NSR Query Results
Output year order : Descending NSR database version of March 18, 2024. Search: Author = T.Sato Found 124 matches. Showing 1 to 100. [Next]2023IS02 Phys.Rev. C 107, 024306 (2023) Y.Ishibashi, A.Gladkov, Y.Ichikawa, A.Takamine, H.Nishibata, T.Sato, H.Yamazaki, T.Abe, J.M.Daugas, T.Egami, T.Fujita, G.Georgiev, K.Imamura, T.Kawaguchi, W.Kobayashi, Y.Nakamura, A.Ozawa, M.Sanjo, N.Shimizu, D.Tominaga, L.C.Tao, K.Asahi, H.Ueno Nuclear magnetic moment of the neutron-rich nucleus 21O NUCLEAR MOMENTS 21O; measured Iβ, b(θ), β-NMR spectra; deduced g-factor, J and π of the ground state as 5/2+ based on comparison to single-particle g-factors, configuration, magnetic moment for the 5/2+ ground state. Comparison to shell-model predictions using the USD, YSOX, and SDPF-M interactions and to random phase approximation (RPA) based calculations. Measured with β-ray detected nuclear magnetic resonance (β-NMR) spectroscopy. Spin-polarized 21O beam produced in 9Be(22Ne, X), E=70 MeV/nucleon reaction, followed by separation of 21O fragments using RIPS separator at RIKEN.
doi: 10.1103/PhysRevC.107.024306
2022OR04 Phys.Rev. C 106, 064301 (2022) R.Orlandi, H.Makii, K.Nishio, K.Hirose, M.Asai, K.Tsukada, T.K.Sato, Y.Ito, F.Suzaki, Y.Nagame, A.N.Andreyev, E.Ideguchi, N.Aoi, T.T.Pham, S.Q.Yan, Y.P.Shen, B.Gao, G.Li New K isomers in 248Cf NUCLEAR REACTIONS 249Cf(18O, 19O)248Cf, E=140.4 MeV; measured reaction products, Eγ, Iγ, γγ-coin, particleγ-coin. 248Cf; deduced levels, J, π, transitions from isomeric states, T1/2 for 2 low-ling transitions, B(E1). Discussed possible configuration of newly observed isomeric state at 950 keV to be two-quasineutron K=8- and the two-quasiproton K=5-. Comparison to other experimental data. Radioactive target. Si-detectors array combined with γ-ray detector array consisted of 4 Ge detectors and 4 4x5 inch LaBr3 scintillators at Tokai Tandem accelerator facility of the Japan Atomic Energy Agency (JAEA).
doi: 10.1103/PhysRevC.106.064301
2022TI01 Nucl.Instrum.Methods Phys.Res. A1026, 166151 (2022) Yu.E.Titarenko, V.F.Batyaev, K.V.Pavlov, A.Yu.Titarenko, S.V.Malinovskiy, V.I.Rogov, V.M.Zhivun, T.V.Kulevoy, M.V.Chauzova, R.S.Khalikov, A.V.Ignatyuk, V.Yu.Blandinskiy, A.A.Kovalishin, M.I.Baznat, A.Yu.Stankovskiy, A.I.Dubrouski, H.I.Kiyavitskaya, T.Xue, Y.Tian, M.Zeng, Z.Zeng, O.Normahmedov, T.Sato 206, 207, 208, natPb(p, x)194Hg and 209Bi(p, x)194Hg excitation functions in the energy range 0.04-2.6 GeV NUCLEAR REACTIONS Pb, 209Bi(p, X)194Hg, E=0.04-2.6 GeV; measured reaction products, Eγ, Iγ; deduced production σ. Comparison with theoretical calculations.
doi: 10.1016/j.nima.2021.166151
2021HO17 Prog.Theor.Exp.Phys. 2021, 103D03 (2021) W.Horiuchi, T.Sato, Y.Uesaka, K.Yoshida Electron wave functions in beta-decay formulas revisited (I): Gamow-Teller and spin-dipole contributions to allowed and first-forbidden transitions RADIOACTIVITY 160Sn, 80Ni(β-); calculated T1/2 using LO and NLO formulas; deduced impact of Coulomb effects on the beta-decay rate.
doi: 10.1093/ptep/ptab069
2020BO04 Phys.Rev.Lett. 124, 112501 (2020) F.Boulay, G.S.Simpson, Y.Ichikawa, S.Kisyov, D.Bucurescu, A.Takamine, D.S.Ahn, K.Asahi, H.Baba, D.L.Balabanski, T.Egami, T.Fujita, N.Fukuda, C.Funayama, T.Furukawa, G.Georgiev, A.Gladkov, M.Hass, K.Imamura, N.Inabe, Y.Ishibashi, T.Kawaguchi, T.Kawamura, W.Kim, Y.Kobayashi, S.Kojima, A.Kusoglu, R.Lozeva, S.Momiyama, I.Mukul, M.Niikura, H.Nishibata, T.Nishizaka, A.Odahara, Y.Ohtomo, D.Ralet, T.Sato, Y.Shimizu, T.Sumikama, H.Suzuki, H.Takeda, L.C.Tao, Y.Togano, D.Tominaga, H.Ueno, H.Yamazaki, X.F.Yang, J.M.Daugas g Factor of the 99Zr(7/2+) Isomer: Monopole Evolution in the Shape-Coexisting Region RADIOACTIVITY 99Zr(IT) [from 9Be(238U, X), E=345 MeV/nucleon];measured decay products, Eγ, Iγ; deduced g-ray energies, J, π, level scheme, g-factor using a method of time-differential perturbed angular distribution (TDPAD), T1/2. Comparison with IBFM-1 calculations.
doi: 10.1103/PhysRevLett.124.112501
2020DU01 Phys.Rev. C 101, 014309 (2020) E.Dupont, A.Astier, C.M.Petrache, B.F.Lv, I.Deloncle, J.Kiener, R.Orlandi, H.Makii, K.Nishio, K.Hirose, M.Asai, T.K.Sato, K.Tsukada, Y.Ito, K.R.Kean, R.Yanagihara, G.Scamps New excited 2+ and 3- two-proton states in 21084Po126 populated by two-proton transfer NUCLEAR REACTIONS 208Pb(12C, 10Be)9Be/10Be/11B/12C/13C, 14C/210Po, E=58, 60, 62, 63.7 MeV; measured reaction products, light beamlike ejectiles, Eγ, Iγ, (charged particles)γ-coin at the 18 MV tandem of JAEA Tokai. 210Po; deduced six 2+ and three 3- levels in two-proton stripping reaction, configurations.
doi: 10.1103/PhysRevC.101.014309
2020HA27 Phys.Rev. C 102, 024625 (2020) H.Haba, F.Fan, D.Kaji, Y.Kasamatsu, H.Kikunaga, Y.Komori, N.Kondo, H.Kudo, K.Morimoto, K.Morita, M.Murakami, K.Nishio, J.P.Omtvedt, K.Ooe, Z.Qin, D.Sato, N.Sato, T.K.Sato, Y.Shigekawa, A.Shinohara, M.Takeyama, T.Tanaka, A.Toyoshima, K.Tsukada, Y.Wakabayashi, Y.Wang, S.Wulff, S.Yamaki, S.Yano, Y.Yasuda, T.Yokokita Production of 266Bh in the 248Cm(23Na, 5n)266Bh reaction and its decay properties RADIOACTIVITY 266,267Bh(α)[from 248Cm(23Na, 5n), (23Na, 4n), E=125.9, 130.6, 135.3 MeV]; 262Db(α), (SF)[from 266Bh α decay]; 263Db(EC), (α), (SF)[from 267Bh α decay]; 263Rf(SF)[from 263Db EC decay]; 258Lr(α), (EC)[from 262Db α decay]; 259Lr(α), (SF)[from 263Db α decay]; 258No(SF)[from 258Lr(EC); measured Eα, αα-, ααα- and α(SF)-correlations for 32 observed events using rotating wheel apparatus MANON and gas-jet transport system coupled to gas-filled recoil ion separator GARIS at RIKEN; deduced decay times, half-lives, decay branching ratios, production cross sections for 266Bh and 267Bh. Comparison with previous experimental results for half-lives and branching ratios for decay modes. NUCLEAR REACTIONS 248Cm(23Na, 5n), (23Na, 4n), E=125.9, 130.6, 135.3 MeV; measured reaction products, σ(E) at RIKEN. Comparison with HIVAP calculations, and with previous experimental results.
