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論文

Development of a dissolution method for analyzing the elemental composition of fuel debris using sodium peroxide fusion technique

中村 聡志; 石井 翔*; 加藤 仁*; 伴 康俊; 蛭田 健太; 吉田 拓矢; 上原 寛之; 小畑 裕希; 木村 康彦; 高野 公秀

Journal of Nuclear Science and Technology, 62(1), p.56 - 64, 2025/01

https://doi.org/10.1080/00223131.2024.2381553
 被引用回数：1 パーセンタイル：57.00(Nuclear Science & Technology)

過酸化ナトリウム(Na$$_{2}$$O$$_{2}$$)融解処理法を用いた燃料デブリの元素組成分析法を検討した。融解処理条件として、2種類の模擬デブリ試料((Zr,RE)O$$_{2}$$の固溶体及び溶融炉心-コンクリート相互作用生成物(MCCI)など)を用いて融解処理温度及びるつぼ材について検討した。検討の結果、るつぼ材にNiを用いて、923Kで融解処理を行うことが最適な処理条件であることが示唆された。これを受けて、TMI-2デブリを用いたコンクリートセルでの実証試験に適用し、燃料デブリの完全溶解を確認した。得られたTMI-2デブリ溶解液の元素組成は再現性に優れ、SEM/WDX及びXRDによる分析結果と良好な一致を示し、妥当性を確認した。したがって、本手法は燃料デブリの元素組成分析において、有効であると考えられる。

論文

Extraordinary $$^{99}$$Mo adsorption; Utilizing spray-dried mesoporous alumina for clinical-grade generator development

Alowasheeir, A.*; 江口 美陽*; 藤田 善貴; 土谷 邦彦; 若林 隆太郎*; 木村 辰雄*; 有賀 克彦*; 籏野 健太郎*; 福光 延吉*; 山内 悠輔*

Bulletin of the Chemical Society of Japan, 97(10), p.uoae099_1 - uoae099_7, 2024/10

https://doi.org/10.1093/bulcsj/uoae099
 被引用回数：3 パーセンタイル：37.20(Chemistry, Multidisciplinary)

EO$$_{n}$$PO$$_{m}$$EOn$$_{n}$$の自己集合及び噴霧乾燥により合成されたメソポーラスアルミナ粒子は、臨床グレードのモリブデン-99/テクネチウム-99m($$^{99}$$Mo/$$^{99m}$$Tc)ジェネレータの開発に利用されてきた。メソポーラスアルミナ粒子のMo吸着性能を評価した結果、市販のアルミナ粒子よりも効果的にMoイオンを吸着した。本メソポーラスアルミナ粒子の合成方法における界面活性剤の除去方法がMo吸着特性に及ぼす影響についてバッチ法により系統的に調べた。その結果、Mo吸着容量は45.9から91.2mg-Mo/gであり、Mo吸着容量の高い条件から順に「溶媒抽出したままのアルミナ、焼成(400$$^{circ}$$C及び800$$^{circ}$$C)後のアルミナ、市販アルミナ」であることが分かった。さらに、臨床グレードのジェネレータへの適用性を評価するため、新たにタンデムカラムジェネレータの条件を採用して試験した結果、噴霧乾燥して抽出したメソポーラスアルミナを用いたジェネレーターから溶出した$$^{99m}$$Tcは高い放射核種純度、放射化学的純度、化学純度を示し、$$^{99m}$$Tc標識放射性医薬品の調製に適していることを明らかにした。

論文

Continuous structural phase transition and antiferromagnetic order in ilmenite-type NiVO$$_{3}$$

山本 孟*; 池田 理*; 本田 孝志*; 木村 健太*; 青山 拓也*; 大串 研也*; 鈴木 昭夫*; 石井 賢司*; 松村 大樹; 辻 卓也; et al.

