NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = T.Furumoto Found 39 matches. 2023FU02 Prog.Theor.Exp.Phys. 2023, 063D02 (2023) T.Furumoto, T.Suhara, N.Itagaki Systematic study of the relationship between nuclear structure and reactions for the 10Be nucleus NUCLEAR STRUCTURE 10Be; calculated binding energies, charge and matter radii, B(Eλ). Comparison with available data. NUCLEAR REACTIONS 12C(10Be, 10Be), E=59.4 MeV/nucleon; calculated σ(θ), σ.
doi: 10.1093/ptep/ptad070
2021FU07 Phys.Rev. C 103, 044602 (2021) Relation between transition density and proton inelastic scattering by 12C target at Ep = 65 and 200 MeV NUCLEAR REACTIONS 12C(polarized p, p), (polarized p, p'), E=65, 200 MeV; analyzed experimental data for σ(Ε, θ) and analyzing power Ay(E, θ) for ground state and Hoyle state using microscopic coupled channel (MCC) method with potentials from folding a complex G-matrix effective nucleon-nucleon interaction, and transition density from modified Algebraic Cluster Model (ACM) wave function.
doi: 10.1103/PhysRevC.103.044602
2021FU15 Phys.Rev. C 104, 034613 (2021) T.Furumoto, T.Suhara, N.Itagaki Drastic change of inelastic scattering dependent on the development of dineutron correlations in 10Be NUCLEAR STRUCTURE 10Be; calculated binding energy, energies, B(E2), transition densities, and rms nucleon matter, point neutron and point proton radii for the ground state, and the first 2+ states using four-body (α+α+n+n) microscopic cluster model, and compared with experimental data. NUCLEAR REACTIONS 1H(10Be, p), (10Be, p')E=59.4, 200 MeV/nucleon; calculated differential σ(θ, E) using microscopic structure and reaction models, with parameters for 10Be used from structure calculations. Comparison with experimental data. Relevance to dineutron cluster structure based on its sensitivity to the inelastic cross section to the second 2+ state in 10Be.
doi: 10.1103/PhysRevC.104.034613
2021HO09 Nucl.Phys. A1011, 122204 (2021) Separating isoscalar and isovector dipole excitations in 6Li and 6He using heavy-ion collisions and nuclear-Coulomb interference effects NUCLEAR REACTIONS C, Pb(6Li, 6Li'), (6He, 6He'), E=100-400 MeV/nucleon; calculated σ(E), dipole excitations. 6Li, 6He; deduced the possibility of separating the dipole excitation σ into the IS and IV contributions using heavy-ion collisions.
doi: 10.1016/j.nuclphysa.2021.122204
2020GO06 Phys.Rev. C 102, 014323 (2020) A.Gottardo, G.de Angelis, P.Doornenbal, L.Coraggio, A.Gargano, N.Itaco, K.Kaneko, P.Van Isacker, T.Furumoto, G.Benzoni, J.Lee, H.Liu, M.Matsushita, D.Mengoni, V.Modamio-Hoybjor, S.Momiyama, T.Motobayashi, D.R.Napoli, M.Niikura, E.Sahin, Y.Shiga, H.Sakurai, R.Taniuchi, S.Takeuchi, H.Wang, J.J.Valiente-Dobon, R.Avigo, H.Baba, N.Blasi, F.L.Bello Garrote, F.Browne, F.C.L.Crespi, S.Ceruti, R.Daido, M.-C.Delattre, D.Fang, Zs.Dombradi, T.Isobe, I.Kuti, G.Lorusso, K.Matsui, B.Melon, T.Miyazaki, S.Nishimura, R.Orlandi, Z.Patel, S.Rice, L.Sinclair, P.A.Soderstrom, D.Sohler, T.Sumikama, J.Taprogge, Zs.Vajta, H.Watanabe, O.Wieland, J.Wu, Z.Y.Xu, M.Yalcinkaya, R.Yokoyama Transition strengths in the neutron-rich 73, 74, 75Ni isotopes NUCLEAR REACTIONS Pb(73Ni, 73Ni'), (74Ni, 74Ni'), (75Ni, 75Ni'), E=215 MeV/nucleon, [secondary cocktail beam from 9Be(238U, F), E=345 MeV/nucleon, and separated by A/Q using the BigRIPS fragment separator at RIBF-RIKEN facility]; measured reaction products identified by the ZeroDegree spectrometer, Eγ, Iγ, (scattered Ni nuclei)γ-coin using the WAS3Abi-EURICA setup with the DALI2 NaI(Tl) array for γ detection. 73,74,75Ni; deduced levels, J, π, B(E2) from Coulomb excitation cross sections. Comparison with large-scale shell model calculations.