doi: 10.1103/PhysRevC.102.024625
2020IS04 Phys.Rev. C 101, 052201 (2020) T.Ishikawa, H.Fujimura, H.Fukasawa, R.Hashimoto, Q.He, Y.Honda, A.Hosaka, T.Iwata, S.Kaida, J.Kasagi, A.Kawano, S.Kuwasaki, K.Maeda, S.Masumoto, M.Miyabe, F.Miyahara, K.Mochizuki, N.Muramatsu, A.Nakamura, S.X.Nakamura, K.Nawa, S.Ogushi, Y.Okada, K.Okamura, Y.Onodera, K.Ozawa, Y.Sakamoto, M.Sato, T.Sato, H.Shimizu, H.Sugai, K.Suzuki, Y.Tajima, S.Takahashi, Y.Taniguchi, Y.Tsuchikawa, H.Yamazaki, R.Yamazaki, H.Y.Yoshida wN scattering length from w photoproduction on the proton near the reaction threshold NUCLEAR REACTIONS 1H(γ, ω), E=1.09-1.15 GeV; measured Eγ, Iγ, differential σ(θ), and total σ(Eγ) using the FOREST detector at the Research Center for Electron Photon Science of Tohoku University; deduced scattering parameters, spin-averaged scattering length, and effective range. Comparison with other experimental results and with theoretical predictions.
doi: 10.1103/PhysRevC.101.052201
2020RA23 Nucl.Instrum.Methods Phys.Res. B484, 29 (2020) H.N.Ratliff, N.Matsuda, S.-i.Abe, T.Miura, T.Furuta, Y.Iwamoto, T.Sato Modernization of the DCHAIN-PHITS activation code with new features and updated data libraries
doi: 10.1016/j.nimb.2020.10.005
2020TI03 Nucl.Instrum.Methods Phys.Res. A984, 164635 (2020) Y.E.Titarenko, V.F.Batyaev, K.V.Pavlov, A.Y.Titarenko, S.V.Malinovskiy, V.I.Rogov, V.M.Zhivun, T.V.Kulevoy, M.V.Chauzova, S.V.Lushin, A.S.Busygin, A.V.Ignatyuk, P.N.Alekseev, V.Y.Blandinskiy, A.A.Kovalishin, S.I.Tyutyunnikov, A.A.Baldin, A.N.Sosnin, M.I.Baznat, A.Y.Stankovskiy, A.I.Dubrouski, H.I.Kiyavitskaya, T.Xue, Y.Tian, M.Zeng, Z.Zeng, T.Sato 208, 207, 206, natPb(p, x)207Bi and 209Bi (p, x)207Bi excitation functions in the energy range of 0.04 - 2.6 GeV NUCLEAR REACTIONS 206,207,208Pb, Pb, 209Bi(p, X)207Bi, E=0.04-2.6 GeV; measured reaction products, Eγ, Iγ; deduced σ and uncertainties. Comparison with MCNP-6.1, PHITS, Geant4 and TENDL-2019 calculations.
doi: 10.1016/j.nima.2020.164635
2019IC02 Nat.Phys. 15, 321 (2019) Y.Ichikawa, H.Nishibata, Y.Tsunoda, A.Takamine, K.Imamura, T.Fujita, T.Sato, S.Momiyama, Y.Shimizu, D.S.Ahn, K.Asahi, H.Baba, D.L.Balabanski, F.Boulay, J.M.Daugas, T.Egami, N.Fukuda, C.Funayama, T.Furukawa, G.Georgiev, A.Gladkov, N.Inabe, Y.Ishibashi, T.Kawaguchi, T.Kawamura, Y.Kobayashi, S.Kojima, A.Kusoglu, I.Mukul, M.Niikura, T.Nishizaka, A.Odahara, Y.Ohtomo, T.Otsuka, D.Ralet, G.S.Simpson, T.Sumikama, H.Suzuki, H.Takeda, L.C.Tao, Y.Togano, D.Tominaga, H.Ueno, H.Yamazaki, X.F.Yang Interplay between nuclear shell evolution and shape deformation revealed by the magnetic moment of 75Cu NUCLEAR REACTIONS 27Al(76Zn, p)75Cu, E<345 MeV/nucleon; 9Be(238U, X)76Zn, E= 345 MeV/nucleon; measured reaction products, Eγ, Iγ. 75Cu; deduced γ-ray energies, J, π, nuclear magnetic moment. Comparison with theoretical calculations, systematics.
doi: 10.1038/s41567-018-0410-7
2019XI06 Phys.Rev. C 100, 034315 (2019) Y.Xiao, S.Go, R.Grzywacz, R.Orlandi, A.N.Andreyev, M.Asai, M.A.Bentley, G.de Angelis, C.J.Gross, P.Hausladen, K.Hirose, S.Hofmann, H.Ikezoe, D.G.Jenkins, B.Kindler, R.Leguillon, B.Lommel, H.Makii, C.Mazzocchi, K.Nishio, P.Parkhurst, S.V.Paulauskas, C.M.Petrache, K.P.Rykaczewski, T.K.Sato, J.Smallcombe, A.Toyoshima, K.Tsukada, K.Vaigneur, R.Wadsworth Search for α decay of 104Te with a novel recoil-decay scintillation detector RADIOACTIVITY 108,109Xe, 104,105Te(α)[from 54Fe(58Ni, X), E=250 MeV from the tandem accelerator of the Japan Atomic Energy Agency (JAEA), followed by separation of evaporation residues using Recoil Mass Separator (RMS)]; measured Eα, Iα, αα-correlations using an inorganic scintillator YAP:Ce for implanted nuclei, and a multiwire proportional chamber (MWPC) for α particles; deduced αα-correlations for the 109Xe to 105Te to 101Sn α-decay chain, and no conclusive trace observed for the 108Xe to 104Te to 100Sn α-decay chain, half-life of 108Xe decay, upper limit of 4 ns for the half-life of 104Te; estimated cross section for the production of 108Xe, an order of magnitude lower than the expectation based on earlier cross section measurements and the HIVAP fusion-evaporation code. 109I(p), 108,109Te(α); measured proton and α spectra, half-life of 109I decay. Comparison with data for 108Xe to 104Te to 100Sn α-decay chain reported by 2018Au04.
