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論文

Measurements of neutron capture cross-section for nuclides of interest in decommissioning (II); $$^{58}$$Fe(n,$$gamma$$)$$^{59}$$Fe

中村 詔司; 芝原 雄司*; 遠藤 駿典; Rovira Leveroni, G.; 木村 敦

Journal of Nuclear Science and Technology, 62(3), p.300 - 307, 2025/03

https://doi.org/10.1080/00223131.2024.2427244
 被引用回数：0 パーセンタイル：0.00(Nuclear Science & Technology)

As nuclear facilities are dismantled in decommissioning, large amount of various waste is generated. Even more inconveniently, waste is radioactive due to neutron activation. Thus, the neutron capture cross-sections of nuclides targeted in decommissioning are required to evaluate the radioactivity produced. In this work, $$^{58}$$Fe nuclide was selected among objective nuclides for decommissioning, and its thermal-neutron capture cross-section was measured by a neutron activation method at the graphite thermal column of Kyoto University Research Reactor in 5-MW operation. The thermal-neutron capture cross-section was derived using ${it Westcott'}$s convention. The present work obtained 1.36$$pm$$0.03 barns for the $$^{58}$$Fe(n,$$gamma$$)$$^{59}$$Fe reaction. The present result supports the JENDL-5 evaluation within 2$$sigma$$. If updated with currently recommended nuclear data, some of the reported past data would support the present result.

論文

Verification of direct coupling code system using FRENDY version 2 and GENESIS for light water reactor lattices

藤田 達也; 山本 章夫*

Journal of Nuclear Science and Technology, 62(2), p.179 - 196, 2025/02

https://doi.org/10.1080/00223131.2024.2410918
 被引用回数：0 パーセンタイル：0.00(Nuclear Science & Technology)

本研究では、核反応断面積の摂動に伴う間接効果を考慮したランダムサンプリングに基づく不確かさ定量化を容易に実施可能とするため、核データ処理コードFRENDYバージョン2と3次元非均質中性子輸送計算コードGENESISからなる直接結合コードシステム(FRENDY-V2/GENESIS)を新たに構築した。GENESIS用に準備された多群断面積はFRENDYバージョン2により生成された。Dancoff係数はneutron current methodにより計算した。次に、Carlvik二項有理近似に基づいて背景断面積を計算した。FRENDY-V2/GENESISの計算精度を検証するため、無限中性子増倍率(k-infinity)とUO$$_{2}$$及びMOX燃料格子体系における核分裂反応率分布をMVP3と比較した。また、キャラクタリスティックス法のレイトレーシング等の離散化条件に関する感度解析も併せて実施した。FRENDY-V2/GENESISとMVP3の比較を通して、SHEM361群構造に基づくFRENDY-V2/GENESISは、k-infinityを約50pcm以内、核分裂反応率分布を平均二乗偏差で約0.1%以内で計算可能であった。以上の結果から、FRENDY-V2/GENESISの適用性が検証された。今後は、FRENDY-V2/GENESISは多群断面積の摂動に伴う間接効果に係る議論に活用される。

論文

Measurements of neutron capture cross-section for nuclides of interest in decommissioning (III); $$^{170}$$Er(n,$$gamma$$)$$^{171}$$Er and $$^{180}$$Hf(n,$$gamma$$)$$^{181}$$Hf reactions

中村 詔司; 芝原 雄司*; 遠藤 駿典; Rovira Leveroni, G.; 木村 敦

Journal of Nuclear Science and Technology, 14 Pages, 2025/00

https://doi.org/10.1080/00223131.2025.2457589
 被引用回数：0 パーセンタイル：0.00(Nuclear Science & Technology)

