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Remeasurement of the 239Pu(n,f)/235U(n,f) Cross-Section Ratio with the NIFFTE fission Time Projection Chamber Using Vapor-deposited Targets NIFFTE裂变时间投射室用气相沉积靶重测239Pu(n,f)/235U(n,f)截面比
IF 2.8 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-05-13 DOI: 10.1016/j.nds.2025.04.003
The NIFFTE fission Time Projection Chamber (fissionTPC) has been used to measure the 239Pu(n,f)/235U(n,f) cross-section ratio for neutron-induced fission in the range of 0.1–100 MeV, with high precision. A white neutron source was provided by the Los Alamos Neutron Science Center, where the experiment was conducted as a remeasurement to evaluate a roughly 2% discrepancy of the previous fissionTPC results with ENDF/B-VIII.0. A detailed accounting of measurement uncertainties was performed, based on the fissionTPC's novel ability to provide three-dimensional reconstruction of fission-fragment ionization profiles. Current results obtained using a vapor-deposited, highly uniform 239Pu target, in comparison to the measurement published in 2021, where a 239Pu electroplated target was used, are presented and discussed. The remeasurement presented here is in agreement with the previous fissionTPC result within measurement uncertainties.
利用NIFFTE裂变时间投影室(fissionTPC)在0.1 ~ 100 MeV范围内测量了中子诱导裂变的239Pu(n,f)/235U(n,f)截面比,精度较高。一个白色中子源由洛斯阿拉莫斯中子科学中心提供,在那里进行了实验,作为重新测量,以评估之前的裂变tpc结果与ENDF/ b - vii .0的大约2%的差异。基于fissionTPC提供裂变碎片电离剖面三维重建的新能力,对测量不确定度进行了详细的计算。本文介绍并讨论了目前使用气相沉积、高度均匀的239Pu靶获得的结果,与2021年发表的使用239Pu电镀靶的测量结果进行了比较。在测量不确定度范围内,这里提出的再测量与先前的裂变tpc结果一致。
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引用次数: 0
Nuclear Structure and Decay Data for A=65 Isobars A=65等压线的核结构和衰变数据
IF 2.8 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-05-13 DOI: 10.1016/j.nds.2025.04.004
Jun Chen
Experimental nuclear structure and decay data are evaluated for 13 known nuclides of mass number A=65 (V, Cr, Mn, Fe, Co, Ni, Cu, Zn, Ga Ge, As, Se, Br). Detailed evaluated level properties and related information are presented and recommended spectroscopic parameters are provided, combining all the data from various reactions and decays. At the proton-rich end, 65Br has been studied theoretically but still remains unobserved experimentally, while at the neutron-rich end, 65V has been observed, but its ground-state T1/2 and Jπ wait to be measured and determined. No excited state has been observed for 65V, 65Cr, and 65Se. The ground-state spins and/or parities of 65Fe, 65Co, 65Ge, 65As, and 65Se still have not been definitely determined. Information for excited states in 65Mn and 65As is very limited. 65Cu is the most extensively studied via 26 different reactions and decays, followed by 65Zn and 65Ga. For 65Co and 65Ni, their radioactive decay schemes are incomplete. This work supersedes earlier full evaluations of A=65 published by 2010Br10, 1993Bh04, 1986Wa02, and 1975Au08.
对13种已知质量数为A=65的核素(V、Cr、Mn、Fe、Co、Ni、Cu、Zn、Ga、Ge、As、Se、Br)的实验核结构和衰变数据进行了评价。结合各种反应和衰变的所有数据,给出了详细的评价能级性质和相关信息,并提供了推荐的光谱参数。在富质子端,已经对65Br进行了理论研究,但仍未在实验中观测到;而在富中子端,已经观测到65V,但其基态T1/2和Jπ有待测量和确定。在65V、65Cr和65Se中未观察到激发态。65Fe、65Co、65Ge、65As和65Se的基态自旋和/或对偶仍然没有明确确定。关于65Mn和65As激发态的信息非常有限。通过26种不同的反应和衰变,对65Cu的研究最为广泛,其次是65Zn和65Ga。对于65Co和65Ni,它们的放射性衰变方案是不完整的。这项工作取代了早期发表于2010Br10、1993Bh04、1986Wa02和1975Au08的A=65的完整评估。
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引用次数: 0
High-precision Measurement of the 16O(n,n′γ) Cross Section using γ-ray Detection in Liquid Scintillators with H2O and BeO Targets 用γ射线检测水靶和BeO靶液体闪烁体16O(n,n′γ)截面的高精度测量
IF 2.8 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-05-13 DOI: 10.1016/j.nds.2025.04.001
K.J. Kelly, P.A. Copp, E.A. Bennett, M. Devlin, J.M. O'Donnell, M. Paris, H. Sasaki, R.O. Nelson, J. Surbrook, C. Arnold
The 16O(n,nγ) reaction was measured at the Los Alamos Neutron Science Center white neutron source using γ-ray detection in liquid scintillators present in the upper hemisphere of the Correlated Gamma-Neutron Array for sCattering (CoGNAC). Separate measurements of this reaction were performed using H2O and BeO targets in successive years. The unique high energies of γ rays emitted from the 16O(n,nγ) reaction facilitated a clean selection of this reaction from threshold to 9.8 MeV incident neutron energy without the need for precise measurements of the γ-ray energy or the scattered neutrons. The precise time resolution of the liquid scintillator detectors was then exploited to obtain high-resolution incident neutron energy measurements, and good agreement was obtained between the H2O and BeO results reported here. The dominant literature data sets for this reaction have systematic differences between them, but the present results improve upon the neutron energy resolution of earlier measurements and show important discrepancies in recent data. Tentative data are also shown up to 20 MeV incident neutron energy but are potentially subject to improved understanding of the relative γ-ray and α decay branches from 16O excited states.