doi: 10.1103/PhysRevC.102.014323
2019FU03 Phys.Rev. C 99, 034605 (2019) T.Furumoto, K.Tsubakihara, S.Ebata, W.Horiuchi Microscopic global optical potential for nucleon-nucleus systems in the energy range 50-400 MeV NUCLEAR STRUCTURE Z=10, A=17-34; Z=20, A=34-60; Z=40, A=80-120; Z=50, A=100-150; Z=70, A=150-210; Z=82, A=180-245; calculated charge radii using relativistic mean field (RMF) and Hartree-Fock (HF)+BCS densities, and compared with available experimental values. 32,36,40,44,48S, 80,90,100,110Sn; calculated point-neutron, proton, and matter density distributions using RMF and HF+BCS models. NUCLEAR REACTIONS 10C, 276U(n, X), E=50 MeV; 12C, 242U(p, X), E=400 MeV; calculated real and imaginary parts of central and spin-orbit components of the SF potentials using the HF+BCS densities. 12C, 40Ca, 56Fe, 90Zr, 208Pb(p, X), E=50-400 MeV; calculated total reaction σ(E) using the RMF and HF+BCS densities to construct the SF potential. 12C, 16O, 24Mg, 28Si, 40Ca, 48,50Ti, 52Cr, 56Fe, 58Ni, 64,68Zn, 90Zr, 98Mo, 106Pd, 114Cd, 120Sn, 142Nd, 158Gd, 164Dy, 180Hf, 184W, 194Pt, 208Pb, 238U(p, X), E=60, 65.5, 99 MeV; 12C, 40Ca, 56Fe, 90Zr, 114Cd, 184W, 208Pb, 238U(n, X), E=50-400 MeV; Ni(p, X), E=60 MeV for A=50-80 Ni nuclei; Sn(p, X), E=65.5 MeV for A=100-150 Sn nuclei; 12C, 16O, 28Si, 40Ca, 56Fe, 58Ni, 64Zn, 90Zr, 114Cd, 120Sn, 208Pb, 238U(n, X), E=50, 379 MeV; analyzed total reaction σ(E) using microscopic global optical potential (MGOP1 and MGOP2) models. 12C, 40Ca, 208Pb(n, n), E=65-225; 28Si, 56Fe, 90Zr(n, n), E=55, 65, 75 MeV; 16O, 40Ca, 56Fe, Cd, 120Sn(n, n), E=65-351.5 MeV; 238U(n, n), E=52.5-120 MeV; analyzed σ(E, θ). 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 40Ar, 40,42,44,48Ca, 46,48,50Ti, 50,52,54Cr, 54,56Fe, 58,60,62,64Ni, 90Zr, 98,100Mo, 144,148,150,152,154Sm, 160Gd, 164Dy, 166,168Er, 172,174,176Yb, 178,180Hf, 182,184W, 192Os, 208Pb, 232Th, 238U(p, p), (polarized p, p), E=65 MeV; 12C(p, p), (polarized p, p), E=51.93-340 MeV; 16O(p, p), (polarized p, p), E=61-317.4 MeV; 24Mg, 28,30Si, 32,34S, 40,48Ca(p, p), (polarized p, p), E=51.9-400 MeV; 46,48,50Ti, 50Cr, 54,56Fe, 58,60,62Ni, 66,68Zn, 74,76,78,80,82Se(p, p), (polarized p, p), E=51.9-333 MeV; 88Sr, 90,92Zr(p, p), (polarized p, p), E=57.5-200 MeV; 106,108,110Pd, 112Cd, 116Sn(p, p), E=51-61.4 MeV; 116,118,120,122,124Sn(p, p), (polarized p, p), E=61.5-300 MeV; 148,154Sm, 192Os, 194,198Pt, 204,206,208Pb(p, p), (polarized p, p), E=61.4-400 MeV; 22,24O, 56Ni(p, p), E=46.6-285 MeV; 48S(p, p), E=100-400 MeV; 100,110Zr(p, p), (polarized p, p), E=100-400 MeV; analyzed σ(θ, E), analyzing powers Ay(θ, E), and spin-rotation functions; deduced microscopic global optical potential (MGOP) for nucleon-nucleus systems in a wide range of nuclear mass numbers (A=10-276) and incident energies of 50-400 MeV. Microscopic global optical potential (MGOP1 and MGOP2) models, based on a single-folding (SF) model with the complex G-matrix interaction, with nuclear densities generated from mean-field calculations using relativistic-mean-field (RMF) and Skyrme-Hartree-Fock+BCS approaches.
