available nuclear data libraries and has been under development for decades. FENDL contains sub-libraries for incident neutron, proton, and deuteron cross sections including general purpose and activation files used for particle transport and nuclide inventory calculations.
In this work, we describe the history, selection of evaluations for the various sub-libraries (neutron, proton, deuteron) with the focus on transport and reactor dosimetry applications, the processing of the nuclear data for application codes (e.g. MCNP), and the development of the TENDL-2017 library which is the currently recommended activation library for FENDL. We briefly describe the IAEA IRDFF library as the recommended library for dosimetry fusion applications. We also present work on validation of the neutron sub-library using a variety of fusion relevant computational and experimental benchmarks using the MCNP transport code and ACE-formatted cross section libraries. A variety of cross section libraries are used for the validation work including FENDL-2.1, FENDL-3.1d, FENDL-3.2, ENDF/B-VIII.0, and JEFF-3.2 with the emphasis on the FENDL libraries.
The results of the validation using computational benchmarks showed generally good agreement among the tested neutron cross section libraries for neutron flux, nuclear heating, and primary displacement damage (dpa). Gas production (H/He) in structural materials showed substantial differences to the reference FENDL-2.1 library. The results of the experimental validation showed that the performance of FENDL-3.2b is at least as good and in most cases better than FENDL-2.1.
Future work will consider improved evaluations developed by the International Nuclear Data Evaluation Network (INDEN) for materials such as O, Cu, W, Li, B, and F. Additionally, work will need to be done to investigate differences in gas production in structural materials. Covariance matrices will need to be developed or updated as availability of consistent and comprehensive uncertainty information will be needed as fusion technology and facility construction matures. Finally, additional validation work for high energy neutrons, protons and deuterons, as well as validation work for the activation library will be needed.
{"title":"FENDL: A library for fusion research and applications","authors":"G. Schnabel , D.L. Aldama , T. Bohm , U. Fischer , S. Kunieda , A. Trkov , C. Konno , R. Capote , A.J. Koning , S. Breidokaite , T. Eade , M. Fabbri , D. Flammini , L. Isolan , I. Kodeli , M. Košťál , S. Kwon , D. Laghi , D. Leichtle , S. Nakayama , A. Žohar","doi":"10.1016/j.nds.2024.01.001","DOIUrl":"https://doi.org/10.1016/j.nds.2024.01.001","url":null,"abstract":"<div><p>The Fusion Evaluated Nuclear Data Library (FENDL) is a comprehensive and validated collection of nuclear cross section data coordinated by the International Atomic Energy Agency (IAEA) Nuclear Data Section (NDS). FENDL assembles the best nuclear data for fusion applications selected from available nuclear data libraries and has been under development for decades. FENDL contains sub-libraries for incident neutron, proton, and deuteron cross sections including general purpose and activation files used for particle transport and nuclide inventory calculations.</p><p>In this work, we describe the history, selection of evaluations for the various sub-libraries (neutron, proton, deuteron) with the focus on transport and reactor dosimetry applications, the processing of the nuclear data for application codes (e.g. MCNP), and the development of the TENDL-2017 library which is the currently recommended activation library for FENDL. We briefly describe the IAEA IRDFF library as the recommended library for dosimetry fusion applications. We also present work on validation of the neutron sub-library using a variety of fusion relevant computational and experimental benchmarks using the MCNP transport code and ACE-formatted cross section libraries. A variety of cross section libraries are used for the validation work including FENDL-2.1, FENDL-3.1d, FENDL-3.2, ENDF/B-VIII.0, and JEFF-3.2 with the emphasis on the FENDL libraries.</p><p>The results of the validation using computational benchmarks showed generally good agreement among the tested neutron cross section libraries for neutron flux, nuclear heating, and primary displacement damage (dpa). Gas production (H/He) in structural materials showed substantial differences to the reference FENDL-2.1 library. The results of the experimental validation showed that the performance of FENDL-3.2b is at least as good and in most cases better than FENDL-2.1.</p><p>Future work will consider improved evaluations developed by the International Nuclear Data Evaluation Network (INDEN) for materials such as O, Cu, W, Li, B, and F. Additionally, work will need to be done to investigate differences in gas production in structural materials. Covariance matrices will need to be developed or updated as availability of consistent and comprehensive uncertainty information will be needed as fusion technology and facility construction matures. Finally, additional validation work for high energy neutrons, protons and deuterons, as well as validation work for the activation library will be needed.</p></div>","PeriodicalId":49735,"journal":{"name":"Nuclear Data Sheets","volume":"193 ","pages":"Pages 1-78"},"PeriodicalIF":3.7,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0090375224000012/pdf?md5=4d854e009f05ad6e51d234a39785a763&pid=1-s2.0-S0090375224000012-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139694292","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-02-01DOI: 10.1016/j.nds.2024.01.004
I. Durán , R. Capote , P. Cabanelas
Precise normalization of ToF yield measurements of neutron induced fission in fissile targets is challenging, but the appropriate normalization is also of critical importance for nuclear energy and criticality safety, among other applications. A typical normalization relies on the Thermal Neutron Constants (TNC) recommended at the thermal point (fission and capture thermal cross sections) by the Neutron Standards. However, many ToF experiments do not collect data down to the thermal energy and use normalization cross-section integrals defined at different arbitrary energy intervals. Normalization fission cross-section integrals are recommended in between-valleys energy regions 8.1–14.7 eV, 7.8–11 eV, 9–20 eV, and 11.7–19.5 eV for fissile targets 233U, 235U, 239Pu, and 241Pu with values equal to 689.0(10.8), 245.7(4.1), 1059(6), and 1378(33) , respectively. The 235U normalization integral derived in this work of 245.7(4.1) is in good agreement within quoted uncertainties with the Neutron Standards value of 247.5(3.0) .