Physical Review Materials (Internet), 8(9), p.094402_1 - 094402_6, 2024/09

https://doi.org/10.1103/PhysRevMaterials.8.094402
 被引用回数：2 パーセンタイル：56.91(Materials Science, Multidisciplinary)

We investigate the crystal and electronic structures as well as magnetic properties of ilmenite-type NiVO$$_{3}$$, which has attracted research interest as an ${it S}$ = 1 honeycomb lattice magnet. Ilmenite-type NiVO$$_{3}$$ samples were synthesized under high-pressure and high-temperature conditions. Synchrotron X-ray diffraction and Rietveld refinement results demonstrated that NiVO$$_{3}$$ underwent a continuous structural phase transition from the triclinic (${it P$bar{1}$}$) phase to the rhombohedral (${it R$bar{3}$}$) phase at 450 K. This transition is concomitant with the decomposition of the V-V dimers formed by the tetravalent V ions. X-ray absorption spectroscopy measurements confirmed that the Ni and V ions were divalent and tetravalent, respectively. Magnetic and specific heat measurements revealed that NiVO$$_{3}$$ underwent an antiferromagnetic transition at 140 K, and a zigzag-type magnetic order with magnetic propagation vector ${it k}$=(0,1/2,0) was observed by neutron diffraction measurements.

論文

Ferroaxial transitions in glaserite-type Na$$_2$$Ba${it M}$(PO$$_4$$)$$_2$$ (${it M}$ = Mg, Mn, Co, and Ni)

梶田 遥一*; 永井 隆之*; 山岸 茂直*; 木村 健太*; 萩原 雅人; 木村 剛*

Chemistry of Materials, 36(15), p.7451 - 7458, 2024/08

https://doi.org/10.1021/acs.chemmater.4c01406
 被引用回数：2 パーセンタイル：56.91(Chemistry, Physical)

Ferroaxial transitions of Na$$_{2}$$Ba${it M}$(PO$$_{4}$$)$$_{2}$$ (${it M}$ = Mg, Mn, Co, and Ni) with the glaserite structure, featuring rotational distortions of PO$$_{4}$$ tetrahedra, are investigated. Neutron powder diffraction (NPD) measurements on polycrystalline samples were carried out in the temperature range from room temperature to 800 K. Structure analyses on the NPD data revealed that all of the compounds studied here have a ferroaxial structure (space group: ${it P}$ $$bar{3}$$)at room temperature and undergo a ferroaxial transition into a non-ferroaxial phase (space group: ${it P}$ $$bar {3}$$${it m}$1) upon heating. Structural parameters change continuously at the transition temperature, which suggests that the ferroaxial transition of Na$$_{2}$$Ba${it M}$(PO$$_{4}$$)$$_{2}$$ systems is of the second order. Furthermore, to examine the structural stability, ab initio phonon calculations were carried out for Na$$_{2}$$BaMg(PO$$_{4}$$)$$_{2}$$. The calculated result shows that the rotational phonon mode instability inherent in the non-ferroaxial ${it P}$ $$bar{3}$$${it m}$1 phase leads to the ${it P}$ $$bar{3}$$ phases as a ground state, which well explains the experimental result. This study revealed that Na$$_{2}$$Ba${it M}$ (PO$$_{4}$$)$$_{2}$$ systems with the glaserite structure are a class of ferroaxial compounds showing a second-order pure ferroaxial transition.

論文

Laser-based angle-resolved photoemission spectroscopy with micrometer spatial resolution and detection of three-dimensional spin vector

岩田 拓万*; 高佐 永遠*; 西岡 幸美*; 大和田 清貴*; 角田 一樹; Annese, E.*; 鹿子木 将明*; 黒田 健太*; 岩澤 英明*; 有田 将司*; et al.

Scientific Reports (Internet), 14, p.127_1 - 127_8, 2024/01

https://doi.org/10.1038/s41598-023-47719-z
 被引用回数：7 パーセンタイル：89.50(Multidisciplinary Sciences)

We have developed a state-of-the-art apparatus for laser-based spin- and angle-resolved photoemission spectroscopy with micrometer spatial resolution ($$rm mu$$-SARPES). This equipment is achieved through the combination of a high-resolution photoelectron spectrometer, a 6-eV laser with high photon flux that is focused down to a few micrometers, a high-precision sample stage control system, and a double very-low-energy-electron-diffraction spin detector. The setup achieves an energy resolution of 1.5 (5.5) meV without (with) the spin detection mode, compatible with a spatial resolution better than 10 $$rm mu$$m. This enables us to probe both spatially-resolved electronic structures and vector information of spin polarization in three dimensions. The performance of $$rm mu$$-SARPES apparatus is demonstrated by presenting ARPES and SARPES results from topological insulators and Au photolithography patterns on a Si (001) substrate.

