NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = K.Harada Found 31 matches. 2016HA25 Phys.Rev. C 94, 024004 (2016) Numerical study of renormalization group flows of nuclear effective field theory without pions on a lattice
doi: 10.1103/PhysRevC.94.024004
2014IT01 Phys.Rev.Lett. 113, 102501 (2014) M.Itoh, S.Ando, T.Aoki, H.Arikawa, S.Ezure, K.Harada, T.Hayamizu, T.Inoue, T.Ishikawa, K.Kato, H.Kawamura, Y.Sakemi, A.Uchiyama Further Improvement of the Upper Limit on the Direct 3α Decay from the Hoyle State in 12C NUCLEAR REACTIONS 12C(12C, 3α)12C, E=110 MeV; measured reaction products, Eα, Iα; deduced yields, Dalitz plots, Hoyle state, branching ratios, J, π. Comparison with available data.
doi: 10.1103/PhysRevLett.113.102501
2011HA12 Phys.Rev. C 83, 034002 (2011) Pions are neither perturbative nor nonperturbative: Wilsonian renormalization-group analysis of nuclear effective field theory including pions
doi: 10.1103/PhysRevC.83.034002
2007FU04 Phys.Rev. C 75, 034310 (2007) H.Fujita, Y.Fujita, T.Adachi, A.D.Bacher, G.P.A.Berg, T.Black, E.Caurier, C.C.Foster, H.Fujimura, K.Hara, K.Harada, K.Hatanaka, J.Janecke, J.Kamiya, Y.Kanzaki, K.Katori, T.Kawabata, K.Langanke, G.Martinez-Pinedo, T.Noro, D.A.Roberts, H.Sakaguchi, Y.Shimbara, T.Shinada, E.J.Stephenson, H.Ueno, T.Yamanaka, M.Yoshifuku, M.Yosoi Isospin structure of Jπ = 1+ states in 58Ni and 58Cu studied by 58Ni(p, p') and 58Ni(3He, t)58Cu measurements NUCLEAR REACTIONS 58Ni(p, p'), E=160 MeV; measured Ep, σ(θ=0°). 58Ni(3He, t), E=140 MeV/nucleon; measured triton spectra, σ(θ=0°). 58Ni, 58Cu deduced 1+ level energies, B(GT), isospin symmetry features. Comparison with shell model predictions.
doi: 10.1103/PhysRevC.75.034310
2007HA30 Nucl.Phys. A790, 418c (2007) Power counting for nuclear effective field theory and Wilsonian renormalization group
doi: 10.1016/j.nuclphysa.2007.03.074
2006HA18 Phys.Lett. B 636, 305 (2006) Wilsonian RG and redundant operators in nonrelativistic effective field theory
doi: 10.1016/j.physletb.2006.03.072
2005HA34 Prog.Theor.Phys.(Kyoto) 113, 1315 (2005) K.Harada, Y.Mitsunari, N.Yamashita Effective Theory Approach to the Skyrme Model and Application to Pentaquarks
doi: 10.1143/PTP.113.1315
2003YO12 Mod.Phys.Lett. A 18, 444 (2003) H.Yoshino, K.Harada, M.Matsuda, J.Nagata Phase-shift analysis of p-3He scattering below 200 MeV NUCLEAR REACTIONS 3He(p, p'), E=4-200 MeV; analyzed data; deduced phase shifts.
doi: 10.1142/S021773230301065X
2001FU07 Nucl.Phys. A687, 311c (2001) Y.Fujita, T.Adachi, H.Akimune, A.D.Bacher, G.P.A.Berg, T.Black, I.Daito, C.C.Foster, H.Fujimura, H.Fujita, M.Fujiwara, K.Hara, K.Harada, M.N.Harakeh, K.Hatanaka, T.Inomata, J.Janecke, J.Kamiya, Y.Kanzaki, K.Katori, T.Kawabata, W.Lozowski, K.Nagayama, T.Noro, D.A.Roberts, H.Sakaguchi, Y.Shimbara, T.Shinada, E.J.Stephenson, A.Tamii, K.Tamura, M.Tanaka, H.Ueno, T.Wakasa, T.Yamanaka, M.Yoshifuku, M.Yosoi Isospin Symmetry-Structure Study at New High-Resolution Course of RCNP NUCLEAR REACTIONS 27Al(3He, t), E=150 MeV/nucleon; 27Al(p, p'), E=160 MeV; measured excitation energy spectra Gamow-Teller strength distributions, M1 strength distributions, resonance parameters.