Additional cross-section integrals in the thermal region from 20–60 meV are derived to fix both the normalization and the slope of the fission cross section at the thermal point providing additional constraints for R-matrix evaluations of experimental fission yields. Ratios and feature very low uncertainty due to the strong positive correlations between the numerator and the denominator and are comprehensively derived for the first time. Integral ratios of 39.31(54), 13.08(20), 41.65(22), and 40.46(85) are recommended as reference for fissile targets 233U, 235U, 239Pu, and 241Pu, respectively. Similarly, ratios
{"title":"Normalization of ToF (n,f) Measurements in Fissile Targets: Microscopic cross-section integrals","authors":"I. Durán , R. Capote , P. Cabanelas","doi":"10.1016/j.nds.2024.01.004","DOIUrl":"https://doi.org/10.1016/j.nds.2024.01.004","url":null,"abstract":"<div><p>Precise normalization of ToF yield measurements of neutron induced fission in fissile targets is challenging, but the appropriate normalization is also of critical importance for nuclear energy and criticality safety, among other applications. A typical normalization relies on the Thermal Neutron Constants (TNC) recommended at the thermal point (fission <span><math><msubsup><mrow><mi>σ</mi></mrow><mrow><mi>f</mi></mrow><mrow><mn>0</mn></mrow></msubsup></math></span> and capture <span><math><msubsup><mrow><mi>σ</mi></mrow><mrow><mi>γ</mi></mrow><mrow><mn>0</mn></mrow></msubsup></math></span> thermal cross sections) by the Neutron Standards. However, many ToF experiments do not collect data down to the thermal energy and use normalization cross-section integrals defined at different arbitrary energy intervals. Normalization fission cross-section integrals <span><math><msub><mrow><mi>I</mi></mrow><mrow><mn>3</mn></mrow></msub></math></span> are recommended in between-valleys energy regions 8.1–14.7 eV, 7.8–11 eV, 9–20 eV, and 11.7–19.5 eV for fissile targets <sup>233</sup>U, <sup>235</sup>U, <sup>239</sup>Pu, and <sup>241</sup>Pu with values equal to 689.0(10.8), 245.7(4.1), 1059(6), and 1378(33) <span><math><mi>b</mi><mo>⋅</mo><mi>e</mi><mi>V</mi></math></span>, respectively. The <sub>235</sub>U normalization integral <span><math><msub><mrow><mi>I</mi></mrow><mrow><mn>3</mn></mrow></msub></math></span> derived in this work of 245.7(4.1) <span><math><mi>b</mi><mo>⋅</mo><mi>e</mi><mi>V</mi></math></span> is in good agreement within quoted uncertainties with the Neutron Standards value of 247.5(3.0) <span><math><mi>b</mi><mo>⋅</mo><mi>e</mi><mi>V</mi></math></span>.</p><p>Additional cross-section integrals <span><math><msub><mrow><mi>I</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span> in the thermal region from 20–60 meV are derived to fix both the normalization and the slope of the fission cross section at the thermal point providing additional constraints for R-matrix evaluations of experimental fission yields. Ratios <span><math><msubsup><mrow><mi>σ</mi></mrow><mrow><mi>f</mi></mrow><mrow><mn>0</mn></mrow></msubsup><mo>/</mo><msub><mrow><mi>I</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span> and <span><math><msub><mrow><mi>I</mi></mrow><mrow><mn>3</mn></mrow></msub><mo>/</mo><msub><mrow><mi>I</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span> feature very low uncertainty due to the strong positive correlations between the numerator and the denominator and are comprehensively derived for the first time. Integral ratios <span><math><msub><mrow><mi>I</mi></mrow><mrow><mn>3</mn></mrow></msub><mo>/</mo><msub><mrow><mi>I</mi></mrow><mrow><mn>1</mn></mrow></msub></math></span> of 39.31(54), 13.08(20), 41.65(22), and 40.46(85) are recommended as reference for fissile targets <sup>233</sup>U, <sup>235</sup>U, <sup>239</sup>Pu, and <sup>241</sup>Pu, respectively. Similarly, ratios <span><math><msubsup><mrow><mi>σ</mi></mrow><mrow><mi","PeriodicalId":49735,"journal":{"name":"Nuclear Data Sheets","volume":"193 ","pages":"Pages 95-104"},"PeriodicalIF":3.7,"publicationDate":"2024-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S009037522400005X/pdf?md5=81f56bc93151d9f0f06777235966e6c4&pid=1-s2.0-S009037522400005X-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"139694295","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}