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論文

On the role of austenite stability in yielding behavior of a medium Mn steel with a duplex austenite-martensite microstructure

Wang, Y.*; Gong, W.; Harjo, S.; 他7名*

Acta Materialia, 288, p.120840_1 - 120840_14, 2025/04

 被引用回数:3 パーセンタイル:84.88(Materials Science, Multidisciplinary)

Low yield strength and the presence of Luders bands constitute principal impediments to the extensive applications of conventional medium Mn steels with a duplex microstructure of ferrite and austenite. Flash heating and the concept of chemical heterogeneity have been combined to engineer a duplex austenite-martensite microstructure in medium Mn steels, which has proven effective in augmenting the yield strength and mitigating the occurrence of Luders bands. However, the underlying mechanisms remain ambiguous. In the present work, the effect of austenite stability on yielding behavior was systematically investigated in an austenite-martensite duplex medium Mn steel. Austenite stability was identified as the critical factor governing yield strength, where reduced stability promotes early stage deformation induced martensite transformation, thereby decreasing yield strength. Diminished austenite stability may as well induce enhanced work hardening, thereby result in the inclination and eventual elimination of yield plateau, concomitant with the disappearance of Luders bands. These observations expand our current understanding of the yielding behavior in medium Mn steels and offer insights for the design of other advanced high strength steels.

論文

Heterogeneous Earth's mantle drilled at an embryonic ocean

Sanfilippo, A.*; 安邊 啓明; 他27名*

Nature Communications (Internet), 16, p.2016_1 - 2016_11, 2025/02

 被引用回数:0 パーセンタイル:0.00(Multidisciplinary Sciences)

Mantle processes control plate tectonics and exert an influence on biogeochemical cycles. However, the proportion of the mantle accessible to sampling is minimal, and a significant portion of our knowledge is derived from xenoliths, orogenic peridotite massifs exposed on land, and abyssal peridotites. Sampling of in-situ sections of the mantle is extremely challenging because they are buried beneath a magmatic crust with its sedimentary cover. In this study, we report the lithological characteristics of two mantle sections from an embryonic, very young, (~3 Ma) oceanic basin drilled by the International Ocean Discovery Program (IODP) in the central Tyrrhenian Sea. In contrast to observations made in drilled mantle sections from Mid Ocean Ridges (MORs) and hyperextended passive margins such as those in Iberia and Newfoundland, our findings revealed an exceptionally heterogeneous and generally fertile mantle. This represents a snapshot of young oceanic basement in a continental rifting environment characterised by general igneous starvation. The lithological heterogeneity ranges from fertile lherzolites to depleted harzburgites and dunites, variably interlayered with pyroxenites. Plagioclase- and clinopyroxene-rich layers, hydrous potassic magmatic veins, and gabbroic intrusions in these peridotites indicate substantial mantle re-fertilization and delayed inception of magmatic crust. The diverse lithological recovery indicates that magma-poor rifts do not necessarily require a chemically depleted mantle, too refractory to melt. Instead, we propose that deep lithospheric processes such as mantle refertilisation and prolonged lithospheric thinning hinder melt focusing and the formation of a steady-state spreading centre.

論文

Single-layer spin-orbit-torque magnetization switching due to spin berry curvature generated by minute spontaneous atomic displacement in a Weyl oxide

堀内 皓斗*; 荒木 康史; 若林 勇希*; 家田 淳一; 山ノ内 路彦*; 他7名*

Advanced Materials, p.2416091_1 - 2416091_9, 2025/00

 被引用回数:0 パーセンタイル:0.00(Chemistry, Multidisciplinary)