在美国洛斯阿拉莫斯中子科学中心(Los Alamos Neutron Science Center)的白中子源上,利用相关伽玛-中子散射阵列(CoGNAC)上半球液体闪烁体中的γ射线探测,测量了16O(n,n’γ)反应。在连续的几年中,用H2O和BeO靶分别对该反应进行了测量。从16O(n,n ' γ)反应中发射的γ射线的独特高能量有助于在不需要精确测量γ射线能量或散射中子的情况下,从阈值到9.8 MeV入射中子能量的干净选择该反应。然后利用液体闪烁体探测器的精确时间分辨率来获得高分辨率的入射中子能量测量,并且在这里报道的H2O和BeO结果之间得到了很好的一致性。该反应的主要文献数据集之间存在系统差异,但目前的结果改进了早期测量的中子能量分辨率,并显示了最近数据的重要差异。暂定数据也显示了高达20 MeV的入射中子能量,但可能需要改进对来自16O激发态的相对γ射线和α衰变分支的理解。
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引用次数: 0
Nuclear Data Sheets Symbols and Abbreviations 核数据表符号和缩写
IF 2.8 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-04-07 DOI: 10.1016/S0090-3752(25)00030-4
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引用次数: 0
Recommended Nuclear Structure and Decay Data for A=206 Isobars A=206等压线的推荐核结构和衰变数据
IF 2.8 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-04-07 DOI: 10.1016/j.nds.2025.03.002
F.G. Kondev
Evaluated nuclear structure and decay data for all nuclei with mass number A=206 (206Pt, 206Au, 206Hg, 206Tl, 206Pb, 206Bi, 206Po, 206At, 206Rn, 206Fr, 206Ra and 206Ac), are presented. All available experimental data are compiled and evaluated, and best values for level and γ-ray energies, quantum numbers, lifetimes, γ-ray intensities and transition probabilities, as well as other nuclear properties, are recommended. Inconsistencies and discrepancies that exist in the literature are discussed. A number of computer codes (https://www-nds.iaea.org/public/ensdf_pgm/) developed by members of the NSDD network were used during the evaluation process. This work supersedes the earlier evaluation by F.G. Kondev (2008Ko21), published in Nuclear Data Sheets 109, 1527 (2008).
给出了所有质量数为A=206的原子核(206Pt, 206Au, 206Hg, 206Tl, 206Pb, 206Bi, 206Po, 206At, 206Rn, 206Fr, 206Ra和206Ac)的核结构评估和衰变数据。对所有可用的实验数据进行了汇编和评估,并推荐了能级和γ射线能量、量子数、寿命、γ射线强度和跃迁概率以及其他核性质的最佳值。讨论了文献中存在的不一致和差异。在评估过程中使用了由NSDD网络成员开发的一些计算机代码(https://www-nds.iaea.org/public/ensdf_pgm/)。这项工作取代了F.G. Kondev (2008Ko21)发表在《核数据表》109,1527(2008)上的早期评估。
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引用次数: 0
Nuclear Structure and Decay Data for A=32 Isobars A=32等压线的核结构和衰变数据
IF 2.8 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-04-07 DOI: 10.1016/j.nds.2025.03.001
Jun Chen
Experimental nuclear structure and decay data are evaluated for 9 known nuclides of mass number A=32 (F, Ne, Na, Mg, Al, Si, P, S, Cl, Ar). Detailed evaluated information is presented for each reaction and decay and recommended values combining all available data are provided for all spectroscopic properties of each level, γ transition, and decay radiation. Effort has been made to search for 32F (2019Ah07) with no success, suggesting unbound towards neutron emission. Information for excited states in 32Ne, 32Na and 32Ar are very limited, and spin-parity of 32Na remains undetermined experimentally; only a few excited states have been identified in 32Al, and the decay schemes of 32Mg β decay to 32Al and 32Al to 32Si are still incomplete; 32Mg, 32P and 32S have been studied via various reactions and decays, with 32S one of the most extensively studied nuclei in the sd-shell. This work supersedes earlier full evaluations of A=32 by 2011Ou01, 1998En04, 1990En08 and 1978En02.