doi: 10.1016/S0375-9474(01)00637-6
2001LI14 Prog.Theor.Phys.(Kyoto) 105, 233 (2001) V.Limkaisang, K.Harada, J.Nagata, H.Yoshino, Y.Yoshino, M.Shoji, M.Matsuda Phase-Shift Analysis of pp Scattering at TL = 25-500 MeV NUCLEAR REACTIONS 1H(p, p), E=25-500 MeV; analyzed σ(θ), analyzing powers, spin-correlation observables; deduced pion-proton coupling constant, phase shifts.
doi: 10.1143/PTP.105.233
1995MA92 Prog.Theor.Phys.(Kyoto) 93, 1059 (1995) M.Matsuda, J.Nagata, H.Yoshino, K.Harada, S.Ohara Noticeable Change of p-p Spin-Orbit Interaction at Short Distance - A Possible First-Order Phase Transition Found in p-p Scattering at T(L) = 3 ∼ 10 GeV - NUCLEAR REACTIONS 1H(p, p), E at 3.6-12 GeV/c; analyzed phase shifts; deduced short-range, repulsive spin-orbit interaction features.
doi: 10.1143/ptp/93.6.1059
1994KO45 J.Labelled Compd.Radiopharm. 35, 213 (1994) T.Koiso, O.Ishibashi, K.Harada, M.Nakayama, A.Sugii A New Ge-68/Ga-68 Generator System Prepared from N-Methylglucamine Type Organic Polymer
1987IW02 Z.Phys. A326, 201 (1987) Enhancement of the Subbarrier Fusion Reaction due to Neck Formation NUCLEAR REACTIONS, ICPND 40Ca(40Ca, X), E=45-65 MeV; 58Ni(58Ni, X), E=90-110 MeV; 64Ni(64Ni, X), E=85-110 MeV; 74Ge(74Ge, X), E=105-135 MeV; 80Se(80Se, X), E=125-150 MeV; 90Zr(90Zr, X), E=170-195 MeV; calculated fusion σ(E), potential energies. Neck formation, Krappe-Nix-Sierk model.
1984IW04 Nucl.Phys. A419, 472 (1984) An Extension of the Generalized Exciton Model and Calculations of (p, p') and (p, α) Angular Distributions NUCLEAR REACTIONS 197Au, 209Bi, 120Sn(p, p'), E=62 MeV; calculated σ(θ, Ep'). 120Sn(p, α), E=62 MeV; 209Bi(p, α), E=39, 62 MeV; calculated σ(θ, Eα). Generalized exciton model.
doi: 10.1016/0375-9474(84)90627-4
1983OT01 Phys.Lett. 121B, 106 (1983) Pre-Equilibrium Description of Fast Light Particle Emission in Heavy-Ion Reactions NUCLEAR REACTIONS 181Ta(14N, p), (14N, d), (14N, t), (14N, α), E=115 MeV; calculated σ(Ep), σ(Ed), σ(Et), σ(Eα). Extended exciton model.
doi: 10.1016/0370-2693(83)90895-X
1983SA27 Phys.Rev. C28, 1527 (1983) Pre-Equilibrium Emission of Light Composite Particles in the Framework of the Exciton Model NUCLEAR REACTIONS 89Y, 120Sn, 197Au, 54Fe(p, p), (p, d), (p, t), (p, 3He), (p, α), E=62 MeV; 58Ni(p, t), (p, α), (p, 3He), E=90 MeV; calculated σ(Ep), σ(Ed), σ(Et), σ(E(3He)), σ(Eα); deduced composite particle emission mechanism. Exciton model.
doi: 10.1103/PhysRevC.28.1527
1982IW03 Phys.Rev. C26, 1821 (1982) Mechanism of Cluster Emission in Nucleon-Induced Preequilibrium Reactions NUCLEAR REACTIONS 54Fe, 118,120Sn(p, α), E=29-62 MeV; calculated σ(E, Eα); deduced reaction mechanism. Exciton model, preequilibrium emission.
doi: 10.1103/PhysRevC.26.1821
1981IW03 Z.Phys. A302, 149 (1981) A.Iwamoto, K.Harada, S.Yamaji, S.Yoshida Microscopic Calculation of Friction Coefficients for use in Heavy-Ion Reaction NUCLEAR REACTIONS 196Pt(40Ar, X), E not given; calculated friction coefficient. Deep inelastic collision, linear response theory, two-center shell model.