Spin Berry curvature characterizes the band topology as the spin counterpart of Berry curvature and is crucial in generating novel spintronics functionalities. By breaking the crystalline inversion symmetry, the spin Berry curvature is expected to be significantly enhanced; this enhancement will increase the intrinsic spin Hall effect in ferromagnetic materials and, thus, the spin-orbit torques (SOTs). However, this intriguing approach is not applied to devices; generally, the spin Hall effect in ferromagnet/heavy-metal bilayer is used for SOT magnetization switching. Here, SOT-induced partial magnetization switching is demonstrated in a single layer of a single-crystalline Weyl oxide SrRuO$$_{3}$$ (SRO) with a small current density of $$approx 3.1 times 10^6 {rm A} {rm cm}^{-2}$$. Detailed analysis of the crystal structure in the seemingly perfect periodic lattice of the SRO film reveals barely discernible oxygen octahedral rotations with angles of $$approx 5^circ$$ near the interface with a substrate. Tight-binding calculations indicate that a large spin Hall conductivity is induced around small gaps generated at band crossings by the synergy of inherent spin-orbit coupling and band inversion due to the rotations, causing magnetization reversal. The results indicate that a minute atomic displacement in single-crystal films can induce strong intrinsic SOTs that are useful for spin-orbitronics devices.

論文

First measurement of missing energy due to nuclear effects in monoenergetic neutrino charged-current interactions

Marzec, E.*; 百々 拓; 羽賀 勝洋; 原田 正英; 長谷川 勝一; 春日井 好己; 木下 秀孝; 増田 志歩; 明午 伸一郎; 酒井 健二; et al.

Physical Review Letters, 134, p.081801_1 - 081801_9, 2025/00

 被引用回数:1 パーセンタイル:0.00(Physics, Multidisciplinary)

We present the first measurement of the missing energy due to nuclear effects in monoenergetic, muon neutrino charged-current interactions on carbon, originating from $$K^+ to mu^+ nu_{mu}$$ decay at rest ($$E_{nu_{mu}} = 235.5 MeV$$), performed with the J-PARC Sterile Neutrino Search at the J-PARC Spallation Neutron Source liquid scintillator based experiment. Toward characterizing the neutrino interaction, ostensibly $$nu_{mu}n to mu^- p$$ or $$nu_{mu}$$ $$^{12}$$C $$to$$ $$mu^-$$ $$^{12}$$N, we define the missing energy as the energy transferred to the nucleus ($$omega$$) minus the kinetic energy of the outgoing proton(s), $$E_m equiv omega - Sigma T_p$$, and relate this to visible energy in the detector, $$E_m = E_{nu_{mu}} (235.5 MeV) - m_{mu}(105.7 MeV) + [m_n - m_p(1.3 MeV)] - E_{vis}$$. The missing energy, which is naively expected to be zero in the absence of nuclear effects (e.g., nucleon separation energy, Fermi momenta, and final-state interactions), is uniquely sensitive to many aspects of the interaction, and has previously been inaccessible with neutrinos. The shape-only, differential cross section measurement reported, based on a $$(77pm 3%)$$ pure double-coincidence kaon decay-at-rest signal (621 total events), provides detailed insight into neutrino-nucleus interactions, allowing even the nuclear orbital shell of the struck nucleon to be inferred. The measurement provides an important benchmark for models and event generators at hundreds of MeV neutrino energies, characterized by the difficult-to-model transition region between neutrino-nucleus and neutrino-nucleon scattering, and relevant for applications in nuclear physics, neutrino oscillation measurements, and Type-II supernova studies.

論文

Enhanced magnetism derived from pore-edge spins in thin Fe$$_3$$GeTe$$_2$$ nanomeshes

小幡 玲二*; 吉川 貴史*; 齊藤 英治; 他7名*

Nanotechnology, 35(47), p.475601_1 - 475601_9, 2024/11

 被引用回数:1 パーセンタイル:35.22(Nanoscience & Nanotechnology)

The growth of two-dimensional van der Waals magnetic materials presents attractive opportunities for exploring new physical phenomena and valuable applications. Among these materials, Fe$$_{3}$$GeTe$$_{2}$$ (FGT) exhibits a variety of remarkable properties and has garnered significant attention. Herein, we have for the first time created a nanomesh structure-a honeycomb-like array of hexagonal nanopores-with the zigzag pore-edge atomic structure on thin FGT flakes with and without oxidation of the pore edges. It is revealed that the magnitude of ferromagnetism (FM) significantly increases in both samples compared with bulk flakes without nanomeshes. Critical temperature annealing results in the formation of zigzag pore edges and interpore zigzag-edge nanoribbons. We unveil that the non-oxide (O) termination of the Fe dangling bonds on these zigzag edges enhances FM behavior, while O-termination suppresses this FM by introducing antiferromagnetic behavior through edge O-Fe coupling. FGT nanomeshes hold promise for the creation of strong FM and their effective application in magnetic and spintronic systems.