論文

Ferroaxial transitions in glaserite-type compounds; Database screening, phonon calculations, and experimental verification

山岸 茂直*; 林田 健志*; 三澤 龍介*; 木村 健太*; 萩原 雅人; 村田 智城*; 廣瀬 左京*; 木村 剛*

Chemistry of Materials, 35(2), p.747 - 754, 2023/01

https://doi.org/10.1021/acs.chemmater.2c03540
 被引用回数：9 パーセンタイル：67.40(Chemistry, Physical)

The so-called "ferroaxial transition" characterized by a rotational structural distortion that breaks a mirror symmetry has gained growing interest in terms of a new class of ferroic state in crystalline materials. RbFe(MoO$$_{4}$$)$$_{2}$$ which belongs to glaserite-type compounds, X□;1 Y□;2 [M(TO$$_{4})_{2}$$], is one of the most representative materials showing a ferroaxial transition, i.e., ferroaxial materials. Considering a variety of glaserite-type compounds, we expect that they provide a good arena for ferroaxial materials. In this work, we explored new ferroaxial materials by formula-based screening using regular expression search and symmetry detection algorithm. As a result, we found that a glaserite-type compound, K$$_{2}$$Zr(PO$$_{4}$$)$$_{2}$$, is one of the promising candidates for ferroaxial materials. Experimentally, we demonstrate that K$$_{2}$$Zr(P O$$_{4}$$)$$_{2}$$ shows a ferroaxial transition at about 700 K, which is well explained by ab initio phonon calculations. The ferroaxial nature of K$$_{2}$$Zr(PO$$_{4}$$)$$_{2}$$ is further confirmed by the observation of its domain structures using a linear electrogyration effect, that is, optical rotation in proportion to an applied electric field. Our work provides an effective approach to exploring ferroaxial materials.

論文

Phase transition and domain formation in ferroaxial crystals

林田 健志*; 上村 洋平*; 木村 健太*; 松岡 悟志*; 萩原 雅人; 廣瀬 左京*; 盛岡 仁*; 長谷川 達夫*; 木村 剛*

Physical Review Materials (Internet), 5(12), p.124409_1 - 124409_10, 2021/12

https://doi.org/10.1103/PhysRevMaterials.5.124409
 被引用回数：33 パーセンタイル：83.95(Materials Science, Multidisciplinary)

The ferroaxial order, which is characterized by a rotational structural distortion in a crystal, has been recently proposed as one of ferroic orders. Though the domain formation is a characteristic feature in ferroic materials, there has been little study done concerning that for the ferroaxial order. Here, we investigate ferroaxial domains that are formed through a ferroaxial transition in two representative ferroaxial materials, NiTiO$$_{3}$$ and RbFe(MoO$$_{4}$$)$$_{2}$$. We spatially resolve their domain structures using an optical method based on electric-field- induced optical rotation, that is, electrogyration (EG). In NiTiO$$_{3}$$, multi-domains are constructed when crystals undergo a ferroaxial transition and the domain size depends on the cooling rate around the transition temperature. Furthermore, the ferroaxial domain structure obtained by the EG measurement is well matched with that by scanning X-ray diffraction (XRD). RbFe(MoO$$_{4}$$)$$_{2}$$ also exhibits multi-domain states in which domain patterns are different each time a crystal undergoes a ferroaxial transition. In addition, the temperature dependence of the EG signal well obeys that of the order parameter of a first-order phase transition. These results ensure the effectiveness of the EG effect to elucidate the nature of ferroaxial order.

論文

Coexistence of magnetoelectric and antiferroelectric-like orders in Mn$$_{3}$$Ta$$_{2}$$O$$_{8}$$

木村 健太*; 八木 直輝*; 長谷川 舜介*; 萩原 雅人; 三宅 厚志*; 徳永 将史*; Cao, H.*; 益田 隆嗣*; 木村 剛*

Inorganic Chemistry, 60(20), p.15078 - 15084, 2021/10

https://doi.org/10.1021/acs.inorgchem.1c02461
 被引用回数：3 パーセンタイル：22.10(Chemistry, Inorganic & Nuclear)