In the decommissioning of nuclear facilities, large amounts of radioactive waste are generated due to neutron activation. In that case, neutron capture cross-sections of nuclides targeted in decommissioning are required to evaluate their radioactivities produced. The present study selected two nuclides, $$^{171}$$Er and $$^{181}$$Hf, among objective ones for decommissioning, and thermal-neutron capture cross-sections for their parent nuclides were measured by the neutron activation method at the Kyoto University Research Reactor under 1-MW operation. The thermal-neutron capture cross-sections were derived on the basis of Westcott's convention. The present study obtained the results as follows: 8.19$$pm$$0.35 barns for the $$^{170}$$Er(n,$$gamma$$)$$^{171}$$Er reaction and 13.57$$pm$$0.14 barns for the $$^{180}$$Hf(n,$$gamma$$)$$^{181}$$Hf reaction. As a by-product, the measurements of the Hf sample also yielded 0.427$$pm$$0.006 barns for the $$^{179}$$Hf(n,$$gamma$$)$$^{180m}$$Hf reaction. This study revealed that some experimental and data evaluations differ from the present results by more than the experimental uncertainties.

論文

Measurements of neutron capture cross-sections for nuclides of interest in decommissioning; $$^{45}$$Sc, $$^{63}$$Cu, $$^{64}$$Zn, $$^{109}$$Ag, and $$^{113}$$In

中村 詔司; 芝原 雄司*; 遠藤 駿典; Rovira Leveroni, G.; 木村 敦

Journal of Nuclear Science and Technology, 61(11), p.1415 - 1430, 2024/11

https://doi.org/10.1080/00223131.2024.2346347
 被引用回数：1 パーセンタイル：57.00(Nuclear Science & Technology)

廃止措置においては、生成放射能の評価に資する核データとして、中性子捕獲断面積を整備する必要がある。本研究では、整備すべき対象核種のうち$$^{45}$$Sc, $$^{63}$$Cu, $$^{65}$$Zn, $$^{109}$$Ag及び$$^{113}$$Inを選定し、KURのTC-Pnを用いてそれらの熱中性子捕獲断面積測定を行った。その結果、熱中性子捕獲断面積の結果が、以下のとおり得られた:$$^{45}$$Sc(n, $$gamma$$)$$^{46}$$Sc反応は27.18$$pm$$0.28 barn、$$^{63}$$Cu(n, $$gamma$$)$$^{64}$$Cu反応は4.34$$pm$$0.06 barn、$$^{64}$$Zn(n, $$gamma$$)$$^{65}$$Zn反応は0.719$$pm$$0.011 barn、$$^{109}$$Ag(n, $$gamma$$)$$^{rm 110m}$$Ag反応は4.05$$pm$$0.05 barn、そして$$^{113}$$In(n, $$gamma$$) $$^{114}$$In$$^{m1+m2}$$反応は8.53$$pm$$0.27 barn。ScとZnの結果は、これまでに報告されている評価値を誤差範囲で支持するが、一方、他の核種については評価値と異なる結果となった。得られた結果は、生成量評価にはもちろん、これらの核種を中性束モニタとして利用する場合に用いることが考えられる。

論文

An Evaluation on Inelastic Thermal Neutron Scattering Cross-Section Data of Crystalline Graphite

沖田 将一朗; 安部 豊*; 田崎 誠司*; 深谷 裕司

Radioisotopes, 73(3), p.233 - 240, 2024/11

https://doi.org/10.3769/radioisotopes.73.233

In the latest nuclear data libraries ENDF/B-VIII.0 and JENDL-5, the inelastic scattering cross-section data for reactor graphite and crystalline graphite are employed. The data for reactor graphite reproduces the measurement values very well, while the data for crystalline graphite tends to underestimate the measurement values, and there is room for improvement. Therefore, in the present study, for future updates of JENDL, a new molecular dynamics simulation model for crystalline graphite is prepared and inelastic scattering cross-section data are evaluated based on both incoherent approximation and Vineyard approximation. As a result, the obtained inelastic scattering cross-section data of crystalline graphite show very good agreement with the measured data and successfully presented more reliable data than those employed in ENDF/B-VIII.0 and JENDL-5.

