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論文

Measurements of circular polarization from the 0.75-eV p-wave resonance of the $$^{139}$$La(n,$$gamma$$)$$^{140}$$La reaction

遠藤 駿典; 藤岡 宏之*; 後藤 優*; 猪野 隆*; 岩本 修; 岩本 信之; 河村 しほり*; 木村 敦; 北口 雅暁*; 小林 龍珠; et al.

JPS Conference Proceedings (Internet), 45, p.011056_1 - 011056_8, 2026/06

https://doi.org/10.7566/JPSCP.45.011056

The NOPTREX collaboration aims to search for time-reversal symmetry breaking (T-violation) using compound nuclear reactions. To elucidate the mechanism of T-violation in compound nuclear reactions, we are measuring the spin-angle correlation term of the (n,$$gamma$$) reaction. We have already successfully measured the angular distribution and transverse asymmetry of emitted gamma-rays for several nuclei, such as $$^{139}$$La and $$^{117}$$Sn. As the next step, we measured the circular polarization of the emitted gamma-rays from the 0.75-eV p-wave resonance of $$^{139}$$La(n,$$gamma$$)$$^{140}$$La reactions. The measurements were performed at J-PARC MLF BL04 (ANNRI). The circular polarization of gamma-rays was measured using the developed gamma-ray polarimeter. Although the circular polarization observed was weak, this first measurement on the resonances allowed us to place limits on the circular polarization from the p-wave resonance. In this presentation, we will report the details of the experiment and future plans.

論文

Study of the distribution of partial radiative widths for the $$^{181}$$Ta(n,$$gamma$$)$$^{182}$$Ta reaction

河村 しほり*; 遠藤 駿典; 岩本 修; 岩本 信之; 木村 敦; 北口 雅暁*; 中村 詔司; 奥平 琢也*; Rovira Leveroni, G.; 清水 裕彦*

JPS Conference Proceedings (Internet), 45, p.011069_1 - 011069_7, 2026/06

https://doi.org/10.7566/JPSCP.45.011069

Random Matrix Theory (RMT) has been proposed to deal with the statistics of eigenvalues and eigenfunctions of complex many-body quantum systems. For the Gaussian orthogonal ensemble (GOE) of matrices, RMT is expected to correctly describe fluctuation properties of nuclear levels at relatively high excitations, such as near the neutron threshold. The reduced partial width amplitudes, which determine the strength of the coupling between a resonance and a particular channel, have a Gaussian probability distribution centered at zero, while the reduced partial widths (the squares of the partial width amplitudes) have a chi-square distribution with one degree of freedom: the Porter-Thomas distribution. The fluctuation properties of partial radiative widths have been measured and studied for many nuclides. For $$^{182}$$Ta, the results reported by Wasson et al. and Stelts et al. are inconsistent, and its fluctuation properties of widths are not precisely understood. One possible reason for this disagreement may arise from imprecise determination of the spins of the resonances. We therefore planned to determine the spins of the resonances from measurements and examine the statistical fluctuations of the partial radiative widths based on the results of spins. In this study, as a first step, we measured the gamma-rays emitted by neutron capture reactions of $$^{181}$$Ta at J-PARC MLF ANNRI (BL04) and confirmed the fluctuations of the radiative widths. Using the spins of the resonances listed in the nuclear data library, JENDL-5, the present result was consistent with that of Stelts et al. which deviated from the Porter-Thomas distribution.

論文

Measurements of neutron capture cross-sections for nuclides of interest in decommissioning (V); $$^{94}$$Zr(n, $$gamma$$)$$^{95}$$Zr and $$^{96}$$Zr(n, $$gamma$$)$$^{97}$$Zr reactions at JRR-3

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

Journal of Nuclear Science and Technology, 63(6), p.653 - 666, 2026/06

https://doi.org/10.1080/00223131.2025.2586632
 被引用回数：0 パーセンタイル：0.00(Nuclear Science & Technology)