doi: 10.1103/PhysRevC.99.034605
2019SA48 Prog.Theor.Exp.Phys. 109, 101D01 (2019) K.Sato, T.Furumoto, Y.Kikuchi, K.Ogata, Y.Sakuragi Large-amplitude quadrupole shape mixing probed by the (p, p') reaction: A model analysis NUCLEAR REACTIONS 154Sm(p, p'), E=35, 65, 66.5 MeV; calculated σ(θ). Comparison with experimental results.
doi: 10.1093/ptep/ptz095
2019VA03 Phys.Rev. C 99, 034306 (2019) V.Vaquero, A.Jungclaus, P.Doornenbal, K.Wimmer, A.M.Moro, K.Ogata, T.Furumoto, S.Chen, E.Nacher, E.Sahin, Y.Shiga, D.Steppenbeck, R.Taniuchi, Z.Y.Xu, T.Ando, H.Baba, F.L.Bello Garrote, S.Franchoo, K.Hadynska-Klek, A.Kusoglu, J.Liu, T.Lokotko, S.Momiyama, T.Motobayashi, S.Nagamine, N.Nakatsuka, M.Niikura, R.Orlandi, T.Y.Saito, H.Sakurai, P.A.Soderstrom, G.M.Tveten, Zs.Vajta, M.Yalcinkaya In-beam γ-ray spectroscopy of 136Te at relativistic energies NUCLEAR REACTIONS C, 197Au(136Te, 136Te'), C(137Te, 136Te), E=139, 140 MeV/nucleon, [secondary 136,137Te beam from 9Be(238U, F), E=345 MeV/nucleon primary reaction]; measured Eγ, Iγ, γγ-coin, σ(θ), exclusive σ following Coulomb excitation to individual excited states using the DALI2 spectrometer array for γ detection, and the BigRIPS and ZeroDegree spectrometers for beam and product identification, respectively at RIBF-RIKEN facility. 136Te; deduced levels, J, π, B(E2) values. Comparison with theoretical predictions, and with previous experimental results. Systematics of B(E2) values for the first 2+ states in 132,134,136Te.
doi: 10.1103/PhysRevC.99.034306
2018FU10 Phys.Rev. C 97, 044602 (2018) T.Furumoto, T.Suhara, N.Itagaki Effect of channel coupling on the elastic scattering of lithium isotopes NUCLEAR STRUCTURE 6,7,8,9Li; calculated levels, J, π, rms radii of the charged proton, point proton, point neutron, and point matter for ground states, transition strengths from the ground states to the excited states. Stochastic multi-configuration mixing method based on the microscopic-cluster model (MCM). Comparison with experimental data. NUCLEAR REACTIONS 12C, 28Si(6Li, 6Li), (7Li, 7Li), (8Li, 8Li), (9Li, 9Li), E=53 MeV/nucleon; 12C, 28Si(7Li, 7Li), E=50 MeV/nucleon; 12C(9Li, 9Li), E=59.4, 60 MeV/nucleon; 12C(10Be, 10Be), E=59.4 MeV/nucleon; calculated differential σ(θ) using microscopic coupled-channel (MCC) method with complex G-matrix interaction. Comparison with experimental results.
