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NSR database version of April 24, 2024.

Search: Author = M.Kamimura

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2023KA09      Phys.Rev. C 107, 034607 (2023)

M.Kamimura, Y.Kino, T.Yamashita

Comprehensive study of muon-catalyzed nuclear reaction processes in the dtμ molecule

NUCLEAR REACTIONS 2H(t, nα), E(cm)=1-300 keV; calculated S(E) factors using three different sets of nuclear interactions. 4He(n, X), E=21.5-22.6 MeV; calculated total σ(E) using one set of nuclear interactions, and compared with experimental data; calculated muon-catalyzed fusion in a dtμ-molecule yielding reaction products of 4He+n+μ+17.6 MeV and 4Heμ+n+17.6 MeV; deduced fusion rate, momentum and energy spectra of emitted muon and 4Heμ-sticking probability using coupled-channel method and T-matrix method.

doi: 10.1103/PhysRevC.107.034607
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2023KA17      Prog.Theor.Exp.Phys. 2023, 071D01 (2023)

M.Kamimura

Derivation of transition density from the observed 4He(e, e')4He(0+2) form factor raising the α-particle monopole puzzle

NUCLEAR REACTIONS 4He(e-, e-'), E not given; analyzed data. 4He; deduced energy levels, J, π, transition density from the monopole transition form factor of the electron-scattering excitation of the 0+2 state.

doi: 10.1093/ptep/ptad090
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2017CA16      Few-Body Systems 58, 67 (2017)

J.Carbonell, R.Lazauskas, E.Hiyama, M.Kamimura

On the Possible Existence of Four Neutron Resonances

NUCLEAR REACTIONS 3He(n, n), E=0.03-10 MeV;3He(n, x), E not given; calculated possible tetraneutron resonance trajectory for 0+ state; deduced resonance, σ, resonance energy and width vs other parameters, higher 4n resonances, tetraneutron production response function via double charge exchange; deduced parameters.

doi: 10.1007/s00601-017-1219-0
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2016HI03      Phys.Rev. C 93, 044004 (2016)

E.Hiyama, R.Lazauskas, J.Carbonell, M.Kamimura

Possibility of generating a 4-neutron resonance with a T=3/2 isospin 3-neutron force

NUCLEAR STRUCTURE 4n; calculated narrow resonant states of tetraneutron for Jπ=0+, 2+ and 2-. 4H, 4He, 4Li; calculated energies of the lowest T=1, Jπ=2- states. 3n; calculated resonance trajectories for Jπ=3/2-, 1/2- and 1/2+ states. Complex scaling method (CSM) for resonance positions and widths. Gaussian expansion method used to solve Schrodinger equation and Lagrange-mesh technique to solve Faddeev-Yakubovsky (FY) equation. Comparison with recent experimental data from RIKEN.

doi: 10.1103/PhysRevC.93.044004
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2015HI04      Phys.Rev. C 91, 054316 (2015)

E.Hiyama, M.Isaka, M.Kamimura, T.Myo, T.Motoba

Resonant states of the neutron-rich Λ hypernucleus 7ΛHe

NUCLEAR STRUCTURE 6He; calculated levels, J, π, widths. 7He; calculated levels, J, π, widths of hypernucleus in the framework of α+Λ+n+n four-body cluster model. Comparison with experimental data.

doi: 10.1103/PhysRevC.91.054316
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2013HI03      Nucl.Phys. A908, 29 (2013)

E.Hiyama, S.Ohnishi, M.Kamimura, Y.Yamamoto

Four-body structure of neutron-rich hypernucleus 6ΛH

NUCLEAR STRUCTURE 6H; calculated λ hypernucleus 6H radial density distribution using tnnΛ four-body cluster model; deduced 6ΛH ground state as a resonant state.

doi: 10.1016/j.nuclphysa.2013.04.001
Citations: PlumX Metrics


2013HI07      Few-Body Systems 54, 737 (2013)