doi: 10.1103/PhysRevC.100.034315
2018AL24 Prog.Part.Nucl.Phys. 100, 1 (2018) L.Alvarez-Ruso, M.Sajjad Athar, M.B.Barbaro, D.Cherdack, M.E.Christy, P.Coloma, T.W.Donnelly, S.Dytman, A.de Gouvea, R.J.Hill, P.Huber, N.Jachowicz, T.Katori, A.S.Kronfeld, K.Mahn, M.Martini, J.G.Morfin, J.Nieves, G.N.Perdue, R.Petti, D.G.Richards, F.Sanchez, T.Sato, J.T.Sobczyk, G.P.Zeller NuSTEC1 White Paper: Status and challenges of neutrino-nucleus scattering
doi: 10.1016/j.ppnp.2018.01.006
2018OG02 Phys.Rev. C 98, 024611 (2018) T.Ogawa, T.Sato, S.Hashimoto, K.Niita Cluster formation in relativistic nucleus-nucleus collisions NUCLEAR REACTIONS 12C(12C, 12C'), (56Fe, 56Fe'), (208Pb, 208Pb'), 40Ca(40Ca, 40Ca'), 107Ag(107Ag, 107Ag'), E=4, 158 GeV/nucleon; calculated inelastic σ(E). 197Au(C, X), E=10.6 GeV/nucleon; 28Si(Cu, X), E=14.5 GeV/nucleon; 208Pb(C, X), (Cu, X), E=158 GeV, nucleon; calculated charge distribution of reaction products. 28Si(Al, X), (Au, X), E=high; calculated transverse mass distributions of p, π+, π-, d, K-, and K+ in central and peripheral collisions. 208Pb(208Pb, X), E=20, 40, 80, 158 GeV/nucleon; calculated transverse mass distributions of p, p-bar, π-, K-, and K+ in central collisions. Calculations performed with JAMQMD algorithm. Comparison with experimental values.
doi: 10.1103/PhysRevC.98.024611
2018XU05 Phys.Lett. B 782, 619 (2018) Z.Y.Xu, H.Heylen, K.Asahi, F.Boulay, J.M.Daugas, R.P.de Groote, W.Gins, O.Kamalou, A.Koszorus, M.Lykiardopoulou, T.J.Mertzimekis, G.Neyens, H.Nishibata, T.Otsuka, R.Orset, A.Poves, T.Sato, C.Stodel, J.C.Thomas, N.Tsunoda, Y.Utsuno, M.Vandebrouck, X.F.Yang Nuclear moments of the low-lying isomeric 1+ state of 34Al: Investigation on the neutron 1p1h excitation across N=20 in the island of inversion NUCLEAR MOMENTS 32,34Al; measured transition frequencies using β-NMR/NQR techniques; deduced nuclear g factor and quadrupole moments. Comparison with large-scale shell-model calculations using several effective interactions.
doi: 10.1016/j.physletb.2018.06.009
2017NA08 Rep.Prog.Phys. 80, 056301 (2017) S.X.Nakamura, H.Kamano, Y.Hayato, M.Hirai, W.Horiuchi, S.Kumano, T.Murata, K.Saito, M.Sakuda, T.Sato, Y.Suzuki Towards a unified model of neutrino-nucleus reactions for neutrino oscillation experiments
doi: 10.1088/1361-6633/aa5e6c
2017YA10 Eur.Phys.J. A 53, 54 (2017) N.Yamanaka, B.K.Sahoo, N.Yoshinaga, T.Sato, K.Asahi, B.P.Das Probing exotic phenomena at the interface of nuclear and particle physics with the electric dipole moments of diamagnetic atoms: A unique window to hadronic and semi-leptonic CP violation ATOMIC PHYSICS 129Xe, 199Hg, 225Ra; deduced atomic electric dipole moment (relative to the CP-violation coefficient) from LHC and other published data.
doi: 10.1140/epja/i2017-12237-2
2016KA31 Phys.Rev. C 94, 015201 (2016) H.Kamano, S.X.Nakamura, T.-S.H.Lee, T.Sato Isospin decomposition of γN → N* transitions within a dynamical coupled-channels model NUCLEAR REACTIONS 1n(γ, π-)p, E=1101-1996 MeV; 1n(γ, π0)n, E=1202-1912 MeV; 1H(γ, π0)p, E=1869-2092 MeV; 1H(γ, π+)n, E=1313-2092 MeV; analyzed σ(θ), photon asymmetry, target polarization and recoil polarization using database of the INS DAC Services at GWU; deduced transition amplitudes for photoexcitation of the neutron-to-nucleon resonances, helicity amplitudes. Dynamical coupled-channels analysis.
doi: 10.1103/PhysRevC.94.015201
2015IW02 Nucl.Instrum.Methods Phys.Res. A804, 50 (2015) Y.Iwamoto, M.Hagiwara, D.Satoh, S.Araki, H.Yashima, T.Sato, A.Masuda, T.Matsumoto, N.Nakao, T.Shima, T.Kin, Y.Watanabe, H.Iwase, T.Nakamura Characterization of high-energy quasi-monoenergetic neutron energy spectra and ambient dose equivalents of 80-389 MeV 7Li(p, n) reactions using a time-of-flight method NUCLEAR REACTIONS 7Li(p, n), E=80-389 MeV; measured reaction products, En, In; deduced σ. Comparison with available data.
doi: 10.1016/j.nima.2015.09.045
2015KA32 Phys.Rev. C 92, 025205 (2015); Erratum Phys.Rev. C 95, 049903 (2017) H.Kamano, S.X.Nakamura, T.-S.H.Lee, T.Sato Dynamical coupled-channels model of K-p reactions. II. Extraction of Λ* and Σ* hyperon resonances
doi: 10.1103/PhysRevC.92.025205
2015OG02 Phys.Rev. C 92, 024614 (2015); Pub.Note Phys.Rev. C 92, 029904 (2015) T.Ogawa, T.Sato, S.Hashimoto, D.Satoh, S.Tsuda, K.Niita Energy-dependent fragmentation cross sections of relativistic 12C NUCLEAR REACTIONS C(12C, X)11B/10B/10Be/9Be/7Be/8Li/7Li/6Li, E=100-400 MeV/nucleon; measured reaction products, time-of-flight, angular distribution of fragments, fragment production σ(E), double-differential neutron production cross sections at Heavy Ion Medical Accelerator in Chiba. Benchmarked theoretical nuclear reaction models implemented in the Particle and Heavy Ion Transport code System (PHITS) by combining JAERI quantum molecular dynamics nucleus-nucleus reaction model (JQMD) and the statistical decay Generalized Evaporation Model (GEM). Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.92.024614
2015WU02 Phys.Rev. C 91, 035203 (2015) Incoherent pion production in neutrino-deuteron interactions NUCLEAR REACTIONS 2H(γ, X), E=208-343 MeV; calculated differential σ(E, θ), total σ(E). 2H(ν, X), E(outgoing muon)=550, 600, 650 MeV; calculated differential σ(E, θ) as function of pion scattering and other variables. Comparison with experimental data. Prediction of the cross sections of electroweak pion production on the deuteron in the energy region near the Δ(1232) resonance. Multiple scattering formulation.
doi: 10.1103/PhysRevC.91.035203
2014HA13 Nucl.Instrum.Methods Phys.Res. B333, 27 (2014) S.Hashimoto, Y.Iwamoto, T.Sato, K.Niita, A.Boudard, J.Cugnon, J.-C.David, S.Leray, D.Mancusi New approach to description of (d, xn)(d, xn) spectra at energies below 50 MeV in Monte Carlo simulation by intra-nuclear cascade code with Distorted Wave Born Approximation NUCLEAR REACTIONS Li, 9Be, C(d, n), (d, X), E=12-30 MeV; analyzed available data; calculated σ(θ), σ(θ, E). DWBA calculations, comparison with available data.
doi: 10.1016/j.nimb.2014.04.007
2014HA21 Nucl.Data Sheets 118, 258 (2014) S.Hashimoto, O.Iwamoto, Y.Iwamoto, T.Sato, K.Niita New Approach for Nuclear Reaction Model in the Combination of Intra-nuclear Cascade and DWBA NUCLEAR REACTIONS 7Li(p, n), E=45 MeV;9Be(p, n), E=50 MeV; calculated σ(θ). Compared with data. 7Li(p, xn), E=39, 43 MeV;9Be(p, xn), E-35, 39 MeV;calculated σ(En, θ=00). Compared with data and other calculations. Intranuclear cascade plus DWBA.