論文

Shedding light on the origin of $$^{204}$$Pb, the heaviest $$s$$-process; Only isotope in the solar system

Casanovas-Hoste, A.*; 原田 秀郎; 木村 敦; 他130名*

Physical Review Letters, 133(5), p.052702_1 - 052702_8, 2024/07

https://doi.org/10.1103/PhysRevLett.133.052702
 被引用回数：3 パーセンタイル：48.32(Physics, Multidisciplinary)

$$^{204}$$Tl(n, $$gamma$$) cross section was measured at the CERN neutron time-of-flight facility n_TOF, employing a sample of only 9 mg of $$^{204}$$Tl produced at the Institute Laue Langevin high flux reactor. At the $$s$$-process temperatures of kT $$approx$$ 8 keV and kT $$approx$$ 30 keV, Maxwellian-averaged cross sections (MACS) of 580(168) mb and 260(90) mb, respectively. These figures are about 3% lower and 20% higher than the corresponding values widely used in astrophysical calculations, which were based only on theoretical calculations. By using the new $$^{204}$$Tl MACS, the uncertainty arising from the $$^{204}$$Tl(n, $$gamma$$) cross section on the $$s$$-process abundance of $$^{204}$$Pb has been reduced from $$sim$$30% down to +8%/-6%, and the $$s$$-process calculations are in agreement with the latest solar system abundance of $$^{204}$$Pb reported by K. Lodders in 2021.

論文

Total and double differential scattering cross-section measurements of isotropic graphite

木村 敦; 遠藤 駿典; 中村 詔司

EPJ Web of Conferences, 294, p.01002_1 - 01002_7, 2024/04

https://doi.org/10.1051/epjconf/202429401002

The total and double differential scattering cross sections (DDSCS) of graphite have been measured in the Materials and Life Science Experimental Facility (MLF) in the J-PARC. The DDSCS were measured using the Beam Line No.14 (AMATERAS) in the MLF. The data were normalized using those of vanadium as a standard. Small angle scattering and Bragg edges were observed, and their intensities varied among the samples. The neutron total cross sections in the energy region from 1 to 100 meV were measured using Beam Line No.04 (ANNRI) in the MLF. In the epithermal range (over 40 meV), all samples tended to have values close to the free atom cross-section of graphite. However, at the first Bragg edge, the deduced total cross sections by those samples started to separate from each other. The difference became more significant with decreasing the neutron energy, and the value tended to increase with the grain size of the sample. The results of these measurements suggest that the discrepancies between the derived total cross sections in the low-energy region are due to small-angle scattering caused by grains of graphite with uniform size.

論文

Measurement of nuclide production cross sections for GeV-region proton-induced reactions on $$^{rm nat}$$Mg, $$^{rm nat}$$Si, $$^{rm nat}$$Fe, $$^{rm nat}$$Cu, and $$^{rm nat}$$Zn

杉原 健太*; 明午 伸一郎; 岩元 大樹; 前川 藤夫

Nuclear Instruments and Methods in Physics Research B, 549, p.165299_1 - 165299_12, 2024/04

https://doi.org/10.1016/j.nimb.2024.165299
 被引用回数：0 パーセンタイル：0.00(Instruments & Instrumentation)

Nuclide production cross sections for proton-induced reactions on $$^{rm nat}$$Mg, $$^{rm nat}$$Si, $$^{rm nat}$$Fe, $$^{rm nat}$$Cu and $$^{rm nat}$$Zn at several GeV were measured using an activation technique at Japan Proton Accelerator Research Complex. The aggregate results of 250 cross sections were successfully acquired. The data obtained in this study were compared with the results from nuclear reaction models in PHITS and the data retrieved from Japanese Evaluated Nuclear Data Library High Energy file 2007 (JENDL/HE-2007). Among all of the models, INCL/GEM, JENDL/HE-2007, and JAM/GEM generally showed the good agreement.