E.Hiyama, M.Kamimura

Four-Body Structure of Λ Hypernuclei and 4He Tetramer System

NUCLEAR STRUCTURE 4H, 4He; calculated hypernuclei ground and excited states parameters, energy levels, J, π. Gaussian expansion method.

doi: 10.1007/s00601-012-0471-6
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2013OH06      Prog.Theor.Exp.Phys. 2013, 073D02 (2013)

S.-I.Ohtsubo, Y.Fukushima, M.Kamimura, E.Hiyama

Complex-scaling calculation of three-body resonances using complex-range Gaussian basis functions: Application to 3α resonances in 12C

NUCLEAR STRUCTURE 12C; calculated three-body α resonances, level energies, J, π. Comparison with available data.

doi: 10.1093/ptep/ptt048
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2011OG12      J.Phys.:Conf.Ser. 312, 082008 (2011)

K.Ogata, T.Matsumoto, S.Hashimoto, K.Minomo, T.Egami, Y.Iseri, M.Kohno, S.Chiba, C.A.Bertulani, Y.R.Shimizu, M.Kamimura, M.Yahiro

Status of breakup reaction theory

NUCLEAR REACTIONS 7Li(d, γ), (d, n), (d, p), E=10-50 MeV; calculated σ. 90Zr(p, p), E=65, 800 MeV; calculated dσ with and without Brieva-Rook localization. 208Pb(8B, X), E=250 MeV/nucleon; calculated breakup σ including relativistic corrections. 209Bi(6He, 6He), E=22.5 MeV; calculated σ with and without breakup effects, B(E1) strength distribution. Three- and four-body CDCC.

doi: 10.1088/1742-6596/312/4/082008
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2010HI01      Phys.Rev.Lett. 104, 212502 (2010)

E.Hiyama, M.Kamimura, Y.Yamamoto, T.Motoba

Five-Body Cluster Structure of the Double-Λ Hypernucleus 11ΛΛBe

NUCLEAR STRUCTURE 11Be; calculated energy levels of double hypernucleus; deduced observation of the ground state of 11ΛΛBe in KEK-E373 experiment.

doi: 10.1103/PhysRevLett.104.212502
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2010HI07      Prog.Theor.Phys.(Kyoto), Suppl. 185, 106 (2010)

E.Hiyama, M.Kamimura, Y.Yamamoto, T.Motoba, T.A.Rijken

S = -1 Hypernuclear Structure

NUCLEAR STRUCTURE 4H, 4,6,7He, 7Li, 7,9Be, 12,13C; calculated hypernucleus excitation energies, splittings, n-p relative and probability densities, B(E2). Comparison with experimental data.

doi: 10.1143/PTPS.185.106
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2010HI08      Prog.Theor.Phys.(Kyoto), Suppl. 185, 152 (2010)

E.Hiyama, M.Kamimura, Y.Yamamoto, T.Motoba, T.A.Rijken

S = -2 Hypernuclear Structure

NUCLEAR STRUCTURE 5,7H, 7He, 7,8,9,10Li, 9,10,11,12Be; calculated double hypernucleus energy levels and ground state J, π, rms radii, density distribution, binding energies. Cluster model and the Gaussian Expansion Method (GEM).

doi: 10.1143/PTPS.185.152
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2009HI12      Phys.Rev. C 80, 054321 (2009)

E.Hiyama, Y.Yamamoto, T.Motoba, M.Kamimura

Structure of A=7 iso-triplet Λ hypernuclei studied with the four-body cluster model

NUCLEAR STRUCTURE 6He, 6Li, 6Be, 7He, 7Li, 7Be; calculated levels, J, π, total interaction energies, and density distributions of hypernuclei using four-body cluster model.

doi: 10.1103/PhysRevC.80.054321
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2009MO40      Nucl.Phys. A827, 318c (2009)

T.Motoba, S.Sugimoto, E.Hiyama, Y.Yamamoto, Th.A.Rijken, M.Kamimura

Structure and production of p-shell Ξ-hypernuclei predicted with realistic interactions

doi: 10.1016/j.nuclphysa.2009.05.065
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2008HI16      Phys.Rev. C 78, 054316 (2008)