doi: 10.1016/j.nds.2014.04.052
2014HA38 Nucl.Instrum.Methods Phys.Res. A747, 41 (2014) H.Hayashi, M.Shibata, M.Asai, A.Osa, T.K.Sato, M.Koizumi, A.Kimura, M.Oshima Performance of a total absorption clover detector for Qβ measurements of neutron-rich nuclei far from the β-stability line RADIOACTIVITY 160,161,162,163,164,165,166Eu, 163,165Gd(β-); measured decay products, Eβ, Iβ, Eγ, Iγ; deduced T1/2 and their uncertainties. Comparison with available data.
doi: 10.1016/j.nima.2014.02.012
2014KA49 Phys.Rev. C 90, 065204 (2014) H.Kamano, S.X.Nakamura, T.-S.H.Lee, T.Sato Dynamical coupled-channels model of K-p reactions: Determination of partial-wave amplitudes
doi: 10.1103/PhysRevC.90.065204
2014SA21 Radiochim.Acta 102, 211 (2014) N.Sato, T.K.Sato, M.Asai, A.Toyoshima, K.Tsukada, Z.J.Li, K.Nishio, Y.Nagame, M.Schadel, H.Haba, S.Ichikawa, H.Kikunaga Production of 256Lr in the 249, 250, 251Cf + 11B, 243Am + 18O, and 248Cm + 14N reactions NUCLEAR REACTIONS 249,250,251Cf(11B, xn)256Lr, E=65.1-76.4 MeV; 243Am(18O, 5n), E=106.9-112.4 MeV; 248Cm(14N, 6n), E=101.5 MeV; measured reaction products, Eα, Iα; deduced σ, T1/2. Comparison with available data.
doi: 10.1515/ract-2014-2142
2013KA41 Phys.Rev. C 88, 035209 (2013) H.Kamano, S.X.Nakamura, T.-S.H.Lee, T.Sato Nucleon resonances within a dynamical coupled-channels model of πN and γN reactions
doi: 10.1103/PhysRevC.88.035209
2013MU08 Phys.Rev. C 88, 024618 (2013) M.Murakami, S.Goto, H.Murayama, T.Kojima, H.Kudo, D.Kaji, K.Morimoto, H.Haba, Y.Kudou, T.Sumita, R.Sakai, A.Yoneda, K.Morita, Y.Kasamatsu, H.Kikunaga, T.K.Sato Excitation functions for production of Rf isotopes in the 248Cm + 18O reaction NUCLEAR REACTIONS 248Cm(18O, xn)260Rf/261Rf/261mRf/262Rf, E=88.2, 90.2, 94.8, 101.3 MeV; measured reaction products, Eα, Iα, production σ(E), half-lives using GARIS separator at RIKEN Heavy-Ion Linear Accelerator facility. Beam on-off method. Comparison with previous experimental data, and with theoretical predictions using HIVAP computer code. RADIOACTIVITY 260,261,261m,262Rf(α), (SF)[from 248Cm(18O, xn), E=88.2, 90.2, 94.8, 101.3 MeV]; 257No(α)[from 261Rf α decay]; measured Eα, Iα, α-α correlations, SF-events, half-lives; deduced excitation functions.
doi: 10.1103/PhysRevC.88.024618
2013NA16 J.Phys.Soc.Jpn. 82, 064201 (2013) Y.Nagai, K.Hashimoto, Y.Hatsukawa, H.Saeki, S.Motoishi, N.Sato, M.Kawabata, H.Harada, T.Kin, K.Tsukada, T.K.Sato, F.Minato, O.Iwamoto, N.Iwamoto, Y.Seki, K.Yokoyama, T.Shiina, A.Ohta, N.Takeuchi, Y.Kawauchi, N.Sato, H.Yamabayashi, Y.Adachi, Y.Kikuchi, T.Mitsumoto, T.Igarashi Generation of Radioisotopes with Accelerator Neutrons by Deuterons NUCLEAR REACTIONS 100Mo(n, 2n), E<20 MeV; measured reaction products, Eγ, Iγ; deduced yields. Comparison with available data.
doi: 10.7566/JPSJ.82.064201
2013OG02 Nucl.Instrum.Methods Phys.Res. B300, 35 (2013) T.Ogawa, M.N.Morev, T.Sato, S.Hashimoto Analysis of fragmentation excitation functions of lead by carbon ions up to 400 MeV/u NUCLEAR REACTIONS Pb(C, X)24Na/28Mg/43K/46Sc/48V/54Mn/56Co/59Fe/60Co/65Zn/74As/75Se/76As/83Rb/85Sr/121Te/126I/127Xe/133Ba/139Ce/141Ce/143Pm/144Pm/146Gd/147Gd/149Gd/151Tb/169Lu/169Yb/172Hf/173Lu/175Hf, E<400 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced yields, σ. Comparison with experimental data, PHITS calculations.
doi: 10.1016/j.nimb.2013.01.031
2013OH05 Phys.Rev. C 88, 025204 (2013) S.Ohnishi, Y.Ikeda, H.Kamano, T.Sato Signature of strange dibaryons in kaon- and photon-induced reactions
doi: 10.1103/PhysRevC.88.025204
2012HI03 Eur.Phys.J. A 48, 54 (2012) Y.Hirayama, M.Mihara, Y.X.Watanabe, S.C.Jeong, H.Miyatake, S.Momota, T.Hashimoto, N.Imai, K.Matsuta, H.Ishiyama, S.Ichikawa, T.Ishii, T.Izumikawa, I.Katayama, H.Kawakami, H.Kawamura, I.Nishinaka, K.Nishio, H.Makii, S.Mitsuoka, A.Osa, Y.Otokawa, T.K.Sato Tilted-foil technique for producing a spin-polarized radioactive isotope beam
doi: 10.1140/epja/i2012-12054-1
2011HI15 Eur.Phys.J. A 47, 138 (2011) Y.Hirayama, M.Mihara, Y.X.Watanabe, S.C.Jeong, N.Imai, K.Matsuta, H.Miyatake, T.Hashimoto, H.Ishiyama, S.Ichikawa, T.Ishii, T.Izumikawa, I.Katayama, H.Kawakami, I.Nishinaka, K.Nishio, H.Makii, S.Mitsuoka, S.Momota, A.Osa, Y.Otokawa, T.K.Sato, Y.Wakabayashi Spin-polarization of radioactive 123Ing.s. by the tilted-foil method RADIOACTIVITY 123In(β-)[from U(p, F), E=34 MeV]; measured Iβ(θ, t), β polarization using tilted multifoils at ISOL-based facility TRIAC and β-NMR technique; deduced asymmetry.
doi: 10.1140/epja/i2011-11138-8
2011HO09 Int.J.Mod.Phys. E20, 781 (2011) Electro-weak transitions of 4He using realistic nuclear interactions
doi: 10.1142/S0218301311018666
2011IW07 Nucl.Instrum.Methods Phys.Res. A 629, 43 (2011) Y.Iwamoto, M.Hagiwara, D.Satoh, H.Iwase, H.Yashima, T.Itoga, T.Sato, Y.Nakane, H.Nakashima, Y.Sakamoto, T.Tatsumoto, A.Masuda, J.Nishiyama, A.Tamii, K.Hatanaka, C.Theis, E.Feldbaumer, L.Jaegerhofer, C.Pioch, V.Mares, T.Nakamura Quasi-monoenergetic neutron energy spectra for 246 and 389 MeV 7Li(p, n) reactions at angles from 0 deg to 30 degree NUCLEAR REACTIONS Li(p, x), 7Li(p, n), E=246-389 MeV; measured products, Eν, Iν; deduced σ(θ). Data were imported from EXFOR entry E2297.
