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論文

Investigation of the phonon dispersion associated with superlattice reflections in the BiS$$_{2}$$-based superconductor LaBiS$$_{2}$$O$$_{0.5}$$F$$_{0.5}$$

玉造 博夢; 長谷川 巧*; 佐賀山 基*; 水牧 仁一朗*; 村上 洋一*; 梶谷 丈*; 東中 隆二*; 松田 達磨*; 青木 勇二*; 筒井 智嗣*

Physical Review B, 107(2), p.024303_1 - 024303_8, 2023/01

https://doi.org/10.1103/PhysRevB.107.024303
 被引用回数：0 パーセンタイル：0(Materials Science, Multidisciplinary)

The phonon dispersion of a BiS$$_{2}$$-based superconductor LaBiS$$_{2}$$O$$_{0.5}$$F$$_{0.5}$$ is investigated by first-principles calculations and inelastic X-ray scattering experiments. The origin of superlattice (SL) reflections arising from transverse-type lattice modulation, which were recently reported in [J. Kajitani $textit{et al}$., J. Phys. Soc. Jpn. ${bf 90}$, 103601 (2021)], is discussed in terms of lattice dynamics. Our first-principles calculations of phonon dispersion and the Fermi surfaces (FSs) demonstrate that the phonon mode corresponding to the transverse-type lattice modulation is unstable, and the propagation vector corresponding to the SL reflections is close to the FS nesting vector, which suggests that the phonon softening originates from the FS nesting. Against these calculated expectations, measured phonon dispersion in LaBiS$$_{2}$$O$$_{0.5}$$F$$_{0.5}$$ along the Z-A direction, where the SL point is located, shows no remarkable temperature dependence, and there are no steeply declining branches accompanied with a softening around the SL point. Based on these results, we discuss the two possibilities for the transverse lattice modulation in LaBiS$$_{2}$$O$$_{0.5}$$F$$_{0.5}$$: the order-disorder type structural transition and the displacive structural transition with an overdamped mode, for both of which the local structure distortion or the short range correlation within the BiS$$_{2}$$ plane would be essential.

論文

Empirical correction factor to estimate the plastic collapse bending moment of pipes with circumferential surface flaw

Lacroix, V.*; 長谷川 邦夫; Li, Y.; 山口 義仁

Proceedings of ASME 2022 Pressure Vessels and Piping Conference (PVP 2022) (Internet), 7 Pages, 2022/07

The structural integrity assessment of pipes with circumferential surface flaw under the plastic collapse regime consists of net section collapse analysis. In recent years various researchers showed that this analysis, which has been developed based on classic beam theory, suffers from certain inaccuracies. As such, assessment purely based on net-section collapse and beam theory can reveal both conservative and unconservative results. To address those inaccuracies, in this paper authors introduced a correction factor which aims to mitigate the difference between the ASME B&PV Code Section XI equations and the experimental results. This correction factor is calculated using an empirical formula developed on the basis of a large experimental database of pipe collapse bending tests containing variety of diameter, thickness, flaw depth and flaw length values. Within this work, authors took a systematic approach to identify the most influencing factors on such a correction factor and showed that by applying this correction factor to the current solution of ASME B&PV Code Section XI, this solution becomes more accurate. This corrected approach also is in line with ASME B&PV Code Section XI Appendix C practice for axial flaw in pipes, where a semi-empirical correction factor has been considered as well.

論文

Failure bending stresses for small diameter thick-wall pipes

山口 義仁; 長谷川 邦夫; Li, Y.; Lacroix, V.*

Proceedings of ASME 2022 Pressure Vessels and Piping Conference (PVP 2022) (Internet), 4 Pages, 2022/07

Four-point bending tests without internal pressure were performed for Type 304 stainless steel pipes with circumferential flaws at room temperature. The specimens are 1-inch diameter (33.7 mm) Schedule 160 pipes (6.3 mm wall thickness). The flaws were part-through flaws located at the pipe external side. The flaw angles are from 120$$^{circ}$$ to 240$$^{circ}$$, and the flaw depths are two cases of 50% and 75% of the wall thickness. Plastic collapse stresses obtained from experiments were compared with those calculated using Limit Load Criteria from Appendix C of the American Society of Mechanical Engineers Code Section XI. Limit Load Criteria were developed using flow stress at flawed section of the pipe. The plastic collapse stress test results were larger than those of the calculation results. For flaws with flaw depths less than 50% of the wall thickness, the experimental stresses were significantly large. The Limit Load Criteria given by Section XI provide conservative collapse stresses and could be improved.