E.Hiyama, Y.Yamamoto, T.Motoba, Th.A.Rijken, M.Kamimura

Light Ξ hypernuclei in four-body cluster models

NUCLEAR STRUCTURE 5,7H, 9,10Li, 12Be; calculated level energies, density distributions, binding energies, rms radii. Gaussian expansion method. Hypernuclei.

doi: 10.1103/PhysRevC.78.054316
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2008OG01      Nucl.Phys. A805, 447c (2008)

K.Ogata, T.Matsumoto, T.Egami, Y.Iseri, M.Kamimura, M.Yahiro

Full coupled-channel description of three-body and four-body breakup reactions

NUCLEAR REACTIONS 208Pb(8B, X), E=52 MeV/nucleon; calculated breakup σ(θ) with eikonal CDCC; deduced 7Be(p, γ) astrophysical S-factor. 209Bi(6He, 6He), E=19, 22.5 MeV; calculated total, elastic σ(θ) using four-body CDCC. Comparison with data.

doi: 10.1016/j.nuclphysa.2008.02.283
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2007HA38      Phys.Lett. B 650, 268 (2007)

K.Hamaguchi, T.Hatsuda, M.Kamimura, Y.Kino, T.T.Yanagida

Stau-catalyzed 6Li production in big-bang nucleosynthesis

NUCLEAR REACTIONS 4He(d, γ)6Li, E=low; calculated stau-catalyzed fusion σ, astrophysical S-factor.

doi: 10.1016/j.physletb.2007.05.030
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2006HI05      Few-Body Systems 38, 91 (2006)

E.Hiyama, M.Kamimura, A.Hosaka, H.Toki, M.Yahiro

Five-Body Calculation of Resonance and Scattering States of the uudd(s-bar) System

doi: 10.1007/s00601-005-0143-x
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2006MA31      Phys.Rev. C 73, 051602 (2006)

T.Matsumoto, T.Egami, K.Ogata, Y.Iseri, M.Kamimura, M.Yahiro

Coulomb breakup effects on the elastic cross section of 6He + 209Bi scattering near Coulomb barrier energies

NUCLEAR REACTIONS 209Bi(6He, 6He), E=19, 22.5 MeV; analyzed elastic σ(θ), Coulomb breakup effects. Four-body continuum-discretized coupled-channels model.

doi: 10.1103/PhysRevC.73.051602
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2006OG01      Phys.Rev. C 73, 024605 (2006)

K.Ogata, S.Hashimoto, Y.Iseri, M.Kamimura, M.Yahiro

Determination of S17 from 8B breakup by means of the method of continuum-discretized coupled channels

NUCLEAR REACTIONS 208Pb(8B, p7Be), E=52 MeV/nucleon; analyzed σ(θ). 7Be(p, γ), E=low; deduced astrophysical S-factor. Continuum-discretized coupled channels method.

doi: 10.1103/PhysRevC.73.024605
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2005HI13      Nucl.Phys. A754, 103c (2005)

E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto

Three- and four-body structure of light double Λ hypernuclei

NUCLEAR STRUCTURE 6,7He, 7,8,9Li, 9,10Be; calculated two-Λ hypernucleus levels, J, π. Four-body model.

doi: 10.1016/j.nuclphysa.2004.12.075
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2005HI14      Nucl.Phys. A755, 411c (2005)

E.Hiyama, M.Kamimura, A.Hosaka, H.Toki, M.Yahiro

Five-body calculation of resonance and continuum states of pentaquark baryons with quark-quark correlations

doi: 10.1016/j.nuclphysa.2005.03.047
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2004EG04      Phys.Rev. C 70, 047604 (2004)

T.Egami, K.Ogata, T.Matsumoto, Y.Iseri, M.Kamimura, M.Yahiro

Gaussian expansion approach to nuclear and Coulomb breakup

NUCLEAR REACTIONS 58Ni(8B, p7Be), E=25.8 MeV; calculated breakup σ(θ), Coulomb and nuclear contributions. Continuum discretized coupled channels approach, comparison with data.