In materials showing a linear magnetoelectric (ME) effect, unconventional functionalities can be anticipated such as electric control of magnetism and nonreciprocal optical responses. Thus, the search of new linear ME materials is of interest in materials science. Here, using a recently proposed design principle of linear ME materials, which is based on the combination of local structural asymmetry and collinear antiferromagnetism, we demonstrate that an anion-deficient fluorite derivative Mn$$_{3}$$Ta$$_{2}$$O$$_{8}$$ is a new linear ME material. This is evidenced by the onset of magnetic-field-induced electric polarization in its collinear antiferromagnetic phase below $$T_{rm N}$$ = 24 K. Furthermore, we also find an antiferroelectric-like phase transition at $$T_{rm S}$$ = 55 K, which is attributable to an off-center displacement of magnetic Mn$$^{2+}$$ ions. The present study shows that Mn$$_{3}$$Ta$$_{2}$$O$$_{8}$$ is a rare material that exhibits both ME and antiferroelectric-like transitions. Thus, Mn$$_{3}$$Ta$$_{2}$$O$$_{8}$$ may provide an opportunity to investigate the physics associated with complicated interactions between magnetic (spin) and electric dipole degrees of freedom.

論文

Nature of the Dirac gap modulation and surface magnetic interaction in axion antiferromagnetic topological insulator MnBi$$_{2}$$Te$$_{4}$$

Shikin, A. M.*; Estyunin, D. A.*; Klimovskikh, I. I.*; Filnov, S. O.*; Kumar, S.*; Schwier, E. F.*; 宮本 幸治*; 奥田 太一*; 木村 昭夫*; 黒田 健太*; et al.

Scientific Reports (Internet), 10, p.13226_1 - 13226_13, 2020/08

https://doi.org/10.1038/s41598-020-70089-9
 被引用回数：73 パーセンタイル：95.57(Multidisciplinary Sciences)

Modification of the gap at the Dirac point (DP) in axion antiferromagnetic topological insulator MnBi$$_{2}$$Te$$_{4}$$ and its electronic and spin structure have been studied by angle- and spin-resolved photoemission spectroscopy (ARPES) under laser excitation at various temperatures, light polarizations and photon energies. We have distinguished both large and reduced gaps at the DP in the ARPES dispersions, which remain open above the N$'{e}$el temperature of $$T_textrm{N}$$ = 24.5 K. We propose that the gap above $$T_textrm{N}$$ remains open due to a short-range magnetic field generated by chiral spin fluctuations. Spin-resolved ARPES, XMCD and circular dichroism ARPES measurements show a surface ferromagnetic ordering for the large gap sample and apparently significantly reduced effective magnetic moment for the reduced gap sample.

論文

Materials and Life Science Experimental Facility (MLF) at the Japan Proton Accelerator Research Complex, 2; Neutron scattering instruments

中島 健次; 川北 至信; 伊藤 晋一*; 阿部 淳*; 相澤 一也; 青木 裕之; 遠藤 仁*; 藤田 全基*; 舟越 賢一*; Gong, W.*; et al.

Quantum Beam Science (Internet), 1(3), p.9_1 - 9_59, 2017/12

https://doi.org/10.3390/qubs1030009

J-PARC物質・生命科学実験施設の中性子実験装置についてのレビューである。物質・生命科学実験施設には23の中性子ビームポートがあり21台の装置が設置されている。それらは、J-PARCの高性能な中性子源と最新の技術を組み合わせた世界屈指の実験装置群である。このレビューでは、装置性能や典型的な成果等について概観する。

論文

Simultaneous measurement of neutron-induced fission and capture cross sections for $$^{241}$$Am at neutron energies below fission threshold

廣瀬 健太郎; 西尾 勝久; 牧井 宏之; 西中 一朗*; 太田 周也*; 永山 達郎*; 田村 信行*; 後藤 真一*; Andreyev, A. N.; Vermeulen, M. J.; et al.

Nuclear Instruments and Methods in Physics Research A, 856, p.133 - 138, 2017/06

https://doi.org/10.1016/j.nima.2016.12.021
 被引用回数：5 パーセンタイル：39.65(Instruments & Instrumentation)

Fission and capture reactions were simultaneously measured in the neutron-induced reactions of $$^{241}$$Am at J-PARC. Data were taken with the TOF method in $$E_n$$ = 0.1$$sim$$20 eV. The fission events were observed by detecting prompt fission neutrons using liquid organic scintillators. The capture reaction was measured by detecting $$gamma$$ rays from the compound nuclei using the same detectors, where the prompt fission neutrons and capture $$gamma$$ rays were separated by a pulse shape analysis. The cross sections were obtained by normalizing the relative yields at the first resonance to evaluations or other experimental data. The ratio of the fission to capture cross sections at each resonance is compared with those from an evaluated nuclear data library and other experimental data. Some differences were found between the present values and the library/literature values at several resonances.