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：17 パーセンタイル：80.41(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

Fatigue crack growth for ferritic steel under negative stress ratio

山口 義仁; 長谷川 邦夫; Li, Y.

Journal of Pressure Vessel Technology, 142(4), p.041507_1 - 041507_6, 2020/08

https://doi.org/10.1115/1.4046768
 被引用回数：0 パーセンタイル：0(Engineering, Mechanical)

疲労亀裂進展中における亀裂の開閉口は、亀裂進展速度の評価において重要な現象である。ASME Code Section XIのAppendix A-4300は、負の応力比におけるフェライト鋼の疲労亀裂進展速度を算出する式について、負荷の大きさに応じて二つ提示している。一つは、負荷が小さい場合に、亀裂の閉口を考慮する式である。もう一つは、負荷が大きい場合に、亀裂の閉口を考慮しない式である。本研究では、フェライト鋼に対して、負荷の大きさを徐々に変えながら疲労亀裂進展試験を実施し、負荷の大きさが亀裂閉口に及ぼす影響を調査した。その結果、Appendix A-4300における疲労亀裂進展速度算出式を切り替える負荷の大きさと比較して、より小さい負荷で亀裂が閉口することを明らかにした。

論文

Bromine-isotope selective ionization using field-free alignment of IBr isotopologues with a switched nanosecond laser pulse

赤木 浩*; 熊田 高之; 乙部 智仁*; 板倉 隆二*; 長谷川 宗良*; 大島 康裕*

Chemistry Letters, 49(4), p.416 - 418, 2020/04

https://doi.org/10.1246/cl.200024
 被引用回数：1 パーセンタイル：4.87(Chemistry, Multidisciplinary)

We demonstrate isotope selective ionization of I$$^{79}$$Br and I$$^{81}$$Br isotopologues using field-free alignment induced by a linearly-polarized nanosecond laser pulse with rapid turn off at the maximum. Following the switched nanosecond pulse irradiation, a 60-fs laser pulse ionizes one of the isotopologues preferentially. The ion yield ratio $$I$$(I$$^{81}$$Br$$^+$$)/$$I$$(I$$^{79}$$Br$$^+$$) varies in the range of 0.93-1.06, depending on time delay between the pulses. This is the first demonstration of laser isotope separation of heavy elements using field-free alignment and angular dependent ionization.

論文

Gamma-ray spectroscopy of single $$Lambda$$-hypernuclei at J-PARC; Results and perspective

小池 武志*; 長谷川 勝一; 早川 修平*; 細見 健二; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; 杉村 仁志; 田村 裕和; et al.

AIP Conference Proceedings 2130, p.020011_1 - 020011_9, 2019/07

https://doi.org/10.1063/1.5118379
 被引用回数：2 パーセンタイル：73.22(Physics, Nuclear)

Experimental results from the J-PARC E13 experiments are summarized. A new experimental set up of E13 has established a platform for the future $$gamma$$-ray hypernuclear spectroscopy at J-PARC using kaon beams. New $$gamma$$ rays are identified in $$^4_{Lambda}$$He and $$^{19}_{Lambda}$$F. The energy of 1.406 MeV for the $$^4_{Lambda}$$He$$(1^+ to 0^+)$$ transition confirmed a sizable effect of Charge Symmetry Breaking (CSB) in $$Lambda N$$ interaction in the $$A=4$$ hypernuclear system. The identification of four $$gamma$$ rays in $$^{19}_{Lambda}$$F is made for the first time in $$sd$$ shell hypernuclei. Especially, energy spacing of the ground state doublet is found to be 315.5 keV. A good agreement with two theoretical calculations suggests that the theoretical formalism used in $$p$$ shell hypernuclei is also applicable to heavier hypernuclei. Lastly, an overview of the future J-PARC E63 experiment is given.