doi: 10.1103/PhysRevC.70.047604
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2004HI09      Nucl.Phys. A737, 138 (2004)

E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto

Few-body aspects of light hypernuclei

NUCLEAR STRUCTURE 8Be; calculated level energies. 4,6,7He, 7,8,9Li, 9,10Be, 13C; calculated energy levels, J, π for single and double Λ hypernuclei.

doi: 10.1016/S0375-9474(04)00307-0
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2004HI11      Nucl.Phys. A738, 175 (2004)

E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto

Clustering aspects of light hypernuclei

NUCLEAR STRUCTURE 7He, 7,8,9Li, 9,10Be; calculated double-Λ hypernuclei energy levels. Gaussian expansion method.

doi: 10.1016/j.nuclphysa.2004.04.028
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2004HI14      Prog.Theor.Phys.(Kyoto) 112, 99 (2004)

E.Hiyama, K.Suzuki, H.Toki, M.Kamimura

Role of the Quark-Quark Correlation in Baryon Structure and Non-Leptonic Weak Transitions of Hyperons

doi: 10.1143/PTP.112.99
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2004HI21      Phys.Rev. C 70, 031001 (2004)

E.Hiyama, B.F.Gibson, M.Kamimura

Four-body calculation of the first excited state of 4He using a realistic NN interaction: 4He(e, e')4He(0+2) and the monopole sum rule

NUCLEAR STRUCTURE 4He; calculated ground and excited states energies, radii, mass densities, wave functions. Two-body and three-body forces, Gaussian expansion method.

NUCLEAR REACTIONS 4He(e, e'), E not given; calculated transition form factor. Two-body and three-body forces, Gaussian expansion method.

doi: 10.1103/PhysRevC.70.031001
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2004MA57      Nucl.Phys. A738, 471 (2004)

T.Matsumoto, E.Hiyama, M.Yahiro, K.Ogata, Y.Iseri, M.Kamimura

Four-body CDCC analysis of 6He + 12C scattering

NUCLEAR REACTIONS 12C(6He, 6He), E=38.3 MeV/nucleon; analyzed σ(θ); deduced halo effects. Continuum-discretized coupled-channels approach.

doi: 10.1016/j.nuclphysa.2004.04.089
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2004MB01      Phys.Rev. C 70, 061601 (2004)

T.Matsumoto, E.Hiyama, K.Ogata, Y.Iseri, M.Kamimura, S.Chiba, M.Yahiro

Continuum-discretized coupled-channels method for four-body nuclear breakup in 6He+12C scattering

NUCLEAR REACTIONS 12C(6He, 6He), (6He, 2nα), E=18, 229.8 MeV; calculated elastic and breakup σ(θ), reaction σ. Continuum-discretized coupled-channels method, comparison with data.

doi: 10.1103/PhysRevC.70.061601
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2004OG09      Nucl.Phys. A738, 421 (2004)

K.Ogata, M.Yahiro, Y.Iseri, T.Matsumoto, N.Yamashita, T.Kamizato, M.Kamimura

Determination of S17 from 8B Coulomb dissociation

NUCLEAR REACTIONS 58Ni(8B, p7Be), E=25.8 MeV; analyzed σ(θ); deduced asymptotic normalization coefficient. 7Be(p, γ), E=low; deduced astrophysical S-factor. Continuum-discretized coupled-channels approach.

doi: 10.1016/j.nuclphysa.2004.04.078
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2003HI09      Prog.Part.Nucl.Phys. 51, 1 (2003)

E.Hiyama, Y.Kino, M.Kamimura

Gaussian, Expansion Methods for Few-Body Systems

doi: 10.1016/S0146-6410(03)00082-6
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2003HI24      Mod.Phys.Lett. A 18, 95 (2003)

E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto

Few-body aspects of hypernuclear physics

NUCLEAR STRUCTURE 4H, 4,7He, 7,8,9Li, 9,10Be; calculated Λ and ΛΛ hypernucleus level energies, J, π.