論文

Isotope-dependent site occupation of hydrogen in epitaxial titanium hydride nanofilms

小澤 孝拓*; 福谷 克之; 他7名*

Nature Communications (Internet), 15, p.9558_1 - 9558_8, 2024/11

 被引用回数:0 パーセンタイル:0.00(Multidisciplinary Sciences)

Hydrogen, the smallest and lightest element, readily permeates a variety of materials and modulates their physical properties. Identification of the hydrogen lattice location and its amount in crystals is key to understanding and controlling the hydrogen-induced properties. Combining nuclear reaction analysis (NRA) with the ion channeling technique, we experimentally determined the locations of H and D in epitaxial nanofilms of titanium hydrides from the analysis of the two-dimensional angular mappings of NRA yields. Here we show that 11 at% of H are located at the octahedral site with the remaining H atoms in the tetrahedral site. Density functional theory calculations revealed that the structures with the partial octahedral site occupation are stabilized by the Fermi level shift and Jahn-Teller effect induced by hydrogen. In contrast, D was found to solely occupy the tetrahedral site owing to the mass effect on the zero-point vibrational energy. These findings suggest that site occupation of hydrogen can be controlled by changing the isotope mixture ratio, which leads to promising manifestation of novel hydrogen-related phenomena.

論文

Enhancement of modelling approaches for the assessment of radionuclide transfer in the marine environment

Peri$'a$$~n$ez, R.*; Bezhenar, R.*; Maderych, V.*; Brovchenko, I.*; Liptak, L.*; 小林 卓也; Min, B.-I.*; Suh, K. S.*; Little, A.*; Iosjpe, M.*; et al.

IAEA-TECDOC-2060, 55 Pages, 2024/07

IAEAは、2016年から2019年にかけて、放射線影響評価のためのモデリングとデータに関する(MODARIA II)プログラムを組織した。MODARIA IIの第7作業部会「海洋環境に放出された放射性核種の移行挙動の評価」では、拡散モデルを使用した海洋環境における放射性核種のシミュレーションに関する一般情報をまとめた。そして、東京電力福島第一原子力発電所事故シナリオを用いてCs-137の広域シミュレーションと生物への移行について検討するとともに、大西洋シナリオとして、ヨーロッパの核燃料使用済施設からの歴史的な放出について検討した。最後に、ラグランジェモデルにおける補間スキームの試験を実施した。本書は第7作業部会の活動内容について述べたものである。

論文

Attempt to synthesize the proton-unbound $$^{182,183}$$Bi isotopes

Huang, H.*; Andreyev, A. N.; 他37名*

Physical Review C, 110(1), p.014326_1 - 014326_8, 2024/07

 被引用回数:2 パーセンタイル:74.11(Physics, Nuclear)

The near-symmetric complete fusion reaction $$^{78}$$Kr+$$^{107}$$Ag=$$^{185}$$Bi$$^{*}$$ was studied at the gas-filled recoil separator SHANS with an attempt to synthesize the extremely neutron-deficient proton-unbound $$^{182,183}$$Bi isotopes. No decay events which could be attributed to them were observed. The two- and three-particle evaporation residues $$^{180,179}$$Hg ($$alpha p$$, $$alpha pn$$) and $$^{183,182}$$Pb($$pn$$,$$p2n$$) were identified. Based on the yields of 182,183Pb in the present work and the systematics of the ratios between the cross sections of $$p(x-1)n$$ and $$xn$$ evaporation channels for the most neutron-deficient odd-Z nuclei above lead, the upper limits for the half-lives of $$^{182,183}$$Bi were estimated to be less than 0.3$$mu$$s.