doi: 10.1103/PhysRevC.97.044602
2017QU02 Phys.Rev. C 95, 044616 (2017) W.W.Qu, G.L.Zhang, S.Terashima, T.Furumoto, Y.Ayyad, Z.Q.Chen, C.L.Guo, A.Inoue, X.Y.Le, H.J.Ong, D.Y.Pang, H.Sakaguchi, Y.Sakuragi, B.H.Sun, A.Tamii, I.Tanihata, T.F.Wang, R.Wada, Y.Yamamoto Repulsive three-body force and channel-coupling effects via 12C+12C scattering at 100A MeV NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=100 MeV/nucleon; measured scattered 12C using Grand Raiden high-resolution magnetic spectrometer, and 10B, 11C and other particles by the energy loss and time-of-flight (TOF) information, differential cross sections for the ground state, 4.44 MeV, 2+ state, and the sum of the 7.65 MeV, 0+ and the 9.64 MeV, 3- states in 12C using the Ring Cyclotron facility at RCNP-Osaka. Comparison with microscopic coupled-channel calculations, using the double folding method with three different complex G-matrix interactions, the ESC, CEG07b, and MPa.
doi: 10.1103/PhysRevC.95.044616
2017YA29 Phys.Rev. C 96, 065804 (2017) Y.Yamamoto, H.Togashi, T.Tamagawa, T.Furumoto, N.Yasutake, Th.A.Rijken Neutron-star radii based on realistic nuclear interactions
doi: 10.1103/PhysRevC.96.065804
2016FU01 Acta Phys.Pol. B47, 853 (2016) T.Furumoto, Y.Sakuragi, Y.Yamamoto Approach to High-density Nuclear Matter via Nucleus-Nucleus Elastic Scattering NUCLEAR REACTIONS 16O(16O, 16O), E=70 MeV/nucleon; analyzed available data; calculated σ.
doi: 10.5506/APhysPolB.47.853
2016FU13 Phys.Rev. C 94, 044620 (2016) T.Furumoto, Y.Sakuragi, Y.Yamamoto Medium effect in high-density nuclear matter probed by a systematic analysis of nucleus-nucleus elastic scattering NUCLEAR REACTIONS 16O(16O, 16O), (16O, X), E=70 MeV/nucleon; calculated real and imaginary parts of the double-folding (DF) potential, σ(θ) for elastic scattering and total reaction σ using different interactions. 12C, 28Si, 40Ca, 90Zr, 208Pb(16O, 16O), E=93.9 MeV/nucleon; 12C(12C, 12C), E=84.7, 100, 120.75, 135, 200, 300, 400 MeV; calculated σ(θ). Double-folding (DF) potential with the complex G-matrix interaction including three-body-force (TBF) effect based on multi-Pomeron exchange potential (MPP) model. Comparison with experimental data.
doi: 10.1103/PhysRevC.94.044620
2016YA01 Eur.Phys.J. A 52, 19 (2016) Y.Yamamoto, T.Furumoto, N.Yasutake, Th.A.Rijken Hyperon-mixed neutron star with universal many-body repulsion NUCLEAR REACTIONS 16O(16O, 16O), E=70 MeV/nucleon; calculated σ(θ) using G-matrix folding potentials.
doi: 10.1140/epja/i2016-16019-0
2015MO04 Phys.Rev. C 91, 024916 (2015) K.Morita, T.Furumoto, A.Ohnishi ΛΛ interaction from relativistic heavy-ion collisions
doi: 10.1103/PhysRevC.91.024916
2015QU02 Phys.Lett. B 751, 1 (2015) W.W.Qu, G.L.Zhang, S.Terashima, T.Furumoto, Y.Ayyad, Z.Q.Chen, C.L.Guo, A.Inoue, X.Y.Le, H.J.Ong, D.Y.Pang, H.Sakaguchi, Y.Sakuragi, B.H.Sun, A.Tamii, I.Tanihata, T.F.Wang, R.Wada, Y.Yamamoto Effects of repulsive three-body force in 12C + 12C scattering at 100A MeV NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=100 MeV/nucleon; measured reaction products; deduced σ(θ). Three double-folding models with complex G-matrix interactions, the CEG07b, MPa, and ESC model calculations.