doi: 10.1142/S021773230301003X
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2003KI20      Hyperfine Interactions 146-147, 331 (2003)

Y.Kino, N.Yamanaka, M.Kamimura, H.Kudo

High-Precision Calculation of the Fine and Hyperfine Structure Splittings of Antiprotonic Helium-3, 4 Atoms

ATOMIC PHYSICS 3,4He; calculated hfs in antiprotonic helium atoms.

doi: 10.1023/B:HYPE.0000004218.62114.f2
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2003KI27      Mod.Phys.Lett. A 18, 388 (2003)

Y.Kino, H.Kudo, M.Kamimura

High-precision Coulomb three-body calculation of antiprotonic helium atoms

ATOMIC PHYSICS He; calculated energy levels and widths for antiprotonic helium.

doi: 10.1142/S0217732303010545
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2003MA91      Phys.Rev. C 68, 064607 (2003)

T.Matsumoto, T.Kamizato, K.Ogata, Y.Iseri, E.Hiyama, M.Kamimura, M.Yahiro

New treatment of breakup continuum in the method of continuum discretized coupled channels

NUCLEAR REACTIONS 58Ni(d, d), (d, X), E=80 MeV; 40Ca(6Li, 6Li), (6Li, X), E=156 MeV; calculated elastic σ, breakup S-matrix elements. Continuum discretized coupled channels, pseudostate discretization.

doi: 10.1103/PhysRevC.68.064607
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2003OG02      Phys.Rev. C 67, 011602 (2003); Erratum Phys.Rev. C 67, 019902 (2003)

K.Ogata, M.Yahiro, Y.Iseri, M.Kamimura

Determination of S17 from the 7Be(d, n)8B reaction

NUCLEAR REACTIONS 7Li(d, d), E=8 MeV; 7Li(n, n), E=4.26 MeV; 7Be(d, n), E=7.5 MeV; analyzed σ(θ); deduced parameters. 7Be(p, γ), E not given; deduced astrophysical S-factor. Continuum-discretized coupled channels, three-body model.

doi: 10.1103/PhysRevC.67.011602
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2003OG06      Phys.Rev. C 68, 064609 (2003)

K.Ogata, M.Yahiro, Y.Iseri, T.Matsumoto, M.Kamimura

New coupled-channel approach to nuclear and Coulomb breakup reactions

NUCLEAR REACTIONS 58Ni(8B, p7Be), E=240 MeV; calculated breakup σ(θ). Hybrid calculation.

doi: 10.1103/PhysRevC.68.064609
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2002HI01      Phys.Rev. C65, 011301 (2002)

E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto

Λ-Σ Conversion in Λ4He and Λ4H Based on a Four-Body Calculation

NUCLEAR STRUCTURE 4H, 4He; calculated hypernucleus levels, J, π; deduced role of Λ-Σ conversion. Four-body calculations.

doi: 10.1103/PhysRevC.65.011301
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2002HI15      Phys.Rev. C66, 024007 (2002)

E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto

Four-body cluster structure of A=7-10 double-Λ hypernuclei

NUCLEAR STRUCTURE 7He, 7,8,9Li, 9,10Be; calculated double-Λ hypernuclei level energies, J, π. Four-body cluster model.

doi: 10.1103/PhysRevC.66.024007
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2002IT09      Prog.Theor.Phys.(Kyoto), Suppl. 146, 573 (2002)

M.Ito, K.Kato, Y.Sakuragi, M.Kamimura, E.Hiyama

6He + 6He Molecular States in Highly-Excited 12Be

NUCLEAR STRUCTURE 12Be; calculated molecular states energies, J, coupling effects.

doi: 10.1143/PTPS.146.573
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2001HI05      Nucl.Phys. A684, 227c (2001)

E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto

Three- and Four-Body Structure of Light Hypernuclei

doi: 10.1016/S0375-9474(01)00418-3
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2001HI09      Nucl.Phys. A691, 107c (2001)