論文

Isochronous mass spectrometry at the RIKEN Rare-RI Ring facility

長江 大輔*; 阿部 康志*; 山口 由高*; 洲嵜 ふみ; 他27名*

Physical Review C, 110(1), p.014310_1 - 014310_13, 2024/07

 被引用回数:3 パーセンタイル:84.33(Physics, Nuclear)

A dedicated isochronous storage ring, named the Rare-RI Ring, was constructed at the RI Beam Factory of RIKEN, aiming at precision mass measurements of nuclei located in uncharted territories of the nuclear chart. The Rare-RI Ring employs the isochronous mass spectrometry technique with the goal to achieve a relative mass precision of 10$$^{-6}$$ within a measurement time of less than 1 ms. The performance of the facility was demonstrated through mass measurements of neutron-rich nuclei with well-known masses. Velocity or magnetic rigidity is measured for every particle prior to its injection into the ring, wherein its revolution time is accurately determined. The latter quantity is used to determine the mass of the particle, while the former one is needed for nonisochronicity corrections. Mass precisions on the order of 10$$^{-5}$$ were achieved in the first commissioning, which demonstrates that the Rare-RI Ring is a powerful tool for mass spectrometry of short-lived nuclei.

論文

Gamma-ray spectroscopy of $$^{55}$$Sc

Zidarova, R.*; 宇都野 穣; 他76名*

Physica Scripta, 99(7), p.075309_1 - 075309_9, 2024/06

 被引用回数:0 パーセンタイル:0.00(Physics, Multidisciplinary)

理化学研究所のRIビームファクトリーにて$$^{56}$$Sc($$p$$,$$pn$$)$$^{55}$$Sc反応によって$$^{55}$$Scの励起状態を生成し、そこからの脱励起ガンマ線の放出を測定することによってその原子核のエネルギー準位を構築した。1510(30)keVの励起準位など、いくつかの新しい準位を見つけた。その結果を大規模殻模型計算の結果と比較し、ガンマ崩壊様式を考慮した結果、1510(30)keVの準位は$$7/2^-$$の可能性が高いことがわかった。

論文

$$beta$$ decay of the ground state and of a low-lying isomer in $$^{216}$$Bi

Andel, B.*; Andreyev, A. N.; 他57名*

Physical Review C, 109(6), p.064321_1 - 064321_18, 2024/06

 被引用回数:2 パーセンタイル:74.11(Physics, Nuclear)

A detailed $$beta$$-decay study of the low- and high-spin states in $$^{216}$$Bi has been performed at the ISOLDE Decay Station at the CERN-ISOLDE facility. In total, 48 new levels and 83 new transitions in the $$beta$$-decay daughter $$^{216}$$Po were identified. Shell-model calculations for excited states in $$^{216}$$Bi and $$^{216}$$Po were performed using the H208 and the modified Kuo-Herling particle effective interactions. Based on the experimental observations and the shell-model calculations, the most likely spin and parity assignments for the $$beta$$-decaying states in $$^{216}$$Bi are (3$$^-$$) and (8$$^-$$), respectively.

論文

Coexistence of quantum-spin-hall and quantum-hall-topological-insulating states in graphene/hBN on SrTiO$$_3$$ substrate

小幡 玲二*; 齊藤 英治; 吉川 貴史; 他7名*

Advanced Materials, 36(19), p.2311339_1 - 2311339_8, 2024/05

 被引用回数:1 パーセンタイル:0.00(Chemistry, Multidisciplinary)

SrTiO$$_{3}$$ (STO) substrate, a perovskite oxide material known for its high dielectric constant (epsilon), facilitates the observation of various (high-temperature) quantum phenomena. A quantum Hall topological insulating (QHTI) state, comprising two copies of QH states with antiparallel two ferromagnetic edge-spin overlap protected by the U(1) axial rotation symmetry of spin polarization, has recently been achieved in low magnetic field (B) even as high as approximate to 100 K in a monolayer graphene/thin hexagonal boron nitride (hBN) spacer placed on an STO substrate, thanks to the high epsilon of STO. Despite the use of the heavy STO substrate, however, proximity-induced quantum spin Hall (QSH) states in 2D TI phases, featuring a topologically protected helical edge spin phase within time-reversal-symmetry, is not confirmed. Here, with the use of a monolayer hBN spacer, it is revealed the coexistence of QSH (at B = 0T) and QHTI (at B not equal 0) states in the same single graphene sample placed on an STO, with a crossover regime between the two at low B. It is also classified that the different symmetries of the two nontrivial helical edge spin phases in the two states lead to different interaction with electron-puddle quantum dots, caused by a local surface pocket of the STO, in the crossover regime, resulting in a spin dephasing only for the QHTI state. The results obtained using STO substrates open the doors to investigations of novel QH spin states with different symmetries and their correlations with quantum phenomena. This exploration holds value for potential applications in spintronic devices.