Decommissioning of nuclear facilities generates a wide variety of wastes in large quantities. To make matters more complicated, they are radioactive wastes due to neutron activation. Thus, the neutron capture cross-sections of decommissioned nuclides are required to evaluate the produced radioactivity. This study selected $$^{95}$$Zr and $$^{97}$$Zr nuclides from the nuclides targeted for decommissioning, and aimed to measure the thermal-neutron capture cross-sections of $$^{94}$$Zr and $$^{96}$$Zr, which contribute to the production of $$^{95}$$Zr and $$^{97}$$Zr, respectively. Considering the relatively small cross-sections of Zr isotopes, measurements were performed by a neutron activation method using the pneumatic tube PN-3 of the Japan Research Reactor-3 (JRR-3) because its thermal-neutron flux is 250 times larger than that of the graphite thermal column of the Kyoto University Research Reactor. A natural Zr foil was irradiated in the PN-3 and subjected to $$gamma$$-ray spectrometry. The thermal-neutron capture cross-sections were derived according to Westcott's convention to be 50.9$$pm$$0.6 millibarns for the $$^{94}$$Zr(n,$$gamma$$)$$^{95}$$Zr reaction, and 21.9$$pm$$0.3 millibarns for the $$^{96}$$Zr(n,$$gamma$$)$$^{97}$$Zr reaction. These results are consistent with recent evaluation and experimental data. It was demonstrated that the thermal-neutron capture cross-section of the order of millibarns could be straightforwardly measured by using the PN-3 of JRR-3.

論文

Neutron capture cross-section measurements at TC-Pn in KUR for tungsten among nuclides in decommissioning

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

KURNS Progress Report 2025, P. 101, 2026/06

https://adm.rri.kyoto-u.ac.jp/pub/progressrep2/

本研究は、生成放射能を評価するために、廃止措置で問題となる核種について熱中性子捕獲断面積を測定するものである。本件では、対象核種の中から$$^{186}$$Wを選定し、京大原子炉にて放射化法によりその熱中性子捕獲断面積を測定した。今回、結果の再現性を確認するために2回の断面積測定を行い、$$^{186}$$W(n,$$gamma$$) $$^{187}$$W反応について43.5$$pm$$1.2 barns、43.1$$pm$$1.3 barnsを得た。従来の評価値38.1$$pm$$0.5 barnsは、1.4%ほど過小評価されている可能性がある。得られた断面積の結果の確かさを検証するために、Wを中性子束モニタとして使用した照射実験を1回実施した。今回得られた断面積の結果は、AuやCoモニタで求められる中性子束の結果と整合性のある中性子束を与えることを確認できた。

論文

Accurate measurement of the $$^{129}$$I neutron capture cross-section in the keV neutron region

Rovira Leveroni, G.; 木村 敦; 中村 詔司; 遠藤 駿典; 岩本 修; 岩本 信之; 片渕 竜也*

Journal of Nuclear Science and Technology, 63(4), p.358 - 369, 2026/04

https://doi.org/10.1080/00223131.2025.2543579
 被引用回数：0 パーセンタイル：0.00(Nuclear Science & Technology)

The $$^{129}$$I neutron capture cross-section was measured at the Accurate Neutron-Nucleus Reaction Measurement Instrument (ANNRI) beamline in the Materials and Life Science (MLF) facility of the Japan Proton Accelerator Research Complex (J-PARC). To obtain accurate results in the keV neutron region, the recently developed neutron filtering technique was employed with a 20-cm-thick $$^{nat}$$Si filter to tailor the incident neutron flux into quasi-monoenergetic neutron peaks with averaged neutron energies of 51.5 and 127.7 keV and, at the same time, hugely increase the signal-to-noise ratio. The present cross-section results were determined form the capture yield ratio of $$^{129}$$I to that of $$^{197}$$Au and using the evaluated nuclear data from JENDL-5 as reference. The $$^{129}$$I neutron capture cross section was found to be 0.278 $$pm$$ 0.034 b at 51.5 keV and 0.141 $$pm$$ 0.015 b 127.7 keV, validating the JENDL-5 and JEFF-3.3 evaluations, as well as the results from Noguere et al., in contrast to the larger evaluations of JENDL-4.0 and ENDF/B-VIII.1 and the data from Macklin et al.