E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto

Three- and Four-Body Structure of Light Λ Hypernuclei

NUCLEAR STRUCTURE 4H, 4He, 7Li, 9Be, 13C; calculated hypernucleus levels, spin-orbit splitting, B(E2), related features.

doi: 10.1016/S0375-9474(01)01015-6
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2001KA47      Phys.Rev. C64, 044001 (2001)

H.Kamada, A.Nogga, W.Glockle, E.Hiyama, M.Kamimura, K.Varga, Y.Suzuki, M.Viviani, A.Kievsky, S.Rosati, J.Carlson, S.C.Pieper, R.B.Wiringa, P.Navratil, B.R.Barrett, N.Barnea, W.Leidemann, G.Orlandini

Benchmark Test Calculation of a Four-Nucleon Bound State

NUCLEAR STRUCTURE A=4; calculated four-nucleon bound state energy, radius, related features. Several approaches compared.

doi: 10.1103/PhysRevC.64.044001
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2000HI15      Phys.Rev.Lett. 85, 270 (2000)

E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto

ΛN Spin-Orbit Splittings in Λ9Be and Λ13C Studied with One-Boson-Exchange ΛN Interactions

NUCLEAR STRUCTURE 9Be, 13C; calculated hypernuclei levels, J, π, spin-orbit splitting related features. One-boson exchange models, quark models.

doi: 10.1103/PhysRevLett.85.270
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2000SU11      Nucl.Phys. A670, 307c (2000)

K.Suzuki, E.Hiyama, H.Toki, M.Kamimura

Constituent Quark Model for Baryons with Strong Quark-Pair Correlations and Non-Leptonic Weak Transitions of Hyperon

doi: 10.1016/S0375-9474(00)00119-6
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1999HI02      Phys.Rev. C59, 2351 (1999)

E.Hiyama, M.Kamimura, K.Miyazaki, T.Motoba

γ Transitions in A = 7 Hypernuclei and a Possible Derivation of Hypernuclear Size

NUCLEAR STRUCTURE 7He, 7Li; calculated transitions B(E2), B(M1) in hypernuclei; deduced implications for radius measurement. Three-body model.

NUCLEAR REACTIONS 7Li(π+, K+), E at 1.05 GeV/c; calculated hypernuclear states production σ(E).

doi: 10.1103/PhysRevC.59.2351
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1999PI13      Phys.Rev. C60, 044611 (1999)

R.A.D.Piyadasa, M.Kawai, M.Kamimura, M.Yahiro

Convergence of the Solution of the Continuum Discretized Coupled Channels Method

NUCLEAR REACTIONS 58Ni(d, d), (d, np), E=80 MeV; calculated S-matrix elements; deduced model convergence features. Continuum discretized coupled channels method.

doi: 10.1103/PhysRevC.60.044611
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1998HI13      Nucl.Phys. A639, 169c (1998)

E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto

Four-Body Calculation of Λ4H and Λ4He with Realistic ΛN Interactions

NUCLEAR STRUCTURE 4H, 4He; calculated hypernuclei binding energieslevels, J, π. Four-body calculations, 3N + Λ model.

doi: 10.1016/S0375-9474(98)00267-X
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1998HI14      Nucl.Phys. A639, 173c (1998)

E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto

Four-Body Model Study of Competition between YN Spin-Spin and Spin-Orbit Interactions in Light Hypernuclei

NUCLEAR STRUCTURE 7Li, 13C; calculated hypernuclei levels, J, π; deduced ΛN spin-spin, spin-orbit forces related features.

doi: 10.1016/S0375-9474(98)00268-1
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1998KI07      Nucl.Phys. A631, 649c (1998)

Y.Kino, M.Kamimura, H.Kudo

High-Accuracy 3-Body Coupled-Channel Calculation of Metastable States of Antiprotonic Helium Atoms

ATOMIC PHYSICS 4He; calculated antiprotonic atoms metastable states energies, widths. Three-body coupled channels method.