doi: 10.1007/BF01413045
1981YA09 Phys.Lett. 106B, 433 (1981) S.Yamaji, A.Iwamoto, K.Harada, S.Yoshida Microscopic Calculation of the Mass Diffusion Coefficient using Linear Response Theory NUCLEAR REACTIONS 27Al(20Ne, X), E=120 MeV; 197Au(63Cu, X), E=365, 443 MeV; 209Bi(136Xe, X), E=1130 MeV; 165Ho, 209Bi(84Kr, X), E=714 MeV; 58Ni(16O, X), E=92 MeV; 50Ti(32S, X), E=131, 166 MeV; 197Au, 109Ag(40Ar, X), E=288 MeV; 197Au(40Ar, X), E=340 MeV; 232Th(40Ar, X), E=279, 388 MeV; 197Au(86Kr, X), E=620 MeV; calculated mass diffusion coefficient. Linear response theory.
doi: 10.1016/0370-2693(81)90250-1
1979SA10 Z.Phys. A290, 149 (1979) K.Sato, S.Yamaji, K.Harada, S.Yoshida A Numerical Analysis of the Heavy-Ion Reaction Based on the Linear Response Theory NUCLEAR REACTIONS 28Si(20Ne, X), E=120 MeV; calculated σ(θ). Linear response theory with collective variables, deformation δ, relative distance R, two-dimensional coupled equations of motion.
doi: 10.1007/BF01408109
1977IW01 Phys.Lett. 68B, 35 (1977) On the Focussing Effect and the Large Energy Loss in the Quasi-Fission Reaction NUCLEAR REACTIONS Bi(Kr, F), E=525, 600 MeV; Pb(Kr, F), E=494, 510, 718 MeV; Bi(Xe, F), E=1130 MeV; Sb(Ar, F), E=199, 300 MeV; calculated fission parameters, σ(θ).
doi: 10.1016/0370-2693(77)90028-4
1976IW02 Progr.Theor.Phys. 55, 115 (1976) A.Iwamoto, S.Yamaji, S.Suekane, K.Harada Potential Energy Surfaces for the Fission of the Actinide Nuclei NUCLEAR STRUCTURE 232,236,240,244,248Th, 232,234,236,238,240,242,246,250U, 236,240,244,248,252Pu, 238,242,246,250,254Cm, 240,244,248,250,252,256Cf, 242,246,250,254,258Fm, 244,248,252,256,260No; calculated potential energy surfaces for fission.
doi: 10.1143/PTP.55.115
1974IW01 Progr.Theor.Phys. 51, 1617 (1974) A.Iwamoto, S.Suekane, S.Yamaji, K.Harada Asymmetric Fission of 236U RADIOACTIVITY, Fission 236U(SF); calculated total potential energy surface for asymmetric fission.
doi: 10.1143/PTP.51.1617
1970HA20 Phys.Rev.Lett. 24, 1438 (1970) E1 Transitions from the Septuplet in Bi209 NUCLEAR STRUCTURE 209Bi; calculated B(E1) for septuplet states.
doi: 10.1103/PhysRevLett.24.1438
1970HA38 Phys.Lett. 32B, 542 (1970) M1 Decay of the 1.7 MeV 1+ State in 206Pb NUCLEAR STRUCTURE 206Pb; calculated B(M1) for 1.7-MeV 1+ state.
doi: 10.1016/0370-2693(70)90538-1
1970HA57 Nucl.Phys. A159, 209 (1970) The Effects of Magnetic Dipole Core Polarization in 206Pb and 207Pb NUCLEAR STRUCTURE 206,207Pb; calculated levels, B(M1), μ. Weak-coupling model, magnetic dipole core polarization.
doi: 10.1016/0375-9474(70)90037-0
1968HA19 Phys.Rev. 169, 818 (1968) Unified Theory of Alpha Decay
doi: 10.1103/PhysRev.169.818
1968OK03 Nucl.Phys. A115, 17(1968) K.Okano, S.Kikuchi, K.Nishimura, K.Harada Investigation of the 9Be(3He, N)11C Reaction in the Energy Range 3.5-10 MeV NUCLEAR REACTIONS 9Be(3He, n), E = 3.49-9.96 MeV; measured σ(E; En, θ).
doi: 10.1016/0375-9474(68)90639-8
1967RA37 Nucl.Phys. A94, 33 (1967) E.A.Rauscher, J.O.Rasmussen, K.Harada Coupled-Channel, Alpha Decay Rate Theory Applied to 212mPo RADIOACTIVITY 212mPo; calculated partial T1/2, barrier penetration factors. Coupled-channel formalism.
doi: 10.1016/0375-9474(67)90807-X
1965GL06 Nucl.Phys. 72, 481 (1965) Shell-Model Calculation for 212Po NUCLEAR STRUCTURE 212Po; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(65)90406-2
1958OD07 Nuclear Phys. 7, 251 (1958) Inelastic Scattering of Protons at Intermediate Energies
doi: 10.1016/0029-5582(58)90257-8
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