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NSR database version of April 11, 2024.

Search: Author = K.Harada

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2016HA25      Phys.Rev. C 94, 024004 (2016)

K.Harada, S.Sasabe, M.Yahiro

Numerical study of renormalization group flows of nuclear effective field theory without pions on a lattice

doi: 10.1103/PhysRevC.94.024004
Citations: PlumX Metrics

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

2011HA12      Phys.Rev. C 83, 034002 (2011)

K.Harada, H.Kubo, Y.Yamamoto

Pions are neither perturbative nor nonperturbative: Wilsonian renormalization-group analysis of nuclear effective field theory including pions

doi: 10.1103/PhysRevC.83.034002
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1573. Data from this article have been entered in the XUNDL database. For more information, click here.

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
Citations: PlumX Metrics

2006HA18      Phys.Lett. B 636, 305 (2006)

K.Harada, K.Inoue, H.Kubo

Wilsonian RG and redundant operators in nonrelativistic effective field theory

doi: 10.1016/j.physletb.2006.03.072
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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
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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)

A.Iwamoto, K.Harada

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)

A.Iwamoto, K.Harada

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
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1983OT01      Phys.Lett. 121B, 106 (1983)

T.Otsuka, K.Harada

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
Citations: PlumX Metrics

1983SA27      Phys.Rev. C28, 1527 (1983)

K.Sato, A.Iwamoto, K.Harada

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
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1982IW03      Phys.Rev. C26, 1821 (1982)

A.Iwamoto, K.Harada

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
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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
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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
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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
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1977IW01      Phys.Lett. 68B, 35 (1977)

A.Iwamoto, K.Harada

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
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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
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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
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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
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1970HA38      Phys.Lett. 32B, 542 (1970)

K.Harada, S.Pittel

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
Citations: PlumX Metrics

1970HA57      Nucl.Phys. A159, 209 (1970)

K.Harada, S.Pittel

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
Citations: PlumX Metrics

1968HA19      Phys.Rev. 169, 818 (1968)

K.Harada, E.A.Rauscher

Unified Theory of Alpha Decay

doi: 10.1103/PhysRev.169.818
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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
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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
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1965GL06      Nucl.Phys. 72, 481 (1965)

N.K.Glendenning, K.Harada

Shell-Model Calculation for 212Po

NUCLEAR STRUCTURE 212Po; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(65)90406-2
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1958OD07      Nuclear Phys. 7, 251 (1958)

N.Oda, K.Harada

Inelastic Scattering of Protons at Intermediate Energies

doi: 10.1016/0029-5582(58)90257-8
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