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NSR database version of July 31, 2015.

Search: Author = T.Sato

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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


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


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. 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
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


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
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


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
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


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)

Y.Ikeda, H.Kamano, T.Sato

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)

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


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


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
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


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)

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

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
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


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
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
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


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)

T.Kishimoto, T.Sato

Θ+: Another Explanation and Prediction


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)

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


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


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)

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


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.

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


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)

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


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)

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


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


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.


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


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 -


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.

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


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)

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.


1994KO32     Nucl.Instrum.Methods Phys.Res. A337, 355 (1994)

M.Kobayashi, T.Shinkawa, T.Sato, S.Sugimoto, M.V.Korzhik, A.A.Fyodorov, V.A.Kachanov

YAlO3: Ce-Am light pulsers as a gain monitor for undoped CsI detectors in a magnetic field

doi: 10.1016/0168-9002(94)91103-7


1994SA02     Phys.Rev. C49, 776 (1994)

T.Sato, N.Odagawa, H.Ohtsubo, T.-S.H.Lee

Nuclear Structure Studies with (e, e'), (π, π'), and (γ, π) Reactions: Application to 10B

NUCLEAR REACTIONS 10B(e, e'), E not given; calculated charge, transverse form factors. 10B(π, π'), E=164 MeV; 10B(γ, π+), E=183, 320 MeV; calculated σ(θ).

doi: 10.1103/PhysRevC.49.776


1994SA44     Nucl.Phys. A577, 219c (1994)

T.Sato, N.Odagawa, H.Ohtsubo, T.-S.H.Lee

Nuclear Structure of 10B Studied with (e, e'), (π, π') and (γ, π) Reactions

NUCLEAR REACTIONS 10B(e, e'), E not given; 10B(π, π'), E=164 MeV; 10B(γ, π), E=183, 220 MeV; analyzed data. Different models.

doi: 10.1016/0375-9474(94)90859-1


1993MO30     Hyperfine Interactions 78, 85 (1993)

M.Morita, R.Morita, M.Doi, T.Sato, H.Ohtsubo, K.Koshigiri

Induced Pseudoscalar Interaction in Weak Nucleon Current and Muon Capture in Hyperfine States of Muonic Deuterium

ATOMIC PHYSICS, Mesic-Atoms 2H; calculated muon capture rate in muonic deuterium.

doi: 10.1007/BF00568120


1993OH02     Phys.Rev. D47, 4840 (1993)

T.Ohshima, H.Sakamoto, T.Sato, J.Shirai, T.Tsukamoto, Y.Sugaya, K.Takahashi, T.Suzuki, C.Rosenfeld, S.Wilson, K.Ueno, Y.Yonezawa, H.Kawakami, S.Kato, S.Shibata, K.Ukai

No 17 keV Neutrino: Admixture < 0.073% (95% C.L.)

RADIOACTIVITY 63Ni(β-); measured β-spectra; deduced 17 keV ν admixing with ν(e) upper limit. High confidence limit, magnetic spectrometer.

doi: 10.1103/PhysRevD.47.4840


1993SA15     Z.Phys. A345, 15 (1993)

T.Sato, T.Ogaito, H.Ohtsubo

Application of Semi-Classical Method to the Polarization Problem of Hypernuclei

NUCLEAR REACTIONS 12C(K-, π-), E at 715 MeV/c; 12C(π+, K+), E at 1056 MeV/c; calculated hypernuclei polarization vs θ. Semi-classical approximation to transition amplitude.


1993SA29     Nucl.Phys. A562, 673 (1993)

T.Sato, T.Takaki

Delta-Hole Approach to (γ, π-p) Reaction at Resonance Energy

NUCLEAR REACTIONS 16O(γ, π-p), E=360 MeV; calculated out of plane σ(θp, θπ). Delta-hole approach.

doi: 10.1016/0375-9474(93)90135-K


1993SA39     J.Radioanal.Nucl.Chem. 170, 367 (1993)

T.Sato, T.Suzuki

Formation Cross Section of Iron-60 with Reactor Neutrons in 59Fe(n, γ)60Fe Reaction

NUCLEAR REACTIONS 59Fe(n, γ), E=reactor; measured Eγ, Iγ; deduced reaction σ. Ingrowth of 60Co radioactivity in an Fe sample.