对质量数为A=32的9种已知核素(F、Ne、Na、Mg、Al、Si、P、S、Cl、Ar)的实验核结构和衰变数据进行了评价。详细的评估信息提供了每个反应和衰变,并结合所有可用数据提供了每个能级,γ跃迁和衰变辐射的所有光谱特性的推荐值。人们已经努力寻找32F (2019Ah07),但没有成功,这表明它不受中子发射的束缚。32Ne、32Na和32Ar的激发态信息非常有限,32Na的自旋宇称仍未在实验中确定;在32Al中只发现了少数激发态,32Mg β−衰变到32Al和32Al到32Si的衰变方案仍然不完整;32Mg, 32P和32S已经通过各种反应和衰变进行了研究,其中32S是sd壳层中研究最广泛的原子核之一。这项工作取代了2011年01月、1998年04月、1990年08月和1978年02月对A=32的完整评估。
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引用次数: 0
Nuclear Data Sheets Symbols and Abbreviations 核数据表符号和缩写
IF 2.8 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-03-07 DOI: 10.1016/S0090-3752(25)00019-5
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引用次数: 0
Nuclear Data Sheets for A=154 A=154 的核数据表
IF 2.8 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-03-07 DOI: 10.1016/j.nds.2025.02.002
N. Nica
The experimental results published before Aug 2022 from the various reaction and decay studies leading to nuclides of Z=56 to Z=72, 154Ba, 154La, 154Ce, 154Pr, 154Nd, 154Pm, 154Sm, 154Eu, 154Gd, 154Tb, 154Dy, 154Ho, 154Er, 154Tm, 154Yb, 154Lu, 154Hf, in the A=154 mass chain have been reviewed. These data are collected and presented in decay or reaction datasets, together with Adopted Levels and gammas datasets that are the most extensive collections of nuclear structure data for each nuclide. This work is intended to supersede the previous evaluation of the A=154 nuclides by C.W. Reich (2009Re14), which was published in Nuclear Data Sheets 110, 2257 (2009).
本文综述了在2022年8月之前发表的各种反应和衰变研究的实验结果,这些实验结果导致了A=154质量链中Z=56至Z=72、154Ba、154La、154Ce、154Pr、154Nd、154Pm、154Sm、154Eu、154Gd、154Tb、154Dy、154Ho、154Er、154Tm、154Yb、154Lu、154Hf核素。这些数据是在衰变或反应数据集中收集和呈现的,以及采用的能级和伽马数据集,这些数据集是每种核素的最广泛的核结构数据集。这项工作旨在取代C.W. Reich (2009Re14)先前对A=154核素的评估,该评估发表在《核数据表》110,2257(2009)上。
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引用次数: 0
In Memory of Dr. Richard B. Firestone 纪念理查德-B-费尔斯通博士
IF 2.8 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-03-07 DOI: 10.1016/j.nds.2025.02.001
Jagdish Tuli , Lee Bernstein , Aaron Hurst , Shamsuzzoha Basunia
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引用次数: 0
Nuclear Structure and Decay Data for A=33 Isobars A=33等压线的核结构和衰变数据
IF 2.8 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR Pub Date : 2025-02-01 DOI: 10.1016/j.nds.2025.01.001
Jun Chen , Balraj Singh
Experimental structure and decay data are evaluated for eight known nuclides of mass number A=33 (Na, Mg, Al, Si, P, S, Cl, Ar). Experimental studies for the identification of other three nuclides: 33F, 33Ne and 33K by 2019Ah07, 2007Ba71, and 1986La17, respectively, have not met with success, and values of S(2n) for 33F, S(n) for 33Ne and S(p) for 33K from systematics (2021Wa16) and theoretical calculations (2019Mo01) suggest that these nuclei are likely unbound towards particle emission. Detailed evaluated level properties and related information are presented and recommended spectroscopic parameters are provided, combining all the data from various reactions and decays. Information for excited states in 33Na is limited and the spin of 33Al g.s. still has not been determined unambiguously. The radioactive decay schemes of 33Na, 33Mg, 33Al and 33Si remain incomplete. The 33S nuclide is the most extensively studied from many different reactions and decays, followed by 33Cl and 33P. This work supersedes earlier full evaluations of A=33 published by 2011Ch49, 1990En08 (also 1998En04 update) and 1978En02.
对8种已知质量数为A=33的核素(Na, Mg, Al, Si, P, S, Cl, Ar)的实验结构和衰变数据进行了评价。通过20119ah07、2007Ba71和1986La17分别鉴定33F、33Ne和33K三种核素的实验研究没有取得成功,从系统(2021Wa16)和理论计算(2019Mo01)得出的33F的S(2n)、33Ne的S(n)和33K的S(p)值表明,这些原子核可能不受粒子发射的约束。结合各种反应和衰变的所有数据,给出了详细的评价能级性质和相关信息,并提供了推荐的光谱参数。关于33Na激发态的信息是有限的,33Al g.s.的自旋仍然没有得到明确的确定。33Na、33Mg、33Al和33Si的放射性衰变谱尚不完整。在许多不同的反应和衰变中,对33S核素的研究最为广泛,其次是33Cl和33P。这项工作取代了早期发表于2011Ch49、1990En08(也是1998En04更新)和1978En02的A=33的完整评估。
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引用次数: 0
期刊
Nuclear Data Sheets
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