論文

Measurements of the neutron total and capture cross sections and derivation of the resonance parameters of $$^{181}$$Ta

遠藤 駿典; 木村 敦; 中村 詔司; 岩本 修; 岩本 信之; Rovira Leveroni, G.; 藤 暢輔; 瀬川 麻里子; 前田 亮

Nuclear Science and Engineering, 198(4), p.786 - 803, 2024/04

https://doi.org/10.1080/00295639.2023.2227826
 被引用回数：1 パーセンタイル：25.62(Nuclear Science & Technology)

The neutron transmission ratio and capture yield for $$^{181}$$Ta were measured in J-PARC MLF ANNRI to improve the accuracy of resonance parameters. The total cross section was determined from the transmission ratio in the energy range from 0.2 to 150 eV. The capture cross section was obtained from the capture yield using the pulse height weighting technique (PHWT) in the energy range from thermal to 150 eV. The obtained transmission ratio and capture cross-section were fitted by the resonance analysis code, REFIT, and the resonance parameters were determined below 150 eV. It was also discussed the correlations caused by fitting based on statistical uncertainty and correlations for systematic uncertainty based on sample thickness in the transmission measurements.

論文

A Comparative study of efficient sampling techniques for uncertainty quantification due to cross-section covariance data

藤田 達也

Proceedings of International Conference on Physics of Reactors (PHYSOR 2024) (Internet), p.718 - 727, 2024/04

https://doi.org/10.13182/PHYSOR24-43640

ランダムサンプリング法に基づく不確かさ評価における中性子無限増倍率の不確かさの収束過程を、複数の効率化サンプリング手法間で比較した。中性子無限増倍率の不確かさは、JENDL-5の断面積共分散データに基づく摂動ACEファイルを用いたSERPENT 2.2.1計算を多数回実施し、これを統計処理することにより評価した。本論文では、対称サンプリング(AS)、ラテン超方格サンプリング(LHS)、制御変量法(CV)及びこれらの併用手法に着目した。既往研究で議論されたように、PWR-UO$$_{2}$$燃料集合体体系においてAS及びLHSはこれらを用いない通常のサンプリングよりも高効率の収束を示した。CVについては、単独での適用時は中性子無限増倍率の不確かさの収束過程に大きくは影響しなかったが、既往研究で示されるとおり、ASと併用することで収束性能が改善した。また本論文では、LHSとCVによる新たな併用手法(CV+LHS)を提案した。CV+LHSは、中性子無限増倍率の不確かさの収束傾向を改善し、これはCV+ASよりも高効率であった。当該改善傾向の主な理由は、LHSを適用することにより、CVにおける代替パラメータの平均値の収束性が向上したためであると考えられる。以上から、本研究ではCV+LHSを新しい併用手法として提案し、PWR-UO$$_{2}$$燃料集合体体系におけるランダムサンプリング法に基づく不確かさ評価においてその効率性を確認した。CV+LHSの核種燃焼計算への適用性については、今後の研究で確認する予定である。

論文

Measurement of the $$^{140}$$Ce(n, $$gamma$$) cross section at n_TOF and its astrophysical implications for the chemical evolution of the universe

Amaducci, S.*; 原田 秀郎; 木村 敦; 他130名*

Physical Review Letters, 132(12), p.122701_1 - 122701_8, 2024/03

https://doi.org/10.1103/PhysRevLett.132.122701
 被引用回数：4 パーセンタイル：68.78(Physics, Multidisciplinary)

$$^{140}$$Ce(n,$$gamma$$) is a key reaction for slow neutron-capture ($$s$$-process) nucleosynthesis due to being a bottleneck in the reaction flow. For this reason, it was measured with high accuracy (uncertainty $$approx$$ 5%) at the n_TOF facility, with an unprecedented combination of a high purity sample and low neutron-sensitivity detectors. The measured Maxwellian averaged cross section is up to 40% higher than previously accepted values. Stellar model calculations indicate a reduction around 20% of the s-process contribution to the Galactic cerium abundance and smaller sizeable differences for most of the heavier elements. No variations are found in the nucleosynthesis from massive stars.