doi: 10.1016/j.physletb.2015.10.008
2014DO19 Phys.Rev. C 90, 061302 (2014) P.Doornenbal, S.Takeuchi, N.Aoi, M.Matsushita, A.Obertelli, D.Steppenbeck, H.Wang, L.Audirac, H.Baba, P.Bednarczyk, S.Boissinot, M.Ciemala, A.Corsi, T.Furumoto, T.Isobe, A.Jungclaus, V.Lapoux, J.Lee, K.Matsui, T.Motobayashi, D.Nishimura, S.Ota, E.C.Pollacco, H.Sakurai, C.Santamaria, Y.Shiga, D.Sohler, R.Taniuchi Intermediate-energy Coulomb excitation of 104Sn: Moderate E2 strength decrease approaching 100Sn NUCLEAR REACTIONS C, Pb(104Sn, 104Sn'), E=131 MeV/nucleon; C, Pb(112Sn, 112Sn'), E=154 MeV/nucleon, [secondary 104,112Sn beams from 9Be(124Xe, X), E=345 MeV/nucleon primary reaction]; measured Eγ, Iγ, scattered 104,112Sn spectra, σ(θ) for particles, inelastic cross sections for population of first 2+ states through intermediate-energy Coulomb excitation using DALI2 array for γ rays, BigRIPS and ZeroDegree spectrometers for reaction products at RIKEN facility. 104Sn; deduced levels, J, π, B(E2) for first 2+ state relative to that for 112Sn. Comparison with shell-model calculations, and with previous experimental results. Systematics of experimental and theoretical B(E2) values for first 2+ states in A=104-130 even-A Sn isotopes.
doi: 10.1103/PhysRevC.90.061302
2014FU09 Phys.Rev. C 90, 041601 (2014) T.Furumoto, Y.Sakuragi, Y.Yamamoto Medium effect in the high-density region probed by nucleus-nucleus elastic scattering NUCLEAR REACTIONS 16O(16O, 16O), E=70 MeV/nucleon; calculated double-folding potential dependency on density, elastic σ(θ) using double-folding model with the complex G-matrix interaction and three-body-force (TBF) effect. Investigated medium effect dependency on density. Comparison with experimental results.
doi: 10.1103/PhysRevC.90.041601
2014YA26 Phys.Rev. C 90, 045805 (2014) Y.Yamamoto, T.Furumoto, N.Yasutake, Th.A.Rijken Hyperon mixing and universal many-body repulsion in neutron stars NUCLEAR REACTIONS 16O(16O, 16O), E=70 MeV/nucleon; analyzed differential elastic σ(θ) data with the G-matrix folding potentials; deduced multi-Pomeron exchange potential (MPPs) and used as input to hyperon mixing in neutron stars. NUCLEAR STRUCTURE 13C, 28Si, 51V, 89Y, 139La, 208Pb; calculated energy spectra of hypernuclei using MPPs deduced from analysis of 16O(16O, 16O) reaction, composition of hyperonic neutron-star matter in the case of extended soft core (ESC) baryon-baryon interaction, equation of state (EoS) in neutron matter with hyperon mixing; derived mass-radius relations of neutron stars. Comparison with experimental data for energy spectra of hypernuclei.
doi: 10.1103/PhysRevC.90.045805
2013FU01 Phys.Rev. C 87, 014618 (2013) Channel coupling effect and important role of imaginary part of coupling potential for high-energy heavy-ion scatterings NUCLEAR REACTIONS 12C(12C, X), (12C, 12C), E=100-400 MeV/nucleon, calculated folding potential, coupling potential, elastic σ(E), dynamical polarization potential, inelastic σ(E). Microscopic coupled channel (MCC) method using the complex G-matrix interaction CEG07.