論文

Neutron total and capture cross-section measurement and resolved resonance analysis of Er

Rovira Leveroni, G.; 木村 敦; 中村 詔司; 遠藤 駿典; 岩本 修; 岩本 信之; 片渕 竜也*

Annals of Nuclear Energy, 225, p.111688_1 - 111688_18, 2026/01

https://doi.org/10.1016/j.anucene.2025.111688
 被引用回数：0 パーセンタイル：0.00(Nuclear Science & Technology)

The neutron total and capture cross sections of $$^{nat}$$Er were measured at the Accurate Neutron-Nucleus Reaction Measurement Instrument beamline in the Materials and Life Science Experimental Facility of the Japan Proton Accelerator Research Complex. For the neutron total cross-section measurements, Li-glass detectors were employed to derive the neutron transmission ratio of three $$^{nat}$$Er transmission samples with thicknesses of 1 mm, 0.175 mm and 0.05 mm. The neutron capture cross-section was determined from measurements of 0.025-mm-thick $$^{nat}$$Er samples with NaI(Tl) and Ge spectrometers in separate experiments, since they offer complementary capabilities. Moreover, the capture cross-section of $$^{167}$$Er was derived below 1 eV, since it accounted for over 95% of the capture events in $$^{nat}$$Er. Finally, the resolved resonance region up to 65 eV was analyzed using the REFIT code. The resonance parameters of 20 $$^{167}$$Er resonances, together with one resonance for each $$^{164}$$Er and $$^{166}$$Er were determined in a least-square fit using a combination of both capture data and the transmission data from the thicker 1 mm and 0.175 mm samples. T

論文

Revised neutron capture cross section of $$^{204}$$Pb by combining activation method and high-precision thermal ionization mass spectrometry

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

Journal of Nuclear Science and Technology, 9 Pages, 2026/00

https://doi.org/10.1080/00223131.2026.2666320
 被引用回数：0 パーセンタイル：0.00(Nuclear Science & Technology)

In view of the requirement for accurate cross-section data of the stable Pb isotopes in order to discuss the neutron moderation effect and neutron economy in the design of accelerator-driven systems, the authors previously derived the thermal-neutron capture cross-section of $$^{204}$$Pb by using thermal ionization mass spectrometry to be 0.537$$pm$$0.030 barn. The uncertainty in the $$^{205}$$Pb/$$^{204}$$Pb isotope ratio determined by mass spectrometry was 4.3$$%$$, bringing the total uncertainty to 5.6$$%$$. This study demonstrated that a new silica-gel emitter used in mass spectrometry improved isotope ratio precision to 1$$%$$. This enabled us to determine the reaction rate with 1$$%$$ accuracy, which exceeds the accuracy of conventional activation analysis. Owing to improved accuracy in mass spectrometry, the uncertainty has been reduced and the value of isotope ratio has changed slightly. Accordingly, the authors report a revised $$^{204}$$Pb neutron capture cross-section of 0.512$$pm$$0.019 barn.

論文

Field-induced anomaly in the anisotropic non-Fermi-liquid normal state of UBe$$_{13}$$

清水 悠晴*; 橘高 俊一郎*; 河野 洋平*; 中村 翔太*; 芳賀 芳範; 山本 悦嗣; 町田 一成*; 網塚 浩*; 榊原 俊朗*

Physical Review B, 112(24), p.245157_1 - 245157_10, 2025/12

https://doi.org/10.1103/bxq6-tznr
 被引用回数：1 パーセンタイル：0.00(Materials Science, Multidisciplinary)

We report the results of high-resolution dc magnetization and specific heat measurements on the unconventional superconductor UBe$$_{13}$$.Suppression of the non-Fermi-liquid behavior under field and a nontrivial fifth-order magnetic susceptibility were observed at low temperatures, suggesting the Fermi-surface reconstruction accompanying the crossover from non-Fermi-liquid to Fermi-liquid state in UBe$$_{13}$$.

報告書

JAEA原災法対象施設における四足歩行ロボットの走行機能確認

渡辺 夏帆; 西山 裕; 今橋 正樹; 田口 祐司; 飯塚 由伸; 大内 卓哉; 井上 修一; 小澤 太教; 根本 隆弘; 菅谷 孝; et al.