論文

New JENDL-4.0/HE neutron and proton ACE files

今野 力

Journal of Nuclear Science and Technology, 61(1), p.121 - 126, 2024/01

https://doi.org/10.1080/00223131.2023.2237970
 被引用回数：1 パーセンタイル：25.62(Nuclear Science & Technology)

JENDL-4.0/HEの中性子と陽子ACEファイルは2017年に作られ、そのうちの22核種の中性子ACEファイルと25核種の陽子ACEファイルがPHITSコードと一緒に公開されている。最近、JENDL-4.0/HEの中性子と陽子ACEファイルに入っている以下の5つのデータに問題があることが見つかった; $$^{15}$$Nと$$^{18}$$OのACEファイル、発熱数、損傷エネルギー生成断面積、2次中性子多重度、核分裂断面積。そこで、これらの問題を修正したJENDL-4.0/HEの新しい中性子と陽子ACEファイルを作成した。この論文では問題点及び新しい中性子と陽子ACEファイルをどのように作成したかについて詳述する。

論文

Measurements of neutron total and capture cross sections of $$^{139}$$La and evaluation of resonance parameters

遠藤 駿典; 河村 しほり*; 奥平 琢也*; 吉川 大幹*; Rovira Leveroni, G.; 木村 敦; 中村 詔司; 岩本 修; 岩本 信之

European Physical Journal A, 59(12), p.288_1 - 288_12, 2023/12

https://doi.org/10.1140/epja/s10050-023-01203-4
 被引用回数：2 パーセンタイル：45.98(Physics, Nuclear)

ランタン(La)-139の断面積と共鳴パラメータは、原子力分野への応用や基礎核物理の研究にとって重要である。本論文では、大強度陽子加速器施設(J-PARC)のANNRIにてLaの中性子全断面積と捕獲断面積を測定した。Negative共鳴を含む4つの共鳴の共鳴パラメータを、共鳴解析コードREFITを用いて求めた。その結果いくつかの共鳴パラメータにおいて、評価済み核データライブラリとの不一致が見られた。さらに全断面積を再現するために、スピン依存する散乱半径もフィットした。得られた散乱半径は、評価済み核データライブラリで記録されたものよりも大きいことがわかった。

論文

Measurement of nuclide production cross sections for proton-induced reactions on $$^{nat}$$Ti and $$^{93}$$Nb at 0.8 and 3.0 GeV

杉原 健太*; 明午 伸一郎; 岩元 大樹; 前川 藤夫

Nuclear Instruments and Methods in Physics Research B, 545, p.165153_1 - 165153_9, 2023/12

https://doi.org/10.1016/j.nimb.2023.165153
 被引用回数：2 パーセンタイル：46.61(Instruments & Instrumentation)

The nuclide production cross sections for proton-induced reactions on $$^{nat}$$Ti and $$^{93}$$Nb at 0.8 and 3.0 GeV were measured using an activation technique at Japan Proton Accelerator Research Complex. A total of 27 and 94 nuclide production cross sections for the $$^{nat}$$Ti(p,X) and $$^{93}$$Nb(p,X) reactions were obtained, respectively. The present data were compared with the results from nuclear reaction models in PHITS and data retrieved from Japanese Evaluated Nuclear Data Library High Energy file 2007 (JENDL/HE-2007). The prediction accuracy of JENDL/HE-2007 was the best for the $$^{7}$$Be production cross section of both targets. As an overall trend, underestimation of INCL and all of the models were confirmed for the $$^{nat}$$Ti(p,X) and $$^{93}$$Nb(p,X) reactions, respectively.

