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General Policies - Presentation of Data 一般政策 - 数据的列报
IF 3.7 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2024-03-06 DOI: 10.1016/S0090-3752(24)00023-1
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引用次数: 0
Nuclear Structure and Decay Data for A=165 Isobars A=165 等离子体的核结构和衰变数据
IF 3.7 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2024-03-06 DOI: 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.

汇编并评估了 18 种质量为 165(Pm、Sm、Eu、Gd、Tb、Dy、Ho、Er、Tm、Yb、Lu、Hf、Ta、W、Re、Os、Ir、Pt)的已知核素的核光谱实验数据。每个反应和衰变实验都有详细的信息。综合所有可用数据,提供了能量、自旋和奇偶性、水平半衰期的建议值,以及 γ 辐射的能量、分支比和多极性,以及放射性衰变中 β 和 α 辐射的特征。通过衰变和高自旋伽马射线光谱测量,165Dy、165Ho、165Er、165Tm、165Yb、165Lu 和 165Hf 是研究最广泛的核素,其次是 165Tb、165Ta、165W、165Re 和 165Os。165Sm、165Gd 和 165Pt 尚未发现激发态,而 165Eu 和 165Ir 仅有 g.s. 和一种异构体的信息,但没有 γ 射线。这项工作取代了早先在2006Ja09年对A=165 核素的评估。
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引用次数: 0
Nuclear Data Sheets Symbols and Abbreviations 核数据表符号和缩略语
IF 3.7 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2024-03-06 DOI: 10.1016/S0090-3752(24)00025-5
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引用次数: 0
237Np Fission Spectrum Cumulative Fission Product Yield Measurement Using Godiva IV Critical Assembly 利用戈迪瓦 IV 临界组件测量 237Np 裂变谱累积裂变产物当量
IF 3.7 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2024-02-01 DOI: 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.

对各种锕系元素的快中子诱发裂变产物产率进行精确的积分测量,对应用核科学具有重要意义。这项工作的目标是改善 237Np 裂变产物产率值的不确定性。使用 Godiva IV 临界组件在爆发模式下诱导 NpO2(NO3)靶裂变。辐照样品在 50 分钟内被转移到高分辨率 γ 射线探测装置上。利用自动峰值搜索算法,通过衰变γ射线能量和半衰期来识别同位素。所确定的每种同位素的初始活度都被用来计算其裂变产物产率。
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引用次数: 0
Measurement of the 22Na half-life and evidence supporting the exponential-decay law 22Na 半衰期的测量和支持指数衰减规律的证据
IF 3.7 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2024-02-01 DOI: 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.

22Na 的半衰期是通过在一个温度稳定的房间内使用重入式电离室在 14.5 年中进行的 523 次活性测量确定的。这些数据是从总共 127 830 次电离电流测量中筛选和汇总的,其重现性标准偏差为 0.065%。电离电流是在空气电容器上收集的,并以电压随时间的变化进行测量。指数衰减曲线的残差显示出一个明显的年周期,振幅为 0.0055 (5)%,在补偿了与环境湿度的相关性后,降至 0.0012 (5)%。这些数据证实了指数衰减规律的有效性,在日标、月标和多年度标尺上都没有 0.0005 % 标准偏差的周期性扰动。本研究获得的 22Na 半衰期值为 950.68 (12) d 或 2.60290 (34) a,相对标准不确定性为 0.013 %。该值与文献中其他测量结果的平均值一致,尽管后者存在不确定性预算不完整的问题。由于统计精度高,系统误差的不确定性估计保守,这项工作获得的结果可作为可靠的参考值推荐使用。
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引用次数: 0
239Pu Fission Spectrum Cumulative Fission Product Yield Measurement Using Godiva IV Critical Assembly 利用戈迪瓦四临界组件测量 239Pu 裂变谱累积裂变产物当量
IF 3.7 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2024-02-01 DOI: 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 (>99%) 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.

对各种锕系元素的快中子诱发裂变产物产率进行精确的整体测量对应用核科学具有重要意义。这项工作的目标是改善 239Pu 裂变产物产率值的不确定性。在猝发模式下,使用 Godiva IV 临界组件在纯 239Pu (>99%) 靶件中诱发了裂变。辐照样品在 45 分钟内被转移到高分辨率 γ 射线探测器上。利用自动峰值搜索算法,通过衰变γ射线能量和半衰期来识别同位素。所确定的每种同位素的初始活度都被用来计算其裂变产物产率。
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引用次数: 0
Absolute Branching Ratios of Prominent γ Rays Following α Decay of 233U 233U α 衰变后主要 γ 射线的绝对分支比
IF 3.7 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2024-02-01 DOI: 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 (>99.98%) was separated from its decay products before preparation of a 4.74-mg/cm2 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 α-γ/α 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.