論文

First-principles study of solvent-solute mixed dumbbells in body-centered-cubic tungsten crystals

鈴土 知明; 都留 智仁; 長谷川 晃*

Journal of Nuclear Materials, 505, p.15 - 21, 2018/07

AA2017-0485.pdf:0.51MB

https://doi.org/10.1016/j.jnucmat.2018.03.052
 被引用回数：17 パーセンタイル：86.67(Materials Science, Multidisciplinary)

タングステン(W)は、将来の核融合炉のプラズマ対向材料として有望視されており、W合金の耐放射線性を向上させその機械的特性を改善するための最適な合金成分を選択することが重要な課題である。本研究では、W結晶中の溶媒と溶質の混合ダンベルを第一原理計算によって調査した。その結果、チタン, バナジウム, クロムはW材の延性を低下させる原因となる照射誘起析出を起こさずに、空孔と格子間原子の再結合を促進させるため、照射効果という観点からではW材の合金元素として望ましいことがわかった。

論文

Fatigue crack growth for ferritic steel under negative stress ratio

山口 義仁; 長谷川 邦夫; Li, Y.

Proceedings of 2018 ASME Pressure Vessels and Piping Conference (PVP 2018), 6 Pages, 2018/07

疲労亀裂進展中における亀裂の開閉口は、亀裂進展速度の評価において重要な現象である。ASME Code Section XIのAppendix A-4300は、負の応力比におけるフェライト鋼の疲労亀裂進展速度を算出する式について、負荷の大きさに応じて二つ提示している。一つは、負荷が小さい場合に、亀裂の閉口を考慮する式である。もう一つは、負荷が大きい場合に、亀裂の閉口を考慮しない式である。本研究では、フェライト鋼に対して、負荷の大きさを徐々に変えながら疲労亀裂進展試験を実施し、負荷の大きさが亀裂閉口に及ぼす影響を調査した。その結果、Appendix A-4300における疲労亀裂進展速度算出式を切り替える負荷の大きさと比較して、より小さい負荷で亀裂が閉口することを明らかにした。

論文

Retreat from stress; Rattling in a planar coordination

末國 晃一郎*; Lee, C. H.*; 田中 博己*; 西堀 英治*; 中村 篤*; 笠井 秀隆*; 森 仁志*; 臼井 秀知*; 越智 正之*; 長谷川 巧*; et al.

Advanced Materials, 30(13), p.1706230_1 - 1706230_6, 2018/03

https://doi.org/10.1002/adma.201706230
 被引用回数：51 パーセンタイル：89.35(Chemistry, Multidisciplinary)

高性能デバイスとしての熱電材料には、高い電気伝導度と低い熱伝導度という相反する要求を同時に満たす必要がある。本研究では、テトラへドライト(Cu,Zn)$$_{12}$$(Sb,As)$$_{4}$$S$$_{13}$$の結晶構造とフォノンダイナミクスを調べ、平面内に配位している銅原子のラットリング運動がフォノンを効率良く散乱することを見出した。これらの知見は、平面配位構造を有する高性能熱電材料の新たな開発指針を与えるものである。

論文

First determination of the level structure of an $$sd$$-shell hypernucleus, $$^{19}_{Lambda}$$F

Yang, S. B.*; 江川 弘行; 長谷川 勝一; 早川 修平; 細見 健二; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; 谷田 聖; et al.

Physical Review Letters, 120(13), p.132505_1 - 132505_5, 2018/03

AA2018-0124.pdf:0.62MB

https://doi.org/10.1103/PhysRevLett.120.132505
 被引用回数：8 パーセンタイル：54.37(Physics, Multidisciplinary)

We report on the first observation of $$gamma$$ rays emitted from an $$sd$$-shell hypernucleus, $$^{19}_{Lambda}$$F. The energy spacing between the ground state doublet, $$1/2^+$$ and $$3/2^+$$ states, of $$^{19}_{Lambda}$$F is determined to be $$315.5pm0.4({rm stat.})^{+0.6}_{-0.5}({rm syst.})$$ keV by measuring the $$gamma$$-ray energy of the $$M1(3/2^+ to 1/2^+)$$ transition. In addition, three $$gamma$$-ray peaks are observed and assigned as $$E2(5/2^+ to 1/2^+)$$, $$E1(1/2^- to 1/2^+)$$, and $$E1(1/2^- to 3/2^+)$$ transitions. The excitation energies of the $$5/2^+$$ and $$1/2^-$$ states are determined to be $$895.2pm0.3({rm stat.})pm0.5({rm syst.})$$ keV and $$1265.6pm1.2({rm stat.})^{+0.5}_{-0.7}({rm syst.})$$ keV, respectively. It is found that the ground state doublet spacing is well described by theoretical models based on existing $$s$$- and $$p$$-shell hypernuclear data.