論文

An Estimation method for an unknown covariance in cross-section adjustment based on unbiased and consistent estimator

丸山 修平; 遠藤 知弘*; 山本 章夫*

Journal of Nuclear Science and Technology, 60(11), p.1372 - 1385, 2023/11

https://doi.org/10.1080/00223131.2023.2203707
 被引用回数：1 パーセンタイル：25.62(Nuclear Science & Technology)

A new estimation method of an unknown covariance, which is defined by the difference between the true covariance (the population covariance) and a prior covariance assumed by an analyst, is proposed. The unknown covariance is estimated using an empirical covariance consistent with the observed data. To estimate the unknown covariance, an unbiased and consistent estimator in regression analysis has been incorporated into the conventional cross-section adjustment. This estimator does not require assumptions for the probability distribution of the observation data. The statistical properties of this estimator were numerically verified. In addition, the effectiveness of the proposed method was confirmed by another numerical test using actual integral experimental data. In the second numerical test, the modeling uncertainty (covariance) due to the deterministic analysis method was assumed to be unknown. The results showed that the proposed method could practically estimate the unknown covariance and adjusted cross-sections using only prior information on covariances.

論文

Measurements of capture cross-section of $$^{93}$$Nb by activation method and half-life of $$^{94}$$Nb by mass analysis

中村 詔司; 芝原 雄司*; 遠藤 駿典; 木村 敦

Journal of Nuclear Science and Technology, 60(11), p.1361 - 1371, 2023/11

https://doi.org/10.1080/00223131.2023.2198526
 被引用回数：3 パーセンタイル：62.75(Nuclear Science & Technology)

廃止措置の対象核種の中から$$^{93}$$Nbについて、熱中性子捕獲断面積($$sigma$$$$_{0}$$)および共鳴積分(I$$_{0}$$)を放射化法により測定した。また、$$^{94}$$Nbの半減期を質量分析により測定した。ニオブ93試料は、京都大学複合原子力科学研究所の研究炉に整備されている水圧輸送艦を用いて照射した。金-アルミ合金線、およびコバルト-アルミ合金線を用いて、照射位置における中性子束成分を測定した。厚さ25$$mu$$mのガドリニウム箔を用いた照射も行って、熱および熱外中性子による反応率の寄与をより分けた。ガドリニウムの厚さから、カットオフ・エネルギーは0.133eVに設定した。ニオブ試料中に含まれている不純物により生成される$$^{182}$$Taの放射能を減衰させるために、約2年間ニオブ試料を冷却した。$$gamma$$線スペクトロスコピーにより照射されたニオブ試料およびモニタの生成放射能を測定した。Westcottコンベンションに基づいて解析を行い、$$sigma$$$$_{0}$$およびI$$_{0}$$を、それぞれ1.11$$pm$$0.04barnおよび10.5$$pm$$0.6barnと導出することができた。$$gamma$$線測定の後に、ニオブ試料の質量分析を行い、反応率を導出した。$$gamma$$線スペクトロスコピーと質量分析で得られたデータを組み合わせることにより、$$^{94}$$Nbの半減期を、(2.00$$pm$$0.15)$$times$$10$$^{4}$$年と導出することができた。

論文

Review of JENDL/HE-2007 neutron-induced fission cross sections of uranium-235 and 238 above 200 MeV

深堀 智生

INDC(JPN)-210 (Internet), 5 Pages, 2023/10

$$^{235}$$U(n,f)の断面積値がENDF形式に正しく編集されておらず、間違った値がJENDL/HE-2007ファイルに格納・配布されている。JENDL/HE-2007ライブラリの$$^{235}$$U(n,f)断面積の高エネルギー部分は、FISCALコードの計算結果を使用して評価されている。このレポートでは、200MeV以上のJENDL/HE-2007ライブラリの正しい$$^{235}$$U(n,f)断面積値が示されている。

論文

Measurement of the neutron-induced fission cross section of $$^{230}$$Th at the CERN n_TOF facility