JAEA-Testing 2025-001, 56 Pages, 2025/11

JAEA-Testing-2025-001.pdf:2.61MB

日本原子力研究開発機構(JAEA)福島廃炉安全工学研究所安全管理部遠隔機材運用課(旧:楢葉遠隔技術開発センター(Naraha Center for Remote Control Technology Development (NARREC))遠隔機材整備運用課)(以下「運用課」という。)所管の原子力緊急事態支援組織は、JAEA各拠点の防災業務計画に定められた遠隔機材を発災時に備え管理している。当該防災業務計画の対象は、原子力科学研究所のJRR-3 (Japan Research Reactor-3)、核燃料サイクル工学研究所の再処理施設、大洗原子力工学研究所の材料試験炉JMTR (Japan Materials Testing Reactor)、高温工学試験研究炉HTTR (High Temperature Engineering Test Reactor)及び高速実験炉常陽、高速増殖原型炉もんじゅ及び新型転換炉原型炉ふげんの7施設である。運用課は、令和3年度に当該7施設の想定発災事象・現場及び走行ルートの調査を行った。その結果、特定の現場において、現有のクローラタイプの走行ロボットの使用よりも操作要員の被ばくを低減できると判断し、令和4年度に四足歩行ロボットSpotを調達した。そして令和5年度に、当該各走行ルートにおいて、映像確認、階段走行等、Spotの機能が問題なく実行できるか、確認を行った。本報告書は、現地において令和5年度に確認試験を実施した6施設(JRR-3、JMTR、HTTR、常陽、もんじゅ及びふげん)について、その走行機能確認の結果を示したものである。

論文

Measurements of neutron capture cross-sections for nuclides of interest in decommissioning (IV); $$^{165}$$Ho(n,$$gamma$$)$$^{rm 166m,166g}$$Ho 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, 62(11), p.1086 - 1099, 2025/11

https://doi.org/10.1080/00223131.2025.2525327
 被引用回数：0 パーセンタイル：0.00(Nuclear Science & Technology)

During the decommissioning of nuclear facilities, large amounts of radioactive wastes are generated from structural materials. When considering the disposal or reuse of such wastes, accurate neutron capture cross-sections are required to evaluate the amounts of radioactive nuclides among the wastes. The present work selected $$^{165}$$Ho among nuclides included in the list for clearance levels in decommissioning, and measured the thermal-neutron capture cross-sections for the $$^{165}$$Ho(n,$$gamma$$)$$^{rm 166m}$$Ho, $$^{rm 166g}$$Ho reactions by the neutron activation method. The thermal cross-section measurements were performed with the graphite thermal column of the Kyoto University Research Reactor under the 5-MW operation and the thermal-neutron capture cross-sections were derived on the basis of Westcott's convention. In this work, a value of 2.79$$pm$$0.04 barn was obtained for the $$^{165}$$Ho(n,$$gamma$$)$$^{rm 166m}$$Ho reaction, and 61.2$$pm$$0.6 barn for the $$^{165}$$Ho(n,$$gamma$$)$$^{rm 166g}$$Ho reaction. The combination of these cross-sections presented 64.0$$pm$$0.6 barn, which supports the recent evaluated data of 64.69 barn and 64.4$$pm$$1.2 barn within the limit of uncertainties.

論文

Change in dislocation density via ausforming in Fe-5%Mn-C alloy with lath martensitic structure

高梨 美咲*; 日高 僚太*; 大久保 亘太*; 増村 拓朗*; 土山 聡宏*; 諸岡 聡; 前田 拓也*; 中村 修一*; 植森 龍治*

ISIJ International, 65(9), p.1384 - 1393, 2025/08

https://doi.org/10.2355/isijinternational.ISIJINT-2025-090
 被引用回数：1 パーセンタイル：26.96(Metallurgy & Metallurgical Engineering)

This study investigates the strengthening mechanism of ausforming in martensitic steels, focusing on the role of dislocation inheritance from austenite. By analyzing Fe-5%Mn-C alloys, the researchers quantified dislocation densities before and after ausforming and examined how carbon content affects hardening. Results show that both hardness and dislocation density of ausformed martensite increase with greater deformation in austenite and higher carbon content. The findings support that ausforming strengthens martensite through dislocation accumulation, consistent with the Bailey-Hirsch relationship. ${it In-situ}$ neutron diffraction revealed that dislocation inheritance occurs only in steels with sufficient carbon, while additional dislocations are introduced during martensitic transformation.

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, 62(7), p.617 - 630, 2025/07

https://doi.org/10.1080/00223131.2025.2457589
 被引用回数：2 パーセンタイル：70.03(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

Study of the spin-memory effect with low-energy gamma-rays in $$^{177}$$Hf(n,$$gamma$$)$$^{178}$$Hf reaction measurement

河村 しほり*; 遠藤 駿典; 岩本 修; 岩本 信之; 木村 敦; 北口 雅暁*; 中村 詔司; 奥平 琢也*; Rovira Leveroni, G.; 清水 裕彦*; et al.