doi: 10.1103/PhysRevC.87.014618
2013FU07 Phys.Rev. C 87, 064320 (2013); Erratum Phys.Rev. C 90, 039902 (2014) T.Furumoto, T.Suhara, N.Itagaki Investigation of the 3/22- state of 9Li with microscopic structure and reaction models NUCLEAR STRUCTURE 9Li; calculated total energies of 1/2-, 3/2-, 5/2- and 7/2- states, low-lying negative-parity levels, J, proton, neutron, and matter radii of ground state, quadrupole moments of ground state and first 3/2-, B(E2) and B(E0) transition strengths between low-lying negative-parity states. Unified framework of microscopic α+t+n+n cluster structure and reaction models. Possibility of triaxial deformation and mixing of dineutron components in 9Li nucleus. Comparison with experimental data. NUCLEAR REACTIONS 12C(9Li, 9Li), (9Li, 9Li'), E=50, 60 MeV/nucleon; calculated quasielastic, elastic and inelastic σ(θ) for ground state and 3/2- states using wave functions from multiconfiguration mixing method, and reaction analysis by microscopic coupled channel (MCC) method. Multistep effects. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.064320
2013OG06 Phys.Rev. C 88, 024616 (2013) K.Ogata, T.Myo, T.Furumoto, T.Matsumoto, M.Yahiro Interplay between the 02+ resonance and the nonresonant continuum of the drip-line two-neutron halo nucleus 22C NUCLEAR REACTIONS 12C(22C, X), E=250 MeV/nucleon; calculated double differential breakup cross section, breakup energy distribution for low-lying resonances and non-resonant continuum. Four-body continuum-discretized coupled-channels (CCDC) method with the cluster-orbital shell model (COSM) wave functions.
doi: 10.1103/PhysRevC.88.024616
2013OH07 Nucl.Phys. A914, 367c (2013) A.Ohnishi, S.Cho, T.Furumoto, T.Hyodo, D.Jido, C.M.Ko, K.Morita, S.H.Lee, M.Nielsen, T.Sekihara, S.Yasui, K.Yazaki, for the ExHIC Collaboration Exotic hadrons and hadron-hadron interactions in heavy-ion collisions
doi: 10.1016/j.nuclphysa.2013.01.083
2013YA15 Phys.Rev. C 88, 022801 (2013) Y.Yamamoto, T.Furumoto, N.Yasutake, Th.A.Rijken Multi-Pomeron repulsion and the neutron-star mass NUCLEAR REACTIONS 16O(16O, 16O), E=70 MeV/nucleon; analyzed σ(θ) data using G-matrix folding potential derived from extended soft core (ESC) model with three-nucleon interaction (TNA) and multi-Pomeron exchange potential (MPP); deduced fitting parameters for the neutron matter equation of state (EoS); calculated neutron-star mass by solving the Tolmann-Oppenheimer-Volkof equation.
doi: 10.1103/PhysRevC.88.022801
2012FU04 Phys.Rev. C 85, 044607 (2012); Erratum Phys.Rev. C 85, 069901 (2012) T.Furumoto, W.Horiuchi, M.Takashina, Y.Yamamoto, Y.Sakuragi Global optical potential for nucleus-nucleus systems from 50 MeV/u to 400 MeV/u NUCLEAR REACTIONS 16O(16O, 16O), E=21.9, 30, 44, 70 MeV/nucleon; 12C(16O, 16O), E=20.6, 38, 93.9 MeV/nucleon; 12C(12C, 12C), E=25, 30, 84.7, 120.75, 135, 200 MeV/nucleon; 28Si, 40Ca, 208Pb(16O, 16O), E=93.9 MeV/nucleon; 60Ni, 120Sn, 208Pb(40Ar, 40Ar), E=44 MeV/nucleon; 40Ca(14C, 14C), (16C, 16C), (18C, 18C), (20C, 20C), (22C, 22C)(18O, 18O), (20O, 20O), (22O, 22O), (24O, 24O), E=100 MeV/nucleon; 40Ca(30Ne, 30Ne), (70Ca, 70Ca), E=100, 200, 300, 400 MeV/nucleon; calculated folding-model potentials (FMPs) elastic scattering cross sections as a function of momentum transfer. New global optical potential (GOP) in 50-400 MeV/nucleon range from microscopic CEG07 folding model with Sao Paulo density. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.044607
2012FU09 Prog.Theor.Phys.(Kyoto), Suppl. 196, 219 (2012) T.Furumoto, Y.Sakuragi, Y.Yamamoto Dynamical Evolution of Heavy-Ion Scattering in the High-Energy Region NUCLEAR REACTIONS 12C(12C, 12C), E=100, 200, 300, 400 MeV; calculated Rutherford ratio of elastic σ, σ(θ); deduced dynamical polarization potential.