doi: 10.1016/j.nima.2010.12.022
2011NI15 J.Korean Phys.Soc. 59, 827s (2011) K.Niita, Y.Iwamoto, T.Sato, N.Matsuda, Y.Sakamoto, H.Nakashima, H.Iwase, L.Sihver Event Generator Models in the Particle and Heavy Ion Transport Code System; PHITS NUCLEAR REACTIONS C(n, n'), (n, γ)E=15 MeV; calculated σ(En, θ). C(n, X), E=0-20 MeV; calculated Kerma factor, energy of produced photons. 56Fe(n, X), E=1.E-6-20 MeV; calculated displacement σ. Pb(n, n'), E=3 GeV; calculated σ(E, θ). Si(n, X), E=19 MeV; calculated deposit energy distribution. Quantum Molecular Dynamics, PHITS code. Compared to ENDF data.
doi: 10.3938/jkps.59.827
2011NI17 J.Korean Phys.Soc. 59, 1640s (2011) K.Niita, H.Iwase, Y.Iwamoto, T.Sato, N.Matsuda, Y.Sakamoto, H.Nakashima, L.Sihver Applicability of the PHITS Code to Heavy Ion Accelerator Facilities NUCLEAR REACTIONS 208Pb(12C, n), E=400 MeV/nucleon; calculated σ(En, θ) using JQMD (JAERI Quantum Molecular Dynamics) incorporated into PHITS code. Compared with data.
doi: 10.3938/jkps.59.1640
2010IK02 Nucl.Phys. A835, 386c (2010) On the resonance energy of the strange dibaryon
doi: 10.1016/j.nuclphysa.2010.01.225
2010KA20 Phys.Rev. C 81, 065207 (2010) H.Kamano, S.X.Nakamura, T.-S.H.Lee, T.Sato Extraction of P11 resonances from πN data
doi: 10.1103/PhysRevC.81.065207
2010NA04 Phys.Rev. C 81, 035502 (2010) S.X.Nakamura, T.Sato, T.-S.H.Lee, B.Szczerbinska, K.Kubodera Dynamical model of coherent pion production in neutrino-nucleus scattering NUCLEAR REACTIONS 12C(π-, X), E=75-275 MeV; calculated total cross section. 12C(π+, π+), E=40, 80 MeV; 12C(π-, π-), E=120, 180, 230, 280 MeV; 12C(γ, π0), E=173 MeV; 12C(γ, π0), E(cm)=200, 290, 350 MeV; calculated σ(θ) of differential cross section. 12C(ν, X), E=0.2-1.5 GeV; calculated σ, pion and muon momentum distributions. Microscopic dynamical model describing neutrino-induced coherent pion production. Comparisons with experimental data.
doi: 10.1103/PhysRevC.81.035502
2010SA30 Radiat.Meas. 45, 1159 (2010) D.Satoh, Y.Iwamoto, M.Hagiwara, H.Iwase, H.Yashima, T.Sato, A.Endo, Y.Sakamoto, Y.Nakane, H.Nakashima, T.Nakamura, A.Tamii, K.Hatanaka Measurement of neutron elastic scattering cross sections for carbon at 134 MeV NUCLEAR REACTIONS C(n, n), E=134 MeV; measured neutron time of flight (TOF); deduced σ(θ). Comparison with other measurements, JENDL/HE-2007 and ENDF/B-VII.0 libraries.
doi: 10.1016/j.radmeas.2010.06.064
2010SU01 Phys.Rev.Lett. 104, 042302 (2010) N.Suzuki, B.Julia-Diaz, H.Kamano, T.-S.H.Lee, A.Matsuyama, T.Sato Disentangling the Dynamical Origin of P11 Nucleon Resonances
doi: 10.1103/PhysRevLett.104.042302
2010SU25 Phys.Rev. C 82, 045206 (2010) Extraction of electromagnetic transition form factors for nucleon resonances within a dynamical coupled-channels model
doi: 10.1103/PhysRevC.82.045206
2010TA14 J.Nucl.Sci.Technol.(Tokyo) 47, 932 (2010) M.Takada, K.Yajima, H.Yasuda, T.Sato, T.Nakamura Measurement of Atmospheric Neutron and Photon Energy Spectra at Aviation Altitudes using a Phoswich-Type Neutron Detector
doi: 10.1080/18811248.2010.9720972
2009HA11 Phys.Lett. B 674, 276 (2009) T.Hashimoto, H.Ishiyama, Y.X.Watanabe, Y.Hirayama, N.Imai, H.Miyatake, S.C.Jeong, M.-H.Tanaka, N.Yoshikawa, T.Nomura, S.Mitsuoka, K.Nishio, T.K.Sato, A.Osa, S.Ichikawa, M.Matsuda, H.Ikezoe, S.K.Das, Y.Mizoi, T.Fukuda, A.Sato, T.Shimoda, K.Otsuki, T.Kajino A new measurement of the astrophysical 8Li(d, t)7Li reaction NUCLEAR REACTIONS 2H(8Li, t), E=0.18, 0.24, 0.30, 0.40, 0.46, 0.60, 0.75 MeV/nucleon; measured charged-particle spectra, σ, σ(θ), σ(E); deduced 7Li excitation energy spectra, astrophysical reaction rate. Comparison with other data.
doi: 10.1016/j.physletb.2009.03.031
2009IK01 Phys.Rev. C 79, 035201 (2009) Resonance energy of the K-bar NN - π YN system
doi: 10.1103/PhysRevC.79.035201
2009JU04 Phys.Rev. C 80, 025207 (2009) B.Julia-Diaz, H.Kamano, T.-S.H.Lee, A.Matsuyama, T.Sato, N.Suzuki Dynamical coupled-channels analysis of 1H(e, e'π)N reactions
doi: 10.1103/PhysRevC.80.025207
2009KA08 Phys.Rev. C 79, 025206 (2009) H.Kamano, B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato Dynamical coupled-channels study of πN → ππN reactions
doi: 10.1103/PhysRevC.79.025206
2009KA39 Phys.Rev. C 80, 065203 (2009) H.Kamano, B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato Double and single pion photoproduction within a dynamical coupled-channels model
doi: 10.1103/PhysRevC.80.065203
2009KI06 Phys.Rev. C 80, 015206 (2009) Y.Kim, T.Sato, F.Myhrer, K.Kubodera Two-pion-exchange and other higher-order contributions to the pp → ppπ0 reaction NUCLEAR REACTIONS p(p, p)pπ0, E not given; calculated contributions to the threshold reaction amplitude with the use of the momentum coupling scheme (MCS) in the plane-wave approximation and in the frozen kinematics approximation (FKA). Comparison with the Weinberg scheme.
doi: 10.1103/PhysRevC.80.015206
2009NA26 Phys.Rev. C 80, 035802 (2009) S.X.Nakamura, K.Sumiyoshi, T.Sato Neutrino deuteron reaction in the heating mechanism of core-collapse supernovae NUCLEAR REACTIONS 2H(ν, e2p), (ν, e+2n), (ν, ν'np), (ν, d), E=0-140 MeV; calculated total σ and energy transfer cross sections reactions with the phenomenological Lagrangian approach. Comparison with ν+3H, ν+3He and ν+4He reactions.