EPJ Web of Conferences, 329, p.05002_1 - 05002_3, 2025/06

https://doi.org/10.1051/epjconf/202532905002
 被引用回数：0 パーセンタイル：0.00(Physics, Nuclear)

共鳴の全角運動量は低エネルギー核反応において重要なパラメータの一つである。実験から共鳴のJを推定する方法はいくつか提案されているが、本研究ではWetzelとThomasによって提案された、共鳴のガンマ線スペクトルにおいて、適切に選ばれた2つの低エネルギーガンマ線の強度比を比較する方法に着目した。この方法は、HuizengaとVandenboschによって提案されたスピンメモリー効果(SME)に基づいている。SMEとは、カスケード遷移において多くの中間励起準位が存在しても、初期の共鳴状態のスピン情報が残ることを意味する。強度比に現れるSMEの強さは、強度比の差から定量的に評価することができる。過去の測定結果から、原子番号Zがマジックナンバー(Z=50)付近でSMEが大きくなることが示唆されている。本研究ではZ=50から離れた元素である天然のHf(Z=72)を用いて、J-PARC・MLF・ANNRIにおいて中性子捕獲反応測定を行った。SMEの強さは、共鳴からの低エネルギー$$gamma$$線の強度比から決定された。その結果、Hf(Z=72)で観測されたSMEはTa(Z=73)よりも非常に大きいことがわかった。

論文

Circular polarization measurement of $$gamma$$-rays emitted from $$^{32}$$S(n,$$gamma$$)$$^{33}$$S reaction with polarized neutrons

遠藤 駿典; 藤岡 宏之*; 井出 郁央*; 飯沼 昌隆*; 岩本 信之; 岩本 修; 亀田 健斗*; 河村 しほり*; 木村 敦; 北口 雅暁*; et al.

EPJ Web of Conferences, 329, p.05003_1 - 05003_3, 2025/06

https://doi.org/10.1051/epjconf/202532905003
 被引用回数：0 パーセンタイル：0.00(Physics, Nuclear)

共鳴の全角運動量は核データにおいて重要なパラメータの一つであるが、その測定は困難な場合が多く、測定で決定されていないことが多い。本研究では共鳴の全角運動量を偏極中性子照射により発生したガンマ線の円偏光度の測定により決定する手法の確立を目指している。円偏光どの測定を行うためのガンマ線ポラリメータを開発し、J-PARC・MLF・ANNRIに設置し、偏極中性子入射による$$^{32}$$S(n,$$gamma$$)$$^{33}$$S反応における5.4MeVガンマ線の円偏光度の測定を行った。この5.4MeVのガンマ線は50%円偏光していることが知られており、このガンマ線を用いてポラリメータの円偏光度への感度であるAnalyzing Powerを決定することが目的である。測定の結果1%程度の差が確認され、ANNRIにて初めて円偏光度の測定に成功した。

論文

Neutron capture cross-section measurement at TC-Pn in KUR for holmium among nuclides in decommissioning

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

KURNS Progress Report 2024, P. 31, 2025/06

本研究は、生成放射能を評価するために、廃止措置で問題となる核種について熱中性子捕獲断面積を測定するものである。本件では、対象核種の中から$$^{166}$$Hoを選定し、京大原子炉にて放射化法によりその熱中性子捕獲断面積を測定した。今回、$$^{165}$$Ho(n,$$gamma$$)$$^{rm 166m}$$Ho反応について2.79$$pm$$0.04 barnを得た。従来の報告値は3.4$$pm$$0.5(b)に対して、誤差1.4$$%$$に向上して導出することができた。また副産物として、$$^{165}$$Ho(n,$$gamma$$)$$^{rm 166g}$$Ho反応について61.2$$pm$$0.6 barnを得た。$$^{rm 166m}$$Hoと$$^{rm 166g}$$Hoの生成の断面積を合わせて、64.0$$pm$$0.6 barnを求めた。今回の結果は、TOF法による過去の報告値64.4$$pm$$2.8(b)や、最近の評価値64.69 barn、64.4$$pm$$1.2 barnを誤差の範囲で支持した。

論文

Change in dislocation density via ausforming in Fe-5%Mn-C alloy with lath martensitic structure

高梨 美咲*; 日高 僚太*; 大久保 亘太*; 増村 拓朗*; 土山 聡宏*; 諸岡 聡; 前田 拓也*; 中村 修一*; 植森 龍治*

鉄と鋼, 111(9), p.503 - 513, 2025/06

https://doi.org/10.2355/tetsutohagane.TETSU-2024-092
 被引用回数：0 パーセンタイル：0.00(Metallurgy & Metallurgical Engineering)