論文

Spectroscopy of neutron-rich Fe isotopes populated in the $$^{70}$$Zn+$$^{238}$$U reaction

Benito, J.*; Lenzi, S. M.*; Recchia, F.*; Axiotis, M.*; Aydin, S.*; Bazzacco, D.*; Benzoni, G.*; Orlandi, R.; 他37名*

Acta Physica Polonica B; Proceedings Supplement, 17(3), p.3-A4_1 - 3-A4_7, 2024/04

 被引用回数:0 パーセンタイル:0.00(Physics, Multidisciplinary)

Excited states of neutron-rich $$^{64,66,68}$$Fe isotopes have been studied through a multinucleon transfer reaction of a $$^{70}$$Zn beam on a $$^{238}$$U target at the National Laboratories of Legnaro, Italy. The magnetic spectrometer PRISMA was used to identified the isotopes produced in the reaction, and the CLARA array of Clover Ge detectors to detect their gamma rays. The obtained level scheme were compared with new, state-of-the-art large scale shell model calculations. The large model space used in the calculation, which included the 2d$$_{5/2}$$ orbital, revealed that this orbit is key in order to obtain excellent agreement between the calculations and the experimental data.

論文

FENDL: A Library for fusion research and applications

Schnabel, G.*; 国枝 賢; 今野 力; 中山 梓介; 他27名*

Nuclear Data Sheets, 193, p.1 - 78, 2024/02

 被引用回数:15 パーセンタイル:99.11(Physics, Nuclear)

国際原子力機関(IAEA)が中心となり、各国の研究者の協力のもと、核融合研究開発のための国際核データライブラリFENDLの更新を行った。最新ライブラリ(FENDL-3.2b)の構築にあたっては、主に米国のENDF、欧州のJEFF、日本のJENDLの相互比較を行い、積分検証結果も踏まえつつ、現状で最も妥当と考えられるデータを個々の核種毎に採用した。従来のライブラリとの大きな違いは、加速器中性子源やそれを用いる材料研究分野からのニーズに応えるためにこれまでのエネルギー上限を20MeVから最大200MeVに拡張し、中性子データのみならず陽子や重陽子データの収録も新規に行なったことである。また、本ライブラリの品質を検証することを目的として、中性子輸送計算や核発熱シミュレーション等を通じた種々のベンチーマーク解析を実施した。それにより、従来のライブラリに比べ実用性が大きく向上していることを示した。

論文

$$^{133}$$In; A Rosetta stone for decays of $$r$$-process nuclei

Xu, Z. Y.*; Andreyev, A. N.; 他47名*

Physical Review Letters, 131(2), p.022501_1 - 022501_6, 2023/07

 被引用回数:4 パーセンタイル:59.55(Physics, Multidisciplinary)

The $$beta$$ decays from both the ground state and a long-lived isomer of $$^{133}$$In were studied at the ISOLDE Decay Station (IDS). With a hybrid detection system sensitive to $$beta$$, $$gamma$$, and neutron spectroscopy, the comparative partial half-lives (log $$ft$$) have been measured for all their dominant $$beta$$-decay channels for the first time, including a low-energy Gamow-Teller transition and several first-forbidden (FF) transitions. Uniquely for such a heavy neutron-rich nucleus, their $$beta$$ decays selectively populate only a few isolated neutron unbound states in $$^{133}$$Sn. Precise energy and branching-ratio measurements of those resonances allow us to benchmark $$beta$$-decay theories at an unprecedented level in this region of the nuclear chart. The results show good agreement with the newly developed large-scale shell model (LSSM) calculations. The experimental findings establish an archetype for the $$beta$$ decay of neutron-rich nuclei southeast of $$^{132}$$Sn and will serve as a guide for future theoretical development aiming to describe accurately the key $$beta$$ decays in the rapid-neutron capture ($$r$$-) process.