doi: 10.1103/PhysRevC.80.035802
2009SU02 Phys.Rev. C 79, 025205 (2009) Extraction of resonances from meson-nucleon reactions
doi: 10.1103/PhysRevC.79.025205
2008CA12 Eur.Phys.J. A 35, 253 (2008) S.Capstick, A.Svarc, L.Tiator, J.Gegelia, M.M.Giannini, E.Santopinto, C.Hanhart, S.Scherer, T.-S.H.Lee, T.Sato, N.Suzuki The physical meaning of scattering matrix singularities in coupled-channel formalisms BRAG 2007 Workshop summary
doi: 10.1140/epja/i2007-10576-1
2008DU17 Phys.Rev. C 78, 025204 (2008) J.Durand, B.Julia-Diaz, T.-S.H.Lee, B.Saghai, T.Sato Coupled-channels study of the π- p → ηn process
doi: 10.1103/PhysRevC.78.025204
2008JU04 Phys.Rev. C 77, 045205 (2008) B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato, L.C.Smith Dynamical coupled-channels effects on pion photoproduction NUCLEAR REACTIONS p(γ, p)π0, E=1154-1632 MeV; calculated cross sections, angular distributions using dynamical coupled-channel model. Comparison with experimental data.
doi: 10.1103/PhysRevC.77.045205
2008OS02 Nucl.Instrum.Methods Phys.Res. B266, 4394 (2008) A.Osa, S.-i.Ichikawa, M.Matsuda, T.K.Sato, S.-C.Jeong Ion source development for the on-line isotope separator at JAEA NUCLEAR REACTIONS 238U(p, F)163Eu/164Eu/165Eu/166Eu, E=36 MeV; measured separation yields, Eγ, Iγ; deduced T1/2. A forced electron beam induced arc discharge (FEBIAD-B2) type ion source.
doi: 10.1016/j.nimb.2008.05.063
2007HA57 Eur.Phys.J. A 34, 363 (2007) H.Hayashi, Y.Akita, O.Suematsu, M.Shibata, M.Asai, T.K.Sato, S.Ichikawa, I.Nishinaka, Y.Nagame, A.Osa, K.Tsukada, T.Ishii, Y.Kojima, A.Taniguchi Qβ measurements of 158, 159Pm, 159, 161Sm, 160-165Eu, 163Gd and 166Tb using a total absorption BGO detector RADIOACTIVITY 158,159Pm, 159,161Sm, 160,161,162,163,164,165Eu, 163Gd, 166Tb(β-) [from 238U(p, F), E=24 MeV and subsequent decay]; measured Eγ, Iγ, Eβ, Iβ; deduced Qβ, mass excess and two-neutron separation energies. Mass separator.
doi: 10.1140/epja/i2006-10522-9
2007IK01 Phys.Rev. C 76, 035203 (2007) Strange dibaryon resonance in the K-bar nn-π YN system
doi: 10.1103/PhysRevC.76.035203
2007JU01 Phys.Rev. C 75, 015205 (2007) B.Julia-Diaz, T.-S.H.Lee, T.Sato, L.C.Smith Extraction and interpretation of γN → Δ form factors within a dynamical model NUCLEAR REACTIONS 1H(e, e'π0), E=high; analyzed σ(θ), related data; deduced form factors.
doi: 10.1103/PhysRevC.75.015205
2007JU07 Phys.Rev. C 76, 065201 (2007) B.Julia-Diaz, T.-S.H.Lee, A.Matsuyama, T.Sato Dynamical coupled-channels model of πN scattering in the W ≤ 2 GeV nucleon resonance region NUCLEAR REACTIONS p(π-, π-), (π-, π0), E<2 GeV; analyzed pion-nucleon scattering using dynamical coupled-channel model.
doi: 10.1103/PhysRevC.76.065201
2007KI18 Phys.Lett. B 657, 187 (2007) Y.Kim, T.Sato, F.Myhrer, K.Kubodera Two-pion-exchange contributions to the pp → ppπ0 reaction
doi: 10.1016/j.physletb.2007.10.023
2007MA01 Nucl.Instrum.Methods Phys.Res. B254, 30 (2007) D.Mancusi, L.Sihver, K.Gustafsson, C.La Tessa, S.B.Guetersloh, C.J.Zeitlin, J.Miller, L.H.Heilbronn, K.Niita, T.Sato, H.Nakashima, T.Murakami, Y.Iwata PHITS - benchmark of partial charge-changing cross sections for intermediate-mass systems NUCLEAR REACTIONS H, C, Al, Cu, Sn, Pb(40Ar, X), E=400 MeV/nucleon; calculated partial charge-changing σ.
doi: 10.1016/j.nimb.2006.10.070
2007MA11 Phys.Rep. 439, 193 (2007) A.Matsuyama, T.Sato, T.-S.H.Lee Dynamical coupled-channel model of meson production reactions in the nucleon resonance region
doi: 10.1016/j.physrep.2006.12.003
2007SA56 Nucl.Instrum.Methods Phys.Res. A583, 507 (2007) D.Satoh, T.Kurosawa, T.Sato, A.Endo, M.Takada, H.Iwase, T.Nakamura, K.Niita Reevaluation of secondary neutron spectra from thick targets upon heavy-ion bombardment NUCLEAR REACTIONS C, Al, Cu, Pb(C, X), E=400 MeV/nucleon; C, Cu(Si, X), E=800 MeV/nucleon; C, Al, Cu, Pb(Fe, X), E=400 MeV/nucleon; C, Al, Cu, Pb(Xe, X), E=400 MeV/nucleon; analyzed experimental data of secondary neutron spectra, comparisons with calculations using Monte-Carlo heavy-ion transport code PHITS.
doi: 10.1016/j.nima.2007-09-023
2007SU23 Phys.Lett. B 657, 32 (2007) M.Sumihama, J.K.Ahn, H.Akimune, Y.Asano, W.C.Chang, S.Date, H.Ejiri, H.Fujimura, M.Fujiwara, K.Hicks, T.Hotta, K.Imai, T.Ishikawa, T.Iwata, H.Kawai, Z.Y.Kim, K.Kino, H.Kohri, N.Kumagai, S.Makino, T.Matsumura, N.Matsuoka, T.Mibe, M.Miyabe, Y.Miyachi, M.Morita, N.Muramatsu, T.Nakano, M.Niiyama, M.Nomachi, Y.Ohashi, H.Ohkuma, T.Ooba, D.S.Oshuev, C.Rangacharyulu, A.Sakaguchi, T.Sato, P.M.Shagin, Y.Shiino, H.Shimizu, Y.Sugaya, H.Toyokawa, A.Wakai, C.W.Wang, S.C.Wang, K.Yonehara, T.Yorita, M.Yosoi, R.G.T.Zegers Backward-angle photoproduction of π0 mesons on the proton at Eγ = 1.5-2.4 GeV NUCLEAR REACTIONS 1H(polarized γ, π0), E=1.5-2.4 GeV; measured missing mass spectra, σ(E, θ), beam asymmetry.
doi: 10.1016/j.physletb.2007.10.032
2007SZ03 Phys.Lett. B 649, 132 (2007) B.Szczerbinska, T.Sato, K.Kubodera, T.-S.H.Lee Neutrino-nucleus reactions in the delta resonance region NUCLEAR REACTIONS 12C(ν, X), (e, X), E=1, 1.1 GeV; calculated e-, μ energy spectra, σ(θ, Q2). Sato-Lee model.
doi: 10.1016/j.physletb.2007.03.046
2006KI01 Phys.Rev. C 73, 025202 (2006) Y.Kim, I.Danchev, K.Kubodera, F.Myhrer, T.Sato Use of Vlow-k in a chiral-perturbation-theory description of the pp → ppπ0 reaction NUCLEAR REACTIONS 1H(p, p'π0), E=280-320 MeV; calculated σ. Chiral perturbation theory, comparison with data.