論文

Misassigned neutron resonances of $$^{142}$$Nd and stellar neutron capture cross sections

片渕 竜也*; 松橋 泰平*; 寺田 和司; 井頭 政之*; 水本 元治*; 廣瀬 健太郎; 木村 敦; 岩本 信之; 原 かおる*; 原田 秀郎; et al.

Physical Review C, 91(3), p.037603_1 - 037603_5, 2015/03

https://doi.org/10.1103/PhysRevC.91.037603
 被引用回数：8 パーセンタイル：48.21(Physics, Nuclear)

Time-of-flight spectra of the neutron capture events of $$^{142}$$Nd were measured using a spallation neutron source at the Japan Proton Accelerator Research Complex. The first six resonances of $$^{142}$$Nd reported in a previous work were not observed. The experimental results and cross-search of resonance energies in nuclear data libraries suggested that resonances of impurity nuclide $$^{141}$$Pr have been mistakenly assigned as $$^{142}$$Nd in the previous experiment. To investigate the impact of non-existence of the resonances to the s-process nucleosynthesis model, the Maxwellian averaged neutron capture cross sections with and without the misassigned resonances were compared.

論文

Response function for the measurement of (n,$$gamma$$) reactions with the ANNRI-Cluster Ge detectors at J-PARC

原 かおる; 後神 進史*; 原田 秀郎; 廣瀬 健太郎; 木村 敦; 金 政浩*; 北谷 文人; 小泉 光生; 中村 詔司; 藤 暢輔; et al.

JAEA-Conf 2014-002, p.88 - 92, 2015/02

https://doi.org/10.11484/jaea-conf-2014-002

Recently, neutron shields of a large Ge detector array at the Accurate Neutron-Nucleus Reaction Measurement Instrument (ANNRI) in the Japan Proton Accelerator Research Complex (J-PARC) were modified to suppress the background from boron rubber sheets to enriched $$^{6}$$LiF tiles. For the new experimental set-up, efficiencies and response functions of the cluster Ge detectors with the BGO anti-coincidence detectors were measured with $$gamma$$-rays from standard sources and prompt $$gamma$$-rays from the $$^{28}$$Si(n,$$gamma$$) and $$^{35}$$Cl(n,$$gamma$$) reactions. The simulation parameters were adjusted with the EGS5 code so as to reproduce the data set of efficiencies and response functions. Based on this information, a pulse height weighting function will be deduced in the energy range of 0.1-10 MeV.

論文

A Round robin propgram of master curve evaluation using miniature C(T) specimens, 3; Comparison of $$T_{0}$$ under various selections of temperature conditions

山本 真人*; 木村 晃彦*; 鬼沢 邦雄; 吉本 賢太郎*; 小川 琢矢*; 馬渕 靖宏*; Viehrig, H.-W.*; 三浦 直樹*; 曽根田 直樹*

Proceedings of 2014 ASME Pressure Vessels and Piping Conference (PVP 2014) (DVD-ROM), 7 Pages, 2014/07

https://doi.org/10.1115/PVP2014-28898

破壊靭性評価のためのマスターカーブ法は、最近試験規格として標準化され、原子炉圧力容器の信頼性を確保するための強力なツールであると期待されている。現行の監視試験において、マスターカーブ法のためのデータを得るためには、シャルピー試験片の試験後の半片から採取可能な小型の試験片の活用が重要である。著者らは、4mm厚のミニチュア破壊靭性試験片(微小C(T))によるマスターカーブ法の適用性を検証するため、典型的な日本の原子炉圧力容器鋼を用いて、国内の学界、産業界や研究機関の参加を得てラウンドロビン試験を進め、微小C(T)の有効性を確認した。本報ではブラインド試験により試験温度の選択を各研究機関が独自に行った結果を取りまとめ、試験温度依存性を比較した。その結果、得られた参照温度$$T_{0}$$には大きな相違はなく、破壊靭性評価にあたって試験温度の選択は大きな影響を及ぼさないことが確認できた。

論文

Measurements of capture $$gamma$$ rays from the neutron resonances of $$^{74}$$Se and $$^{77}$$Se at the J-PARC/MLF/ANNRI

堀 順一*; 八島 浩*; 中村 詔司; 古高 和禎; 原 かおる; 原田 秀郎; 廣瀬 健太郎; 木村 敦; 北谷 文人; 小泉 光生; et al.