doi: 10.1016/S0375-9474(98)00084-0
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1997HI09      Prog.Theor.Phys.(Kyoto) 97, 881 (1997)

E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto

Three- and Four-Body Cluster Models of Hypernuclei using the G-Matrix ΛN Interaction (Λ)9Be, (Λ)13C, (Λ)(Λ)6He and (Λ)(Λ)10Be

NUCLEAR STRUCTURE 6He, 9,10Be, 13C; calculated hypernucleus ground, excited states energies. Three-, four-body cluster models, ΛN interaction.

doi: 10.1143/PTP.97.881
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1996HI03      Phys.Rev. C53, 2075 (1996)

E.Hiyama, M.Kamimura, T.Motoba, T.Yamada, Y.Yamamoto

Three-Body Model Study of A = 6-7 Hypernuclei: Halo and skin structures

NUCLEAR STRUCTURE A=6; A=7; calculated hypernuclei states, binding energies. Three-body model.

doi: 10.1103/PhysRevC.53.2075
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1995HI15      Nucl.Phys. A588, 35c (1995)

E.Hiyama, M.Kamimura

Three-Body Structure of 6He = 4He + n + n using Realistic n-n Potentials

NUCLEAR STRUCTURE 6He; calculated binding energy, two-neutron relative density. Coupled-rearrangement-channel variational method, realistic NN-potential.

doi: 10.1016/0375-9474(95)00096-J
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1991IS06      Nucl.Phys. A533, 574 (1991)

Y.Iseri, M.Tanifuji, H.Kameyama, M.Kamimura, M.Yahiro

Spin-Dependent Interactions and Polarization Observables in Elastic Scattering of Deuterons at Intermediate Energies

NUCLEAR REACTIONS 58Ni(polarized d, d), E=700 MeV; calculated vector, tensor analyzing power vs θ.

doi: 10.1016/0375-9474(91)90534-D
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1990KA06      Nucl.Phys. A508, 17c (1990)

M.Kamimura, H.Kameyama

Coupled Rearragement Channel Calculations of Muonic Molecules and A = 3 Nuclei

NUCLEAR STRUCTURE 3H, 3He; calculated binding energy, S-, D-state probability, asymptotic normalizations. 4He; calculated binding energy. Coupled rearragement channels method.

doi: 10.1016/0375-9474(90)90459-Y
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1989KA19      Phys.Rev. C40, 974 (1989)

H.Kameyama, M.Kamimura, Y.Fukushima

Coupled-Rearrangement-Channel Gaussian-Basis Variational Method for Trinucleon Bound States

NUCLEAR STRUCTURE 2H; calculated wave function. 3H, 3He; calculated binding energy, S-, P-, D-state probabilities, S-, D-wave asymptotic normalizations. Gaussian basis, coupled-rearrangement-channel variational method.

doi: 10.1103/PhysRevC.40.974
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1989MY02      Z.Phys. A334, 423 (1989)

K.S.Myint, Y.Akaishi, H.Tanaka, M.Kamimura, H.Narumi

Relativistic and QED Contributions to the Coulomb Three-Body System in Muon-Catalyzed Fusion


1989TA07      Phys.Lett. 217B, 375 (1989)

M.Tanifuji, H.Kameyama, M.Kamimura, Y.Iseri, M.Yahiro

T(R) and T(L) Tensor Interactions in Deuteron Elastic Scattering

NUCLEAR REACTIONS 58Ni(polarized d, d), E=700 MeV; calculated σ(θ), analyzing power.

doi: 10.1016/0370-2693(89)90063-4
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1988IS02      Nucl.Phys. A490, 383 (1988)

Y.Iseri, H.Kameyama, M.Kamimura, M.Yahiro, M.Tanifuji

Virtual Breakup Effects in Elastic Scattering of Polarized Deuterons

NUCLEAR REACTIONS 16O, 40Ca, 58Ni, 118Sn, 208Pb(polarized d, d), E=56 MeV; analyzed σ(θ), vector, tensor analyzing power vs θ; deduced reaction mechansim.

doi: 10.1