論文

Isotope-selective ionization utilizing field-free alignment of isotopologues using a switched nanosecond laser pulse

赤木 浩*; 熊田 高之; 乙部 智仁*; 板倉 隆二*; 長谷川 宗良*; 大島 康裕*

Applied Physics B, 124(1), p.14_1 - 14_8, 2018/01

https://doi.org/10.1007/s00340-017-6884-7
 被引用回数：2 パーセンタイル：14.76(Optics)

新たな同位体分離法を目指したフィールドフリーアライメントによるイオン化効率の同位体選択性を計算した。従来のフェムト秒レーザーを用いたフィールドフリーアライメント法では、レーザー強度を強くするとイオン化の選択性が無くなってしまうのに対し、200fsでカットオフするナノ秒レーザーパルスを用いると選択性を保持したまま高い同位体選択イオン化が実現することが判明した。

論文

Application of modified REFIT code for J-PARC/MLF to evaluation of neutron capture cross section on $$^{155,157}$$Gd

水山 一仁; 岩本 信之; 岩本 修; 長谷美 宏幸*; 木野 幸一*; 木村 敦; 鬼柳 善明*

EPJ Web of Conferences, 146, p.11042_1 - 11042_4, 2017/09

https://doi.org/10.1051/epjconf/201714611042
 被引用回数：2 パーセンタイル：78.04(Nuclear Science & Technology)

ガドリニウムは$$^{155,157}$$Gdが非常に大きな中性子捕獲断面積をもつため原子炉の中性子吸収材料として用いられる。しかしながら、$$^{157}$$GdのRPIデータとJENDL-4.0ではばらつきがあることが知られている。原子炉の臨界性は捕獲断面積に敏感であり、RPIのデータはICSBEPにあるガドミニウム溶液体系の臨界性を大きくしてしまうことがわかっている。近年、$$^{155,157}$$Gdの中性子捕獲断面積がJ-PARC/MLFでANNRIを用いた実験で飛行時間法によって測定された。J-PARCの中性子パルスはダブルバンチ構造を持っており、また、高精度な共鳴解析には中性子パルスの時間分解能関数も適切に考慮して行う必要がある。そこで、本研究では、中性子パルスのダブルバンチ構造やANNRI用の時間分解能関数を組み込んだ改良REFITを用いて中性子捕獲断面積の実験データをフィットし、共鳴パラメータを導出する。

論文

$$gamma$$-ray spectroscopy of hypernuclei; Recent results and prospect at J-PARC

田村 裕和*; 江川 弘行; 長谷川 勝一; 早川 修平; 細見 健二; Hwang, S.; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; et al.

JPS Conference Proceedings (Internet), 17, p.011004_1 - 011004_11, 2017/07

https://doi.org/10.7566/JPSCP.17.011004

The present status and future prospects of precision $$gamma$$-ray spectroscopy of $$Lambda$$ hypernuclei are described. A new experiment (J-PARC E13) has been performed at the J-PARC K1.8 line employing a newly-developed germanium (Ge) detector array, Hyperball-J, via the $$(K^-,pi^-)$$ reaction on $$^4$$He and $$^{19}$$F targets. This is the first study of $$s$$-shell and $$sd$$-shell $$Lambda$$ hypernuclei with Ge detectors. The $$^4$$He target spectrum exhibited a $$gamma$$-ray peak of $$^4_{Lambda}{rm He}(1^+to 0^+)$$ at $$1.406 pm 0.002 pm 0.002$$ MeV. Compared with the energy ($$1.09 pm 0.02$$ MeV) of the corresponding transition for the mirror hypernucleus, $$^4_{Lambda}{rm H}(1^+to 0^+)$$, the present result clearly indicates a large charge symmetry breaking (CSB) effect. This decisive data for CSB allows a stringent test of baryon-baryon interaction models. As for the $$^{19}$$F target run, a preliminary spectrum shows several $$gamma$$-ray peaks assigned to $$^{19}_{Lambda}{rm F}$$ transitions. Future plans of $$gamma$$-ray spectroscopy are also discussed.