The strengthening mechanism of ausforming in martensitic steels is believed to be due to the inheritance of dislocations in austenite by the subsequently transformed martensite. However, no studies to date have quantified the dislocation density before and after ausforming. In this study, the dislocation densities of Fe-5%Mn-C alloys were analyzed, and the relationship between hardening by ausforming and dislocation accumulation, as well as the effect of carbon on this relationship, were investigated. The hardness of ausformed martensite increased with the ausforming reduction in austenite, and the strengthening effect of ausforming increased with the addition of carbon. Similarly, the dislocation density of ausformed martensite increased with the ausforming reduction in austenite, and the dislocation accumulation by ausforming increased with the addition of carbon. Because the hardness of the ausformed martensite follows the Bailey-Hirsch relationship, the strengthening mechanism owing to ausforming could be explained by dislocation strengthening. To understand the dislocation accumulation process during ausforming, the dislocation density of austenite immediately after ausforming was measured by in-situ heating neutron diffraction. Consequently, the dislocation density of the ausformed austenite was not dependent on the carbon content, indicating that dislocations are not inherited in carbon-free steels. By contrast, in steels with sufficient carbon content, not only are dislocations inherited but additional dislocations are introduced during martensitic transformation.

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：2 パーセンタイル：38.41(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

福島第一原子力発電所廃炉作業への貢献とソースターム予測技術向上におけるFP挙動に関する技術課題に対する取り組み

勝村 庸介*; 高木 純一*; 宮原 直哉*; 内田 俊介*; 駒 義和; 唐澤 英年; 三輪 周平; 佐藤 志彦; 永井 晴康; 倉田 正輝; et al.

日本原子力学会誌ATOMO$$Sigma$$, 67(2), p.128 - 132, 2025/02

https://doi.org/10.3327/jaesjb.67.2_128

本研究専門委員会では、東京電力ホールディングス株式会社福島第一原子力発電所(1F)事故後の核分裂生成物(FP)挙動を予測可能な技術に高めて廃炉作業に貢献することと、1F事故進展事象の把握で得られた情報をソースターム(ST)の予測技術の向上に反映させ、原子炉安全の一層の向上に繋げることを目標とした活動を実施している。最初の2年間は、1F廃炉における燃料デブリやFP挙動の予測、およびST予測精度向上に必要な、今後取り組むべき技術課題を摘出した。2023年度からは、本専門委員会を延長し、取り組むべき技術課題に対応した3つのワーキンググループを結成し、技術課題の解決に向けた検討を進めている。本報告では2023年度の活動での検討内容について報告する。

論文

Spin current generation due to differential rotation

船戸 匠*; 木下 俊一郎*; 棚橋 典大*; 中村 真*; 松尾 衛

Physical Review B, 111(6), p.L060403_1 - L060403_7, 2025/02

https://doi.org/10.1103/PhysRevB.111.L060403
 被引用回数：3 パーセンタイル：63.37(Materials Science, Multidisciplinary)

We study nonequilibrium spin dynamics in differentially rotating systems, deriving an effective Hamiltonian for conduction electrons in the comoving frame. In contrast to conventional spin current generation mechanisms that require vorticity, our theory describes spins and spin currents arising from differentially rotating systems regardless of vorticity. We demonstrate the generation of spin currents in differentially rotating systems, such as liquid metals with Taylor-Couette flow. Our alternative mechanism will be important in the development of nanomechanical spin devices.

論文

Pulsed muon facility of J-PARC MUSE

下村 浩一郎*; 幸田 章宏*; Pant, A. D.*; 砂川 光*; 藤森 寛*; 梅垣 いづみ*; 中村 惇平*; 藤原 理賀; 反保 元伸*; 河村 成肇*; et al.

Interactions (Internet), 245(1), p.31_1 - 31_6, 2024/12

https://doi.org/10.1007/s10751-024-01863-8
 被引用回数：4 パーセンタイル：90.22(Physics, Atomic, Molecular & Chemical)

J-PARC Muon Facility: MUSE (Muon Science Establishment) is responsible for the inter-university user program and the operation, maintenance, and construction of the muon beamlines, namely D-line, S-line, U-line, and H-line, along with the muon source at J-PARC Materials and Life Science Facility (MLF). In this paper, recent developments are briefly presented.

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