报告了能量从 97 到 366 千伏的 233U α 衰变中 19 个显著峰的γ 射线绝对分支比(发射概率)。支化比是通过α-γ巧合测量得到的,并归一化为α单体。在制备直径为 6 毫米、每平方厘米 4.74 毫克的硝酸铀箔之前,高纯度 233U 材料(99.98%)已与其衰变产物分离。这是自 1984 年以来首次报告支化比的绝对归一化,也是唯一通过 α-γ 重合度进行的测量,其中 α-γ/α 比值消除了一些潜在的系统偏差。总体而言,结果与所采用的文献一致,并验证了与裂变 233U 材料无损检测最相关的量,这与钍燃料循环和相关保障措施有关。
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引用次数: 0
Nuclear Data Sheets Symbols and Abbreviations 核数据表符号和缩略语
IF 3.7 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2024-02-01 DOI: 10.1016/S0090-3752(24)00014-0
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引用次数: 0
FENDL: A library for fusion research and applications FENDL:融合研究与应用图书馆
IF 3.7 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2024-02-01 DOI: 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.

核聚变评估数据图书馆(FENDL)是由国际原子能机构(IAEA)核数据部(NDS)协调的核截面数据的综合验证集合。FENDL 汇集了从现有核数据图书馆中挑选出的核聚变应用最佳核数据,已经开发了数十年。FENDL 包含入射中子、质子和氘核截面的子库,包括用于粒子输运和核素清单计算的通用文件和活化文件。在这项工作中,我们介绍了各种子库(中子、质子、氘核)的历史、评估选择(重点是输运和反应堆剂量测定应用)、应用代码(如 MCNP)的核数据处理以及 TENDL-2017 库的开发,该库是目前 FENDL 推荐使用的活化库。我们简要介绍了国际原子能机构 IRDFF 库,该库是剂量测定融合应用的推荐库。我们还介绍了利用 MCNP 传输代码和 ACE 格式截面库,使用各种核聚变相关计算和实验基准对中子子库进行验证的工作。验证工作使用了多种截面库,包括 FENDL-2.1、FENDL-3.1d、FENDL-3.2、ENDF/B-VIII.0 和 JEFF-3.2,重点是 FENDL 库。使用计算基准进行验证的结果表明,在中子通量、核加热和一次位移损伤 (dpa) 方面,经过测试的中子截面库之间普遍具有良好的一致性。结构材料中的气体产生量(H/He)与参考 FENDL-2.1 库有很大差异。实验验证的结果表明,FENDL-3.2b 的性能至少与 FENDL-2.1 相当,而且在大多数情况下都优于 FENDL-2.1。需要开发或更新协方差矩阵,因为随着聚变技术和设施建设的成熟,需要提供一致和全面的不确定性信息。最后,还需要对高能中子、质子和氘核进行额外的验证工作,以及对活化库进行验证工作。
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引用次数: 0
Normalization of ToF (n,f) Measurements in Fissile Targets: Microscopic cross-section integrals 裂变目标中 ToF (n,f) 测量的归一化:微观截面积分
IF 3.7 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2024-02-01 DOI: 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 σf0 and capture σγ0 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 I3 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) beV, respectively. The 235U normalization integral I3 derived in this work of 245.7(4.1) beV is in good agreement within quoted uncertainties with the Neutron Standards value of 247.5(3.0) beV.

Additional cross-section integrals I1 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 σf0/I1 and I3/I1 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 I3/I1 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 σ
对裂变目标中子诱导裂变的 ToF 收率测量进行精确归一化具有挑战性,但适当的归一化对于核能和临界安全等应用也至关重要。典型的归一化依赖于中子标准在热点(裂变 σf0 和俘获 σγ0 热截面)推荐的热中子常数 (TNC)。然而,许多 ToF 实验并不收集低至热能的数据,而是使用在不同任意能量区间定义的归一化截面积分。对于易裂变目标 233U、235U、239Pu 和 241Pu,建议在 8.1-14.7 eV、7.8-11 eV、9-20 eV 和 11.7-19.5 eV 间隔能量区使用归一化裂变截面积分 I3,其值分别等于 689.0(10.8)、245.7(4.1)、1059(6) 和 1378(33) b-eV。本研究得出的 235U 归一化积分 I3 为 245.7(4.1) b-eV,在引用的不确定度范围内与中子标准值 247.5(3.0) b-eV十分吻合。在 20-60 meV 的热区还得出了额外的截面积分 I1,以固定热点处裂变截面的归一化和斜率,为实验裂变产率的 R 矩阵评估提供额外的约束条件。由于分子和分母之间的强正相关性,σf0/I1 和 I3/I1 的比率具有极低的不确定性,并且首次得到了全面的推导。建议将积分比 I3/I1 分别为 39.31(54)、13.08(20)、41.65(22) 和 40.46(85),作为裂变目标 233U、235U、239Pu 和 241Pu 的参考。同样,σf0/I1 的比率为 30.40(18)、31.22(12)、29.58(7) 和 29.95(35),也被推荐作为相应裂变目标的参考。实验人员可以使用这些推荐比率对他们测量的薄靶裂变产率数据进行归一化处理,评估人员也可以使用这些比率对他们的 R 矩阵分析进行约束,这些 R 矩阵分析使用多组测量数据,并按照本工作中的建议进行了重新归一化处理。这种一致性保证了我们基于整个一致的 TOF 实验数据数据库对参考积分进行新评估的可靠性。
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引用次数: 0
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Nuclear Data Sheets
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