doi: 10.1143/PTPS.196.219
2012FU13 J.Phys.:Conf.Ser. 381, 012092 (2012) T.Furumoto, Y.Sakuragi, Y.Yamamoto Prediction of repulsive potential for high-energy heavy-ion scatterings NUCLEAR REACTIONS 12C(12C, 12C), E=100, 200, 300, 400 MeV/nucleon; calculated σ(q) and its decomposition into near- and far-side using DFM (double-folding model) potentials with G-matrix NN interactions CEG07.
doi: 10.1088/1742-6596/381/1/012092
2011CH63 Phys.Rev. C 84, 064910 (2011) S.Cho, T.Furumoto, T.Hyodo, D.Jido, C.M.Ko, S.H.Lee, M.Nielsen, A.Ohnishi, T.Sekihara, S.Yasui, K.Yazaki Exotic hadrons in heavy ion collisions
doi: 10.1103/PhysRevC.84.064910
2011FU16 J.Phys.:Conf.Ser. 312, 082022 (2011) T.Furumoto, Y.Sakuragi, Y.Yamamoto Role of Three-Body Forces in Proton and Heavy-Ion Scatterings NUCLEAR REACTIONS 12C(p, p), E=122 MeV; calculated σ(θ), analyzing power. 12C, 28Si, 40Ca(16O, 16O), E=93.9 MeV/nucleon;16O(16O, 16O), E=70 MeV/nucleon;12C(12C, 12C), E=135 MeV/nucleon; calculated σ(θ). Complex G-matrix CEG-07 with three-body forces. Compared with data.
doi: 10.1088/1742-6596/312/4/082022
2011MU16 Phys.Rev. C 84, 034305 (2011) K.Muta, T.Furumoto, T.Ichikawa, N.Itagaki Three-triton states in 9Li NUCLEAR STRUCTURE 9Li; calculated rms radii and energy convergence of 3/2- 3/2+, 1/2- and 1/2+ states, E0 transition strength; deduced α+t+n+n, t+t+t configurations in excited states of 9Li.
doi: 10.1103/PhysRevC.84.034305
2010FU12 Phys.Rev. C 82, 044612 (2010) T.Furumoto, Y.Sakuragi, Y.Yamamoto Repulsive nature of optical potentials for high-energy heavy-ion scattering NUCLEAR REACTIONS 12C(12C, 12C), 16O(16O, 16O), E=100, 200, 300, 400 MeV/nucleon; calculated differential σ, σ(θ), and potential energies using double-folding model (DFM) with complex G-matrix interaction.
doi: 10.1103/PhysRevC.82.044612
2010FU14 Nucl.Phys. A835, 362c (2010) T.Furumoto, Y.Sakuragi, Y.Yamamoto Hyperon-nucleus folding potentials in the complex G-matrix approach NUCLEAR REACTIONS 28Si(Σ0, Σ0), E=50-200 MeV; calculated σ(θ), analyzing power using G-matrix models ESC08 (Extended Soft-Core Model) and ESC04a.