Nuclear Data Sheets, 119, p.128 - 131, 2014/05

https://doi.org/10.1016/j.nds.2014.08.036
 被引用回数：4 パーセンタイル：31.39(Physics, Nuclear)

本研究では、$$^{74}$$Seと$$^{77}$$Seの中性子共鳴からの捕獲$$gamma$$線を測定した。$$^{74}$$Seは、簡単な殻模型から2p$$_{1/2}$$軌道まで中性子が占有されている偶-偶核であるので、プライマリ$$gamma$$線遷移の始状態と終状態間の強い相関が予想される。$$^{74}$$Seは、安定Se同位体の中で唯一の奇数核であるので、同じ奇数核である$$^{79}$$Seの評価に資する情報を含んでいると期待される。J-PARC、物質・生命科学実験施設(MLF)の中性子核反応実験装置(ANNRI)に整備した4$$pi$$ Geスペクトロメータを用いて、飛行時間法により測定を行った。$$^{74}$$Seの27eV共鳴、及び$$^{77}$$Seの113eV, 212eV, 291eV, 342eV, 690eV及び864eV共鳴に対応する$$gamma$$線波高スペクトルを得た。これらのプライマリ遷移$$gamma$$線の相対強度を求め、報告されている実験データと比較を行った。$$^{74}$$Seの27eV共鳴について、293keV準位への強いプライマリ遷移が観測された。$$^{77}$$Seについては、共鳴ごとに全く異なる崩壊パターンを見いだした。

論文

Cross section measurement of $$^{237}$$Np$$(n,gamma)$$ at J-PARC/MLF/ANNRI

廣瀬 健太郎; 古高 和禎; 原 かおる; 原田 秀郎; 堀 順一*; 井頭 政之*; 加美山 隆*; 片渕 竜也*; 木村 敦; 金 政浩*; et al.

Nuclear Data Sheets, 119, p.48 - 51, 2014/05

https://doi.org/10.1016/j.nds.2014.08.015
 被引用回数：1 パーセンタイル：9.62(Physics, Nuclear)

The cross section of the $$^{237}$$Np$$(n,gamma)$$ reaction has been measured in an energy range from 10 meV to 1 keV at the Japan Proton Accelerator Research Complex (J-PARC). The NaI(Tl) spectrometer installed in the accurate neutron-nucleus reaction measurement instrument (ANNRI) was used for the measurement. The relative cross section was obtained using the neutron spectrum measured by the $$^{10}$$B$$(n,alpha_1)$$ reaction. The absolute value of the cross section was deduced by normalizing the relative cross section to the evaluated value in JENDL-4.0 at the first resonance. In this presentation, the obtained results for the cross section, the Westcott factor and the resonance analysis are reported. This work was supported by JSPS KAKENHI Grant Number 22226016.

論文

Capture cross-section measurement of $$^{241}$$Am(n,$$gamma$$) at J-PARC/MLF/ANNRI

原田 秀郎; 太田 雅之; 木村 敦; 古高 和禎; 廣瀬 健太郎; 原 かおる; 金 政浩*; 北谷 文人; 小泉 光生; 中村 詔司; et al.

Nuclear Data Sheets, 119, p.61 - 64, 2014/05

https://doi.org/10.1016/j.nds.2014.08.019
 被引用回数：19 パーセンタイル：74.09(Physics, Nuclear)

Accurate determination of the neutron capture cross sections of radioactive nuclei is required in the fields of nuclear waste transmutation study and also nuclear astrophysics. The accurate neutron-nucleus reaction measurement instrument (ANNRI), which was installed in the materials and life science experimental facility (MLF) at the J-PARC, is expected to satisfy these demands. The capture cross section of $$^{241}$$Am was measured using a high efficiency Ge spectrometer installed in the ANNRI. By taking advantage of its high $$gamma$$-ray energy resolution, background components were precisely subtracted. The capture cross section of $$^{241}$$Am was deduced for a neutron energy region between 0.01 and 20 eV. The obtained cross section and the Westcott factor are compared with the preceding experiments and evaluated values.