1993SA45     J.Radioanal.Nucl.Chem. 173, 107 (1993)

T.Sato, M.Katada, K.Endo, M.Nakada, H.Sano

Emission Mossbauer Spectroscopic Studies of Mixed-Valence States of 57Fe Atoms Produced in 57Co-Labeled Trinuclear Cobalt-Iron Carboxylates

NUCLEAR REACTIONS 57Fe(γ, γ), E=14.4 keV; measured Mossbauer spectra; deduced mixed valence state temperature dependence. Target atoms from 57Co((EC)-decay) labled in trinuclear Co-Fe carboxylates.


1992KA29     Phys.Lett. 287B, 45 (1992)

H.Kawakami, S.Kato, T.Ohshima, C.Rosenfeld, H.Sakamoto, T.Sato, S.Shibata, J.Shirai, Y.Sugaya, T.Suzuki, K.Takahashi, T.Tsukamoto, K.Ueno, K.Ukai, S.Wilson, Y.Yonezawa

High Sensitivity Search for a 17 keV Neutrino. Negative Indication with an Upper Limit of 0.095%

RADIOACTIVITY 63Ni(β-); measured β-spectrum near 17 keV ν-threshold; deduced no 17 keV ν indication, admixture upper limit.

doi: 10.1016/0370-2693(92)91874-9


1992TA03     Nucl.Phys. A536, 597 (1992)

K.Tamura, T.Niwa, T.Sato, H.Ohtsubo

Relativistic Effects on Electron Scattering of the Deuteron

NUCLEAR REACTIONS 2H(polarized e, e), E not given; calculated deuteron tensor polarization. 2H(e, e'p), E not given; calculated electrodisintegration σ(E(e'), θ). Relativistic effects.

doi: 10.1016/0375-9474(92)90115-Z


1991FU08     Phys.Lett. 267B, 293 (1991)

S.Fukui, N.Horikawa, S.Inaba, T.Inagaki, Y.Inagaki, Y.Ishizaki, T.Iwata, T.Kinashi, M.Kurashina, I.Maeda, T.Matsuda, K.Mori, T.Nakamura, T.Nakanishi, K.Ohmi, C.Ohmori, T.Sato, K.Takamatsu, R.Takashima, T.Tsuru, Y.Yasu

Study of the Etaπ+π- System in the π-p Charge Exchange Reaction at 8.95 GeV/c

NUCLEAR REACTIONS 1H(π-, X), E at 8.95 GeV/c; measured missing mass, ππ(eta) spectra; deduced eta-state mass value.

doi: 10.1016/0370-2693(91)91263-U


1991OD04     Prog.Theor.Phys.(Kyoto) 86, 1277 (1991)

N.Odagawa, T.Sato, H.Ohtsubo

Charged Pion Photoproduction on the p-Shell Nuclei at Low Energy and Rescattering Effect of a Pion

NUCLEAR REACTIONS 12C(γ, π+), E=194 MeV; 13C(γ, π-), E=163, 190 MeV; 15N(γ, π-), E=170 MeV; calculated σ(θ); deduced rescattering process role dependence on pion charge. DWIA.