論文

First application of Markov chain Monte Carlo-based Bayesian data analysis to the Doppler-shift attenuation method

Sun, L. J.*; Fry, C.*; Davids, B.*; Esker, N.*; Wrede, C.*; Smallcombe, J.; 他27名*

Physics Letters B, 839, p.137801_1 - 137801_8, 2023/04

 被引用回数:2 パーセンタイル:43.87(Astronomy & Astrophysics)

Motivated primarily by the large uncertainties in the thermonuclear rate of the 30PS reaction that limit our understanding of classical novae, we carried out lifetime measurements of $$^{31}$$S excited states using the Doppler Shift Lifetimes (DSL2) facility at the TRIUMF Isotope Separator and Accelerator (ISAC-II) facility.

論文

Measurement of the branching fractions for Cabibbo-suppressed decays $$D^{+}to K^{+} K^{-}pi^{+}pi^{0}$$ and $$D_{(s)}^{+}to K^{+}pi^{-}pi^{+}pi^{0}$$ at Belle

Li, L. K.*; 谷田 聖; Belle Collaboration*; 他197名*

Physical Review D, 107(3), p.033003_1 - 033003_9, 2023/02

 被引用回数:0 パーセンタイル:0.00(Astronomy & Astrophysics)

We present measurements of the branching fractions for the singly Cabibbo-suppressed decays $$D^+to K^{+}K^{-}pi^{+}pi^{0}$$ and $$D_s^{+}to K^{+}pi^{-}pi^{+}pi^{0}$$, and the doubly Cabibbo-suppressed decay $$D^{+}to K^{+}pi^{-}pi^{+}pi^{0}$$, based on 980 $${rm fb}^{-1}$$ of data recorded by the Belle experiment at the KEKB $$e^{+}e^{-}$$ collider. We measure these modes relative to the Cabibbo-favored modes $$D^{+}to K^{-}pi^{+}pi^{+}pi^{0}$$ and $$D_s^{+}to K^{+}K^{-}pi^{+}pi^{0}$$. Our results for the ratios of branching fractions are $$B(D^{+}to K^{+}K^{-}pi^{+}pi^{0})/B(D^{+}to K^{-}pi^{+}pi^{+}pi^{0}) = (11.32 pm 0.13 pm 0.26)%$$, $$B(D^{+}to K^{+}pi^{-}pi^{+}pi^{0})/B(D^{+}to K^{-}pi^{+}pi^{+}pi^{0}) = (1.68 pm 0.11pm 0.03)%$$, and $$B(D_s^{+}to K^{+}pi^{-}pi^{+}pi^{0})/B(D_s^{+}to K^{+}K^{-}pi^{+}pi^{0}) = (17.13 pm 0.62 pm 0.51)%$$, where the uncertainties are statistical and systematic, respectively. The second value corresponds to $$(5.83pm 0.42)timestan^4theta_C$$, where $$theta_C$$ is the Cabibbo angle; this value is larger than other measured ratios of branching fractions for a doubly Cabibbo-suppressed charm decay to a Cabibbo-favored decay. Multiplying these results by world average values for $$B(D^{+}to K^{-}pi^{+}pi^{+}pi^{0})$$ and $$B(D_s^{+}to K^{+}K^{-}pi^{+}pi^{0})$$ yields $$B(D^{+}to K^{+}K^{-}pi^{+}pi^{0})= (7.08pm 0.08pm 0.16pm 0.20)times10^{-3}$$, $$B(D^{+}to K^{+}pi^{-}pi^{+}pi^{0})= (1.05pm 0.07pm 0.02pm 0.03)times10^{-3}$$, and $$B(D_s^{+}to K^{+}pi^{-}pi^{+}pi^{0}) = (9.44pm 0.34pm 0.28pm 0.32)times10^{-3}$$, where the third uncertainty is due to the branching fraction of the normalization mode. The first two results are consistent with, but more precise than, the current world averages. The last result is the first measurement of this branching fraction.