Michalopoulou, V.*; 原田 秀郎; 木村 敦; 他134名*

Physical Review C, 108(1), p.014616_1 - 014616_15, 2023/07

https://doi.org/10.1103/PhysRevC.108.014616
 被引用回数：2 パーセンタイル：45.98(Physics, Nuclear)

The neutron-induced fission cross section of $$^{230}$$Th has been measured at the neutron time-of-flight facility n_TOF located at CERN. The experiment was performed at the experimental area EAR-1 with a neutron flight path of 185 m, using Micromegas detectors for the detection of the fission fragments. The $$^{230}$$Th(n,f) cross section was determined relative to the $$^{235}$$U(n, f) one, covering the energy range from the fission threshold up to 400 MeV. The results from the present work are compared with existing cross-section datasets and the observed discrepancies are discussed and analyzed.

論文

Neutron total and capture cross-section measurements of $$^{155}$$Gd and $$^{157}$$Gd in the thermal energy region with the Li-glass detectors and NaI(Tl) spectrometer installed in J-PARC$$cdot$$MLF$$cdot$$ANNRI

木村 敦; 中村 詔司; 遠藤 駿典; Rovira Leveroni, G.; 岩本 修; 岩本 信之; 原田 秀郎; 片渕 竜也*; 寺田 和司*; 堀 順一*; et al.

Journal of Nuclear Science and Technology, 60(6), p.678 - 696, 2023/06

https://doi.org/10.1080/00223131.2022.2134224
 被引用回数：2 パーセンタイル：29.47(Nuclear Science & Technology)

Neutron total and capture cross-section measurements of $$^{155}$$Gd and $$^{157}$$Gd were performed in the ANNRI at the MLF of the J-PARC. The neutron total cross sections were determined in the energy region from 5 to 100 meV. At the thermal neutron energy, the total cross sections were obtained to be 59.4$$pm$$1.7 and 251.9$$pm$$4.6 kilobarn for $$^{155}$$Gd and $$^{157}$$Gd, respectively. The neutron capture cross sections were determined in the energy region from 3.5 to 100 meV with an innovative method by taking the ratio of the detected capture event rate between thin and thick samples. At the thermal energy, the capture cross sections were obtained as 59.0$$pm$$2.5 and 247.4$$pm$$3.9 kilobarn for $$^{155}$$Gd and $$^{157}$$Gd, respectively. The present total and capture cross sections agree well within the standard deviations. The results for $$^{155}$$Gd were found to be consistent with the values in JENDL-4.0 and the experimental data given by Mastromarco et al. and Leinweber et al. within one standard deviation. Moreover, the present results for $$^{157}$$Gd agreed with the evaluated data in JENDL-4.0 and the experimental data by M${o}$ller et al. within one standard deviation and agreed with the data by Mastromarco et al. within 1.4 standard deviations. However, they disagree (11% larger) with the experimental result by Leinweber et al.

論文

Measurement of the $$^{77}$$Se(n,$$gamma$$) cross section up to 200 keV at the n_TOF facility at CERN

Sosnin, N. V.*; 原田 秀郎; 木村 敦; 他128名*

Physical Review C, 107(6), p.065805_1 - 065805_9, 2023/06

https://doi.org/10.1103/PhysRevC.107.065805
 被引用回数：1 パーセンタイル：0.00(Physics, Nuclear)

The $$^{77}$$Se(n,$$gamma$$) reaction is of importance for $$^{77}$$Se abundance during the slow neutron capture process in massive stars. We have performed a new measurement of the $$^{77}$$Se radiative neutron capture cross section at the Neutron Time-of-Flight facility at CERN. Resonance capture kernels were derived up to 51 keV and cross sections up to 200 keV. Maxwellian-averaged cross sections were calculated for stellar temperatures between kT = 5 keV and kT = 100 keV, with uncertainties between 4.2% and 5.7%. Our results lead to substantial decreases of 14% and 19% in $$^{77}$$Se abundances produced through the slow neutron capture process in selected stellar models, compared to using previous recommendation of the cross section.

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