1990DO01     Nucl.Phys. A511, 507 (1990)

M.Doi, T.Sato, H.Ohtsubo, M.Morita

Effect of Meson Exchange Current on Deuteron Muon Capture

NUCLEAR REACTIONS 2H(μ-, 2n), E at rest; calculated neutron spectra, ν asymmetry. Meson exchange model, Siegert theorem.

doi: 10.1016/0375-9474(90)90107-W


1989JE06     Phys.Lett. 228B, 304 (1989)

B.K.Jeon, T.Sato, H.Ohtsubo

Coherent π0 Electroproduction on the Deuteron at Threshold

NUCLEAR REACTIONS 2H(e, π0), E not given; calculated pion production longitudinal form factor.

doi: 10.1016/0370-2693(89)91549-9


1987AL13     Phys.Rev. C36, 732 (1987)

C.Alexandrou, T.Sato

Structure of S(*) from Nuclear Production Experiments

NUCLEAR REACTIONS 12C, 16O(K-, X), E= ≤ 2.4 GeV/c; calculated σ.

doi: 10.1103/PhysRevC.36.732


1987FU13     Prog.Theor.Phys.(Kyoto) 78, 343 (1987)

M.Fukui, K.Koshigiri, T.Sato, H.Ohtsubo, M.Morita

Polarizations of 12B in Muon Capture Reaction with Higher Order Configuration Mixing

NUCLEAR REACTIONS 12C(polarized μ-, ν)12B, E not given; calculated 12B polarization; deduced pseudoscalar to axial coupling constant ratio (g(p)/g(A)). 12C(e, e'), E=80-330 MeV; calculated M1 form factor.


1985SA06     Z.Phys. A320, 507 (1985)

T.Sato, K.Koshigiri, H.Ohtsubo

Electron Scattering and Charge Pion Photoproduction on 12C and 13C

NUCLEAR REACTIONS 13,12C(e, e'), E not given; calculated M1, E2 form factors. 12C(γ, π+), E=194 MeV; calculated σ(θ). 13C(γ, π-), E=190 MeV; calculated σ(θ); deduced core polarization, meson exchange effect role. Shell model, effective interactions.


1983FU15     Phys.Lett. 132B, 255 (1983)

M.Fukui, K.Koshigiri, T.Sato, H.Ohtsubo, M.Morita

The Average Polarization of 12B in the Muon Capture Reaction

NUCLEAR REACTIONS 12C(μ-, ν), E at rest; analyzed recoil 12B polarization; deduced (gp/g(A)). Multi-configurational shell model wave functions.

doi: 10.1016/0370-2693(83)90301-5


1983FU17     Prog.Theor.Phys.(Kyoto) 70, 827 (1983)

M.Fukui, K.Koshigiri, T.Sato, H.Ohtsubo, M.Morita

Nuclear Polarization of 12B in Muon Capture Reaction

NUCLEAR REACTIONS 12C(μ-, ν), E at rest; calculated average, longitudinal 12B recoil polarization; deduced (gp/g(A)). Multi-configuration shell model.


1982SA26     Prog.Theor.Phys.(Kyoto) 68, 840 (1982)

T.Sato, M.Kobayashi, H.Ohtsubo

Meson Exchange Current and Magnetic Moment of Deuteron

NUCLEAR STRUCTURE 2H; calculated corrections to μ. Meson exchange, S-matrix method.


1978HY01     Nucl.Phys. A300, 242 (1978)

H.Hyuga, H.Ohtsubo, T.Sato

Two-Pion Exchange Charge Density and its Related Problems

NUCLEAR STRUCTURE 3He, 3H; calculated two-pion exchange charge density operators contribution to charge form factors.

doi: 10.1016/0375-9474(78)96130-4


1975SA21     J.Nucl.Sci.Technol. 12, 19 (1975)

T.Sato, Y.Kanda, I.Kumabe

Activation Cross Sections for (n, p) and (n, α) Reactions on Nd, Sm, Yb And Lu at 14.6 MeV

NUCLEAR REACTIONS 150Sm, 173Yb, 175Lu(n, p), 146Nd, 152Sm, 174Yb, 176Lu(n, α), E=14.6 MeV; measured activation σ. Ge(Li) detector, pre-equilibrium model.


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