論文

Measurement of the branching fraction of $$Xi_{c}^{0}to Lambda_{c}^{+}pi^{-}$$ at Belle

Tang, S. S.*; 谷田 聖; Belle Collaboration*; 他173名*

Physical Review D, 107(3), p.032005_1 - 032005_6, 2023/02

 被引用回数:4 パーセンタイル:49.66(Astronomy & Astrophysics)

Based on a data sample of 983 fb$$^{-1}$$ collected with the Belle detector at the KEKB asymmetric-energy $$e^+e^-$$ collider, we present the study of the heavy-flavor-conserving decay $$Xi_{c}^{0}to Lambda_{c}^{+}pi^{-}$$ with $$Lambda_{c}^{+}$$ reconstructed via its $$pK^{-} pi^{+}$$ decay mode. The branching fraction ratio $$mathcal{B}(Xi_{c}^{0}to Lambda_{c}^{+}pi^{-})/mathcal{B}(Xi_{c}^{0}to Xi^{-}pi^{+})$$ is measured to be $$0.38 pm 0.04 pm 0.04$$. Combing with the world average value of $$mathcal{B}(Xi_{c}^{0}to Xi^{-}pi^{+})$$, the branching fraction $$mathcal{B}(Xi_{c}^{0}to Lambda_{c}^{+}pi^{-})$$ is deduced to be $$(0.54 pm 0.05 pm 0.05 pm 0.12)%$$. Here, the uncertainties above are statistical, systematic, and from $$mathcal{B}(Xi_c^{0} to Xi^{-}pi^{+})$$, respectively.

論文

First search for the weak radiative decays $$Lambda_c^+ to Sigma^+ gamma$$ and $$Xi_c^0 to Xi^0 gamma$$

Li, Y.*; 谷田 聖; Belle Collaboration*; 他187名*

Physical Review D, 107(3), p.032001_1 - 032001_11, 2023/02

 被引用回数:2 パーセンタイル:29.46(Astronomy & Astrophysics)

We present the first search for the weak radiative decays $$Lambda_c^+ to Sigma^+ gamma$$ and $$Xi_c^0 to Xi^0 gamma$$ using a data sample of 980~fb$$^{-1}$$ collected by the Belle detector operating at the KEKB asymmetric-energy $$e^+e^-$$ collider. There are no evident $$Lambda_c^+ to Sigma^+ gamma$$ or $$Xi_c^0 to Xi^0 gamma$$ signals. Taking the decays $$Lambda_c^+ to p K^- pi^+$$ and $$Xi_c^0 to Xi^- pi^+$$ as normalization channels, the upper limits at 90% credibility level on the ratios of branching fractions $${cal B}(Lambda_c^+ to Sigma^+ gamma)/{cal B}(Lambda_c^+ to p K^{-} pi^+) < 4.0 times 10^{-3}$$ and $${cal B}(Xi_c^0 to Xi^0 gamma)/{cal B}(Xi_c^0 to Xi^- pi^+) < 1.2 times 10^{-2}$$ are determined. We obtain the upper limits at 90% credibility level on the absolute branching fractions $${cal B}(Lambda_c^+ to Sigma^+ gamma) < 2.6 times 10^{-4}$$ and $${cal B}(Xi_c^0 to Xi^0 gamma) < 1.8 times 10^{-4}$$.

論文

Pole position of $$Lambda(1405)$$ measured in $$d(K^-,n)piSigma$$ reactions

相川 脩*; 橋本 直; 谷田 聖; 他73名*

Physics Letters B, 837, p.137637_1 - 137637_8, 2023/02

 被引用回数:10 パーセンタイル:79.31(Astronomy & Astrophysics)

We measured a set of $$pi^pmSigma^mp$$, $$pi^0Sigma^0$$, and $$pi^-Sigma^0$$ invariant mass spectra below and above the $$bar{K}N$$ mass threshold in $$K^-$$-induced reactions on deuteron. We deduced the $$S$$-wave$$bar{K}NrightarrowpiSigma$$ and $$bar{K}Nrightarrowbar{K}N$$ scattering amplitudes in the isospin 0 channel in the framework of a $$bar{K}N$$ and $$piSigma$$ coupled channel. We find that a resonance pole corresponding to $$Lambda(1405)$$ is located at 1417.7$$^{+6.0}_{-7.4}$$(fitting errors)$$^{+1.1}_{-1.0}$$(systematic errors) + $$[-26.1^{+6.0}_{-7.9}$$(fitting errors)$$^{+1.7}_{-2.0}$$(systematic errors)]$$i$$ MeV/$$c^2$$, closer to the $$bar{K}N$$ mass threshold than the value determined by the Particle Data Group.

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