doi: 10.1016/j.nuclphysa.2010.01.219
2010HO08 Phys.Rev. C 81, 061602 (2010) K.Horii, M.Takashina, T.Furumoto, Y.Sakuragi, H.Toki Elastic scattering of 8B from 12C with internal three-cluster structure of 8B NUCLEAR REACTIONS 12C(8B, 8B), E=95 MeV; calculated σ, σ(θ) using adiabatic recoil and cluster folding calculations. 12C, 14N(7Be, 7Be), E=87 MeV; calculated σ(θ). Comparison with experimental data.
doi: 10.1103/PhysRevC.81.061602
2010TA06 Phys.Rev. C 81, 047605 (2010) M.Takashina, T.Furumoto, Y.Sakuragi 16O+16O inelastic scattering studied by a complex G-matrix interaction NUCLEAR REACTIONS 16O(16O, 16O'), E=1120 MeV; analyzed σ(θ) using microscopic coupled-channel (CC) method with complex G-matrix interaction.
doi: 10.1103/PhysRevC.81.047605
2009EL03 Phys.Rev. C 79, 011302 (2009) Z.Elekes, Zs.Dombradi, T.Aiba, N.Aoi, H.Baba, D.Bemmerer, B.A.Brown, T.Furumoto, Zs.Fulop, N.Iwasa, A.Kiss, T.Kobayashi, Y.Kondo, T.Motobayashi, T.Nakabayashi, T.Nannichi, Y.Sakuragi, H.Sakurai, D.Sohler, M.Takashina, S.Takeuchi, K.Tanaka, Y.Togano, K.Yamada, M.Yamaguchi, K.Yoneda Persistent decoupling of valence neutrons toward the dripline: Study of 20C by γ spectroscopy NUCLEAR REACTIONS 208Pb(20C, 20C'), E=37.6 MeV/nucleon; 1H(20C, 20C'), E=41.4 MeV/nucleon; measured Eγ, Iγ. 20C; deduced levels, J, π, charge and neutron transition probabilities, B(E2). Comparison with shell model calculations.
doi: 10.1103/PhysRevC.79.011302
2009FU01 Phys.Rev. C 79, 011601 (2009) T.Furumoto, Y.Sakuragi, Y.Yamamoto Three-body-force effect on nucleus-nucleus elastic scattering NUCLEAR REACTIONS 16O(16O, 16O), E=70 MeV/nucleon; calculated σ(θ). Three-body force. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.011601
2009FU11 Phys.Rev. C 80, 044614 (2009); Erratum Phys.Rev. C 82, 029908 (2010) T.Furumoto, Y.Sakuragi, Y.Yamamoto Effect of repulsive and attractive three-body forces on nucleus-nucleus elastic scattering NUCLEAR REACTIONS 16O(16O, 16O), E=21.875, 70, 100, 200, 300, 400 MeV/nucleon; 12C, 28Si, 40Ca(16O, 16O), E=93.9 MeV/nucleon; 12C(12C, 12C), E=135 MeV/nucleon; calculated σ, σ(θ), folding model potentials, and rms radii using Brueckner theory for nucleon-nucleon effective interaction in complex G-matrix formalism. Investigated the effects of the three-body force (TBF) in nucleon-nucleus elastic scattering.
doi: 10.1103/PhysRevC.80.044614
2008FU13 Phys.Rev. C 78, 044610 (2008) T.Furumoto, Y.Sakuragi, Y.Yamamoto New complex G-matrix interactions derived from two- and three-body forces and application to proton-nucleus elastic scattering NUCLEAR REACTIONS 12C, 40Ca, 90Zr, 208Pb(p, p), E=65-200 MeV; calculated σ, σ(θ), analyzing powers, neutron densities. Complex G-matrix interactions with three-body force.
doi: 10.1103/PhysRevC.78.044610
2006FU11 Phys.Rev. C 74, 034606 (2006) Application of the Jeukenne-Lejeune-Mahaux folding model to α-nucleus elastic scattering NUCLEAR REACTIONS 12C, 16O, 28Si, 40Ca(α, α), E ≈ 40-240 MeV; calculated σ(θ). Folding model, comparison with data.
doi: 10.1103/PhysRevC.74.034606
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