doi: 10.1103/PhysRevC.73.025202
2006KI08 Prog.Theor.Phys.(Kyoto) 116, 241 (2006) Θ+: Another Explanation and Prediction
doi: 10.1143/PTP.116.241
2006KU20 Nucl.Phys. B(Proc.Supp.) S159, 21 (2006) K.Kubodera, S.Nakamura, T.Sato Neutrino-nucleus reactions in the energy range 1-100 MeV
doi: 10.1016/j.nuclphysbps.2006.08.023
2006SA36 Nucl.Phys. B(Proc.Supp.) S159, 141 (2006) T.Sato, B.Szczerbinska, K.Kubodera, T.-S.H.Lee Dynamical model of electroweak pion production in the resonance region NUCLEAR REACTIONS 1H(e, e'π+), (e, e'π0), (ν, eπ+), (ν, μ-π+), E ≈ 1-1.4 GeV; calculated σ(Q2).
doi: 10.1016/j.nuclphysbps.2006.08.030
2005MA63 Phys.Rev. C 72, 025204 (2005) Quark-hadron duality and parity violating asymmetry of electroweak reactions in the Δ region NUCLEAR REACTIONS 1H(e, e'), (ν, e), (ν, ν'), E=high; calculated structure functions. 1H(e, e'π+), (e, e'π0), E=high; calculated polarization observables. 1H(polarized e, e'), E ≈ 0.5-3 GeV; calculated parity-violating asymmetry. Dynamical model, neutral current contributions. Comparisons with data.
doi: 10.1103/PhysRevC.72.025204
2005SA32 Nucl.Phys. B(Proc.Supp.) S149, 221 (2005) Low energy neutrino reaction NUCLEAR REACTIONS 1H(ν, μ-π+), E=0.5-2 GeV; calculated σ. Dynamical model.
doi: 10.1016/j.nuclphysbs.2005.05.095
2005WA19 Nucl.Phys. A754, 327c (2005) T.Watanabe, S.Endo, Y.Fujii, O.Hashimoto, K.Hirose, T.Ishikawa, K.Ito, H.Kanda, M.Katoh, T.Kinoshita, O.Konno, K.Maeda, A.Matsumura, Y.Miura, F.Miyahara, H.Miyase, K.Mizunuma, T.Nakabayashi, S.N.Nakamura, H.Nomura, Y.Okayasu, T.Osaka, A.Otani, M.Oyamada, A.Sasaki, T.Sato, H.Shimizu, T.Takahashi, T.Tamae, H.Tamura, T.Terasawa, H.Tsubota, K.Tsukada, M.Ukai, M.Utoyama, M.Wakamatsu, H.Yamauchi, Y.Yamaguchi, Y.Yamamoto, H.Yamazaki K0 photoproduction on 12C in the threshold region NUCLEAR REACTIONS 12C(γ, K0X), E=0.8-1.1 GeV; measured hyperon production associated invariant mass spectra, kaon production σ.
doi: 10.1016/j.nuclphysa.2005.02.157
2004AN13 Phys.Lett. B 595, 250 (2004) S.Ando, H.W.Fearing, V.Gudkov, K.Kubodera, F.Myhrer, S.Nakamura, T.Sato Neutron beta-decay in effective field theory RADIOACTIVITY 1n(β-); calculated T1/2, angular correlation coefficients, radiative corrections. Effective field theory.
doi: 10.1016/j.physletb.2004.06.037
2004TS09 Phys.Lett. B 602, 60 (2004) K.Tsuji, S.Nakamura, T.Sato, K.Kubodera, F.Myhrer Neutrino magnetic moment contribution to the neutrino-deuteron reaction NUCLEAR REACTIONS 2H(ν, ν'n), E=2.4-20.0 MeV; calculated breakup σ, effect of neutrino magnetic moment.
doi: 10.1016/j.physletb.2004.09.064
2003NA32 Nucl.Phys. A721, 549c (2003) S.Nakamura, T.Sato, S.Ando, T.-S.Park, F.Myhrer, V.Gudkov, K.Kubodera Neutrino-deuteron reactions at solar neutrino energies NUCLEAR REACTIONS 2H(ν, ep), (ν, νn), E=5, 10, 20 MeV; calculated σ. 2H(ν, X), E=0-20 MeV; calculated total charged-current σ.
doi: 10.1016/S0375-9474(03)01121-7
2003SA18 Phys.Rev. C 67, 065201 (2003) Dynamical model of weak pion production reactions NUCLEAR REACTIONS 1n, 1H(ν, μ-π+), E=0.4-2 GeV; 1n(ν, μ-π0), E=0.4-2 GeV; calculated total σ, σ(Q2). Dynamical model, comparisons with data.
doi: 10.1103/PhysRevC.67.065201
2003YA13 Nucl.Phys. A721, 449c (2003) M.Yamaga, M.Dorochenko, T.Inagaki, N.Ishihara, G.Y.Lim, T.Morimoto, H.Okuno, K.Omata, T.Sato, M.Sekimoto, Y.Yoshimura, A.Ajimura, T.Ikei, Y.Ikemoto, M.Nomachi, T.Oba, K.Sakashita, Y.Sugaya, T.Yamanaka, M.Itaya, T.Iwata, T.Hariu, M.Moriya, Y.Tajima, M.Yamamoto, H.Yoshida, Y.Yoshida, A.Lednev, J.Nix, G.Perdue, E.Pod, M.Rawtajizak, Y.Wah, H.Watanabe, V.Baranov, N.Khomouov, A.Kurilin, G.Macharashvili, A.Moissenko, Z.Tsamalaidze, Y.Akune, Y.Fujioka, N.Kawakubo, S.Kobayashi, T.Kojima, J.K.Ahn, H.S.Lee, S.Y.Lee, T.Shinkawa, Y.B.Hsiung, T.Nakano KL → π0νν-bar experiment at KEK 12-GeV PS - E391a-
doi: 10.1016/S0375-9474(03)01096-0
2002LE26 Nucl.Sci.Eng. 142, 1 (2002) G.Leinweber, J.A.Burke, H.D.Knox, N.J.Drindak, D.W.Mesh, W.T.Haines, R.V.Ballad, R.C.Block, R.E.Slovacek, C.J.Werner, M.J.Trbovich, D.P.Barry, T.Sato Neutron Capture and Transmission Measurements and Resonance Parameter Analysis of Samarium NUCLEAR REACTIONS Sm(n, X), (n, γ), E ≈ 0-30 eV; measured transmission and capture σ. 144,147,148,149,150,152,154Sm deduced resonance parameters, resonance integral. 144,147,148,149,150,151,152,154Sm(n, γ), E=thermal; deduced capture σ. Comparison with previous results.
doi: 10.13182/NSE02-A2283
2002NA19 Nucl.Phys. A707, 561 (2002) S.Nakamura, T.Sato, S.Ando, T.-S.Park, F.Myhrer, V.Gudkov, K.Kubodera Neutrino-Deuteron Reactions at Solar Neutrino Energies NUCLEAR REACTIONS 2H(ν, ep), (ν, νp), E=1.5-20.0 MeV; calculated σ. Effective field theory.
doi: 10.1016/S0375-9474(02)00993-4
2001HA17 Phys.Rev. C63, 044002 (2001) C.Hanhart, G.A.Miller, F.Myhrer, T.Sato, U.van Kolck Toy Model for Pion Production in Nucleon-Nucleon Collisions
doi: 10.1103/PhysRevC.63.044002
2001LE14 Nucl.Phys. A684, 327c (2001) Dynamical Study of Δ Excitation with N(e, e'π) Reaction NUCLEAR REACTIONS 1H(e, e'π0), E=high; calculated σ(θ), form factors for Δ resonance production.