論文

Search for excited state of $$Sigma$$ hypernucleus in the J-PARC E13 experiment

中川 真菜美*; 江川 弘行; 長谷川 勝一; 早川 修平; 細見 健二; Hwang, S.; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; et al.

JPS Conference Proceedings (Internet), 17, p.012009_1 - 012009_4, 2017/07

https://doi.org/10.7566/JPSCP.17.012009

One of the main items of the J-PARC E13 experiment is the search for excited states of the $$^4_{Sigma}$$He hypernucleus via the $$^4$$He$$(K^-,pi^-)$$ reaction at 1.5 GeV/c. The missing-mass spectrum of the $$^4$$He$$(K^-,pi^-)X$$ reaction was obtained in an angular range from 0 to 20 degrees. We show the count-base spectrum of the missing-mass in the angular range from 2 to 14 degrees. The ground state of $$^4_{Lambda}$$He and $$^4_{Sigma}$$He were clearly observed in the missing-mass spectrum. We also show three missing-mass spectra divided by the reaction angle.

論文

High statistics $$Sigma p$$ scattering experiment using high intensity pion beams at J-PARC

三輪 浩司*; 長谷川 勝一; 早川 修平; 細見 健二; 今井 憲一; 近藤 恭弘; 成木 恵; 佐甲 博之; 佐藤 進; 杉村 仁志; et al.

JPS Conference Proceedings (Internet), 17, p.041002_1 - 041002_6, 2017/07

https://doi.org/10.7566/JPSCP.17.041002

In order to test theoretical frameworks of the Baryon-Baryon ($$BB$$) interactions and to confirm the "Pauli effect between quarks" for the first time, we have proposed an experiment (J-PARC E40) to measure low-energy hyperon-proton scattering cross sections of the $$Sigma^+ p$$, $$Sigma^- p$$ elastic scatterings and the $$Sigma^- p to Lambda n$$ inelastic scattering in the momentum range of $$400 < p ; ({rm MeV}/c) < 700$$ in the laboratory system. Experimentally, we detect two successive reactions of the $$Sigma$$ production $$(pi^{pm}p to K^+Sigma^{pm})$$ and the $$Sigma p$$ scattering ($$Sigma p to Sigma p$$) in the same liquid hydrogen target. The former is measured with two magnetic spectrometers, and the latter with a scattered proton detector (CATCH). By using a high intensity $$pi$$ beam, we estimate that more than 10000 scattering events can be identified. In this experiment, we aim to provide good quality scattering data to test the theoretical models of the $$BB$$ interaction.

論文

The First gamma-ray spectroscopic study of $$sd$$-shell hypernucleus, $$^{19}_{Lambda}$$F

Yang, S. B.*; 江川 弘行; 長谷川 勝一; 早川 修平; 細見 健二; Hwang, S.; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; et al.

JPS Conference Proceedings (Internet), 17, p.012004_1 - 012004_4, 2017/07

https://doi.org/10.7566/JPSCP.17.012004

The first $$gamma$$-ray spectroscopy of $$sd$$-shell hypernucleus, $$^{19}_{Lambda}$$F, is performed in June, 2015 at the J-PARC K1.8 beam line (J-PARC E13). Precise energy levels of $$^{19}_{Lambda}$$F can be revealed by measured $$gamma$$ rays in this experiment. Especially, the strength of $$Lambda N$$ spin-spin interaction in $$sd$$-shell hypernucleus is obtained through the energy spacing of the ground-state doublet of the hypernucleus. By comparing its strength between the $$s$$, $$p$$, and $$sd$$-shell hypernuclei, a radial dependence $$Lambda N$$ interaction is investigated. The hypernucleus is produced through the $$(K^-,pi^-)$$ reaction with the beam momentum of 1.8 GeV/c. In very preliminary results, we observed two $$gamma$$ rays, and their energies are $$315.8 pm 0.4$$ keV and $$ 895.3 pm 0.3$$ keV where the uncertainties are only statistical.