論文

Cross section measurements of the radioactive $$^{107}$$Pd and stable $$^{105,108}$$Pd nuclei at J-PARC/MLF/ANNRI

中村 詔司; 木村 敦; 北谷 文人; 太田 雅之; 古高 和禎; 後神 進史*; 原 かおる; 原田 秀郎; 廣瀬 健太郎; 金 政浩*; et al.

Nuclear Data Sheets, 119, p.143 - 146, 2014/05

https://doi.org/10.1016/j.nds.2014.08.040
 被引用回数：10 パーセンタイル：55.12(Physics, Nuclear)

長寿命放射性核種$$^{107}$$Pd、及び不純物として含まれている安定核種$$^{105,108}$$Pdの中性子捕獲断面積を測定した。J-PARCの物質・生命科学実験施設(MLF)のBL04に整備された中性子核反応実験装置(ANNRI)を用いて、飛行時間法により熱領域から300eVの中性子エネルギーに対して、中性子捕獲断面積を測定した。報告されていた幾つかの共鳴が、$$^{107}$$Pdに起因しないことなど、共鳴に関する新たな知見が得られた。

論文

Measurements of neutron capture cross sections of $$^{112}$$Sn and $$^{118}$$Sn with J-PARC/MLF/ANNRI

木村 敦; 廣瀬 健太郎; 中村 詔司; 原田 秀郎; 原 かおる; 堀 順一*; 井頭 政之*; 加美山 隆*; 片渕 竜也*; 木野 幸一*; et al.

Nuclear Data Sheets, 119, p.150 - 153, 2014/05

https://doi.org/10.1016/j.nds.2014.08.042
 被引用回数：5 パーセンタイル：36.43(Physics, Nuclear)

The neutron-capture cross sections of $$^{112}$$Sn and $$^{118}$$Sn were measured by the time-of-flight method in the energy range from 10 meV to 2 keV with an array of germanium detectors in ANNRI at J-PARC. The preliminary results of the neutron-capture cross sections for $$^{112}$$Sn and $$^{118}$$Sn were obtained by normalizing the relative cross sections to the thermal cross section measured by Krane and to the evaluated value of JENDL-4.0 at the 47.05-eV resonance, respectively. Twelve new resonances for $$^{112}$$Sn were observed, whereas the 21.02-, 40.38- and 166-eV resonances for $$^{112}$$Sn and the 289-eV resonance for $$^{118}$$Sn which are listed on JENDL-4.0 and/or ENDF/B VII.1 were not observed. The prompt $$gamma$$-ray distributions gated at the $$^{112}$$Sn and $$^{118}$$Sn resonances were obtained. Twenty-three new prompt $$gamma$$-ray emissions were observed in the $$^{112}$$Sn (n,$$gamma$$) reactions.

論文

Energy resolution of pulsed neutron beam provided by the ANNRI beamline at the J-PARC/MLF

木野 幸一*; 古坂 道弘*; 平賀 富士夫*; 加美山 隆*; 鬼柳 善明*; 古高 和禎; 後神 進史*; 原 かおる; 原田 秀郎; 原田 正英; et al.

Nuclear Instruments and Methods in Physics Research A, 736, p.66 - 74, 2014/02

https://doi.org/10.1016/j.nima.2013.09.060
 被引用回数：32 パーセンタイル：90.73(Instruments & Instrumentation)

We studied the energy resolution of the pulsed neutron-beam of Accurate Neutron-Nucleus Reaction Measurement Instrument (ANNRI) at the Japan Proton Accelerator Research Complex/Materials and Life Science Experimental Facility (J-PARC/MLF). A simulation in the energy region from 0.7 meV to 1 MeV has been performed. Moreover, measurements have been done in the thermal and epithermal energies. The neutron energy resolution at ANNRI, which is determined by the time-of-flight technique, depends on the time structure of the neutron pulse. We obtained the neutron energy resolution as a function of the neutron energy by the simulation in the two operation modes of the neutron source: double and single bunch modes. In the double bunch mode, the resolution deteriorates above about 10 eV because the time structure of the neutron pulse splits into two peaks. The time structures at 13 energy points by measurements in the thermal energy region are in agreement with those of the simulation. In the epithermal energy region, the time structures at 17 energy points were obtained by measurements. The FWHM values of the time structures by the simulation and measurements are almost consistent. In the single bunch mode, the energy resolution is better than about 1% between 1 meV and 10 keV at the neutron source operation of 17.5 kW.

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