doi: 10.1016/S0375-9474(01)00431-6
2001NA08 Phys.Rev. C63, 034617 (2001); Erratum Phys.Rev. C 73, 049904 (2006) S.Nakamura, T.Sato, V.Gudkov, K.Kubodera Neutrino Reactions on the Deuteron NUCLEAR REACTIONS 2H(ν, νp), (ν, ep), (ν, e+n), E=2-170 MeV; calculated σ, σ(E), σ(θ). Phenomenological Lagrangian approach.
doi: 10.1103/PhysRevC.63.034617
2001SA12 Nucl.Phys. A684, 26c (2001) Dynamical Study of Nucleon Resonances in πN and γN Reactions NUCLEAR REACTIONS 1H(γ, π0), E=200-450 MeV; 1H(e, e'π0), E=high; analyzed σ(θ), asymmetry; deduced resonance production mechanism features. Dynamical approach.
doi: 10.1016/S0375-9474(01)00484-5
2001SA17 Phys.Rev. C63, 055201 (2001) Dynamical Study of the Δ Excitation in N(e, e'π) Reaction NUCLEAR REACTIONS 1H(γ, π0), (γ, π+), E=200-450 MeV; 1H(e, e'π0), E=high; calculated σ(θ); deduced Δ resonance excitation features. Dynamical model, comparisons with data.
doi: 10.1103/PhysRevC.63.055201
2001SA26 Nucl.Instrum.Methods Phys.Res. A463, 299 (2001) T.Sato, K.Shin, R.Yuasa, S.Ban, H.Lee Measurement of the Neutron Spectrum by the Irradiation of a 2.04-GeV Electron Beam into Thick Targets NUCLEAR REACTIONS 27Al, Cu, Sn, Pb(e, nX), E=2.04 GeV; measured thick-target neutron spectra.
doi: 10.1016/S0168-9002(01)00245-5
2000DM02 Nucl.Phys. A663-664, 465c (2000) V.Dmitrasinovic, K.Kubodera, F.Myhrer, T.Sato A Next-to-Next-to-Leading-Order pp → ppπ0 Transition Operator in Chiral Perturbation Theory NUCLEAR REACTIONS 1H(p, pπ0), E not given; calculated next-to-leading-order S-wave amplitude.
doi: 10.1016/S0375-9474(99)00632-6
2000YO06 Phys.Rev. C61, 065203 (2000) T.Yoshimoto, T.Sato, M.Arima, T.-S.H.Lee Dynamical Test of Constituent Quark Models with πN Reactions NUCLEAR REACTIONS 1H(π-, nX), E=1400-1900 MeV; calculated η production σ. Constituent quark model, dynamical approach, comparison with data.
doi: 10.1103/PhysRevC.61.065203
1999DM03 Phys.Lett. 465B, 43 (1999) V.Dmitrasinovic, K.Kubodera, F.Myhrer, T.Sato A Next-to-Next-to-Leading-Order pp → ppπ0 Transition Operator in Chiral Perturbation Theory NUCLEAR REACTIONS 1H(p, pπ0), E ≈ threshold; calculated transition operators, corrections. Chiral perturbation theory.
doi: 10.1016/S0370-2693(99)01075-8
1999NA21 Phys.Rev. C60, 017001 (1999) H.Nabetani, T.Ogaito, T.Sato, T.Kishimoto Spin Observables in the pn → p Λ Reaction NUCLEAR REACTIONS 1H(n, pX), E not given; calculated hyperon production associated spin observables.
doi: 10.1103/PhysRevC.60.017001
1999TA33 Prog.Theor.Phys.(Kyoto) 102, 333 (1999) S.Taniguchi, T.Sato, H.Ohtsubo Pion Elastic and Charge-Exchange Scattering on p-Shell Nuclei by Isobar-Doorway State Model NUCLEAR REACTIONS 12C(π-, π-), E=150-230 MeV; 16O(π-, π-), E=163 MeV; 16O(π+, π+), E=114-240 MeV; calculated σ(θ). 13C(π+, π+), E=162-223 MeV; 13C, 15N(π+, π0), E ≈ 165 MeV; calculated σ(θ), Ay(θ). 13C(π-, π-), E=114-226 MeV; calculated Ay(θ). Isobar-doorway state model, comparisons with data.
doi: 10.1143/PTP.102.333
1998DM01 Phys.Rev. C58, 1937 (1998) Partial Conservation of Axial Current Constraints on Pion Production or Absorption within Nonrelativistic Nuclear Dynamics
doi: 10.1103/PhysRevC.58.1937
1998MA92 Prog.Theor.Phys.(Kyoto) 100, 977 (1998) Monte-Carlo Study of Bound States in a Few-Nucleon System - Method of Continued Fractions -
doi: 10.1143/PTP.100.977
1997SA42 Phys.Rev. C56, 1246 (1997) T.Sato, T.-S.H.Lee, F.Myhrer, K.Kubodera Chiral Perturbation Theory and the pp → ppπ0 Reaction Near Threshold NUCLEAR REACTIONS 1H(p, p'X), E=280-320 MeV; analyzed pion production σ(E); deduced rescattering term contribution enhancement. Chiral perturbation theory, momentum-space representation.
doi: 10.1103/PhysRevC.56.1246
1997SA71 Nucl.Instrum.Methods Phys.Res. A401, 476 (1997) T.Sato, K.Shin, S.Ban, Y.Namito, H.Nakamura, H.Hirayama Measurements of High-Energy Photonuclear Reaction Yields in the 2.5 GeV Electron Beam Stop NUCLEAR REACTIONS 27Al, Fe, Cu, Nb(γ, X), E not given; measured radioactive products yield vs depth in electron beam stop. Comparison with theory.
doi: 10.1016/S0168-9002(97)01055-3
1997YU03 J.Phys.Soc.Jpn. 66, 73 (1997) H.Yuki, T.Sato, T.Ohtsuki, T.Yorita, Y.Aoki, H.Yamazaki, J.Kasagi, K.Ishii Measurement of the D(d, p)T Reaction in Ti for 2.5 < E(d) < 6.5 keV and Electron Screening in Metal NUCLEAR REACTIONS, ICPND 2H(d, p), E=2.5-6.5 keV; measured proton spectra, thick target yields, σ; deduced electron screening potential in Ti.
doi: 10.1143/JPSJ.66.73
1996SA33 Phys.Rev. C54, 2660 (1996) Meson-Exchange Model for πN Scattering and γN → πN Reaction NUCLEAR REACTIONS 1H(polarized γ, π0), (γ, π+), E=200-400 MeV; analyzed asymmetry vs E, σ(θ). 1H(γ, π-), E=180-380 MeV; analyzed σ(θ). Meson exchange model.
doi: 10.1103/PhysRevC.54.2660
1995CI02 Phys.Rev. C51, 2406 (1995) A.Cichocki, J.Dubach, R.S.Hicks, G.A.Peterson, C.W.de Jager, H.de Vries, N.Kalantar-Nayestanaki, T.Sato Electron Scattering from 10B NUCLEAR REACTIONS 10B(e, e'), (e, e), E=223.53 MeV; measured spectra, longitudinal, transverse form factors. 10B levels deduced charge distribution, B(λ). Extensive model comparisons.
doi: 10.1103/PhysRevC.51.2406
1995OG06 Prog.Theor.Phys.(Kyoto) 94, 199 (1995) Polarization Phenomena in Hypernuclear Reaction NUCLEAR REACTIONS 12,13C(π+, K+), E at 1.056 GeV/c; 12C(K+, K+), (π+, π+), E at 800 MeV/c; 1H(π-, K0), E at 1.04 GeV/c; analyzed σ(θ); calculated hypernucleus polarization vs θ. 1H(π-, K0), E at 1.04 GeV/c; analyzed polarization vs θ. DWIA.
doi: 10.1143/PTP.94.199
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