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NSR database version of March 18, 2024.

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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1462.


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
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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2676. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1448.


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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2490.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2486.


2015WU02      Phys.Rev. C 91, 035203 (2015)

J.-J.Wu, T.Sato, T.-S.H.Lee

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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2465.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2438. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2409.


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
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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


2011HO09      Int.J.Mod.Phys. E20, 781 (2011)

W.Horiuchi, Y.Suzuki, T.Sato

Electro-weak transitions of 4He using realistic nuclear interactions

doi: 10.1142/S0218301311018666
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2297.


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
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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
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2010IK02      Nucl.Phys. A835, 386c (2010)

Y.Ikeda, H.Kamano, T.Sato

On the resonance energy of the strange dibaryon

doi: 10.1016/j.nuclphysa.2010.01.225
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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
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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
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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
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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
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2010SU25      Phys.Rev. C 82, 045206 (2010)

N.Suzuki, T.Sato, T.-S.H.Lee

Extraction of electromagnetic transition form factors for nucleon resonances within a dynamical coupled-channels model

doi: 10.1103/PhysRevC.82.045206
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2140. Data from this article have been entered in the XUNDL database. For more information, click here.


2009IK01      Phys.Rev. C 79, 035201 (2009)

Y.Ikeda, T.Sato

Resonance energy of the K-bar NN - π YN system

doi: 10.1103/PhysRevC.79.035201
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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
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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
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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
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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
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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
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2009SU02      Phys.Rev. C 79, 025205 (2009)

N.Suzuki, T.Sato, T.-S.H.Lee

Extraction of resonances from meson-nucleon reactions

doi: 10.1103/PhysRevC.79.025205
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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
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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
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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
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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


2007IK01      Phys.Rev. C 76, 035203 (2007)

Y.Ikeda, T.Sato

Strange dibaryon resonance in the K-bar nn-π YN system

doi: 10.1103/PhysRevC.76.035203
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2079.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2114.


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
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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
Citations: PlumX Metrics


2006KI08      Prog.Theor.Phys.(Kyoto) 116, 241 (2006)

T.Kishimoto, T.Sato

Θ+: Another Explanation and Prediction

doi: 10.1143/PTP.116.241
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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
Citations: PlumX Metrics


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
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2005MA63      Phys.Rev. C 72, 025204 (2005)

K.Matsui, T.Sato, T.-S.H.Lee

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
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2005SA32      Nucl.Phys. B(Proc.Supp.) S149, 221 (2005)

T.Sato

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
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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
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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
Citations: PlumX Metrics


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
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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
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2003SA18      Phys.Rev. C 67, 065201 (2003)

T.Sato, D.Uno, T.-S.H.Lee

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13851.


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
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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
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2001LE14      Nucl.Phys. A684, 327c (2001)

T.-S.H.Lee, T.Sato

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
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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
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2001SA12      Nucl.Phys. A684, 26c (2001)

T.Sato

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
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2001SA17      Phys.Rev. C63, 055201 (2001)

T.Sato, T.-S.H.Lee

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
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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
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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
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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
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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
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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
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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
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1998DM01      Phys.Rev. C58, 1937 (1998)

V.Dmitrasinovic, T.Sato

Partial Conservation of Axial Current Constraints on Pion Production or Absorption within Nonrelativistic Nuclear Dynamics

doi: 10.1103/PhysRevC.58.1937
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1998MA92      Prog.Theor.Phys.(Kyoto) 100, 977 (1998)

H.Masui, T.Sato

Monte-Carlo Study of Bound States in a Few-Nucleon System - Method of Continued Fractions -

doi: 10.1143/PTP.100.977
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1084.


1996SA33      Phys.Rev. C54, 2660 (1996)

T.Sato, T.-S.H.Lee

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
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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
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1995OG06      Prog.Theor.Phys.(Kyoto) 94, 199 (1995)

T.Ogaito, T.Sato, H.Ohtsubo

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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