論文

Missing-mass spectroscopy with the $$^6$$Li$$(pi^-,K^+)X$$ reaction to search for $$^6_Lambda$$H

本多 良太郎*; 長谷川 勝一; 早川 修平; 細見 健二; 市川 裕大; 今井 憲一; 永宮 正治; 佐甲 博之; 佐藤 進; 杉村 仁志; et al.

Physical Review C, 96(1), p.014005_1 - 014005_23, 2017/07

AA2017-0465.pdf:1.08MB

https://doi.org/10.1103/PhysRevC.96.014005
 被引用回数：14 パーセンタイル：73.79(Physics, Nuclear)

We searched for the bound state of the neutron-rich $$Lambda$$-hypernucleus $$^6_Lambda$$H, using the $$^6$$Li$$(pi^-,K^+)X$$ double charge-exchange reaction at a $$pi^-$$ beam momentum of 1.2 GeV/$$c$$ at J-PARC. A total of $$1.4 times 10^{12}$$ $$pi^-$$ was driven onto a $$^6$$Li target of 3.5 g/cm$$^2$$ thickness. No event was observed below the bound threshold, i.e., the mass of $$^4_Lambda$$H+$$2n$$, in the missing-mass spectrum of the $$^6$$Li$$(pi^-,K^+)X$$ reaction in the $$2^{circ} < theta_{pi K} <20^{circ}$$ angular range. Furthermore, no event was found up to 2.8 MeV/c$$^2$$ above the bound threshold.

論文

Reference curve of fatigue crack growth for ferritic steels under negative R ratio provided by ASME Code Section XI

長谷川 邦夫*; Mare$v{s}$, V.*; 山口 義仁

Journal of Pressure Vessel Technology, 139(3), p.034501_1 - 034501_5, 2017/06

https://doi.org/10.1115/1.4034586
 被引用回数：2 パーセンタイル：12.87(Engineering, Mechanical)

Reference curves of fatigue crack growth rates for ferritic steels in air environment are provided by the ASME Code Section XI Appendix A. The fatigue crack growth rates under negative R ratio are given as da/dN vs. K$$_{max}$$. It is generally well known that the growth rates decreases with decreasing R ratios. However, the da/dN as a function of K$$_{max}$$ are the same curves under R = 0, -1 and -2. In addition, the da/dN increases with decreasing R ratio for R$$<$$-2. This paper converts from da/dN vs. K$$_{max}$$ to da/dN vs. $$Delta$$K$$_{I}$$, using crack closure U. It can be seen that the growth rate da/dN vs. $$Delta$$K$$_{I}$$ is better equation than da/dN vs. K$$_{max}$$ from the view point of stress ratio R. Furthermore, extending crack closure U to R = -5, it can be explained that the da/dN decreases with decreasing R ratio in the range of -5 $$<$$ R $$<$$ 0. This tendency is consistent with the experimental data.

論文

Observation of $$Xi$$ bound states in the $$^{12}$$C$$(K^-,K^+)X$$ reaction at 1.8 GeV/$$c$$ in J-PARC

永江 知文*; 江川 弘行; 長谷川 勝一; 細見 健二; 市川 裕大; 今井 憲一; 佐甲 博之; 佐藤 進; 杉村 仁志; 谷田 聖; et al.

Proceedings of Science (Internet), 281, p.038_1 - 038_7, 2017/05

https://doi.org/10.22323/1.281.0038

We have carried out a pilot data taking of the J-PARC E05 experiment to search for the bound state peaks of $$^{12}_{Xi}$$Be in the $$^{12}$$C$$(K^-,K^+)X$$ reaction at 1.8 GeV/$$c$$. The measurement was performed at the K1.8 beam line of the J-PARC hadron experimental hall with a typical $$K^-$$ beam intensity of $$6 times 10^5$$ every six seconds. So far the best energy resolution of about 6 MeV FWHM was achieved with the existing SKS spectrometer. With a reasonable statistics, we have succeeded to observe peak structures in the bound region, which seems to suggest that the potential depth of $$Xi$$ would be deeper than 14 MeV estimated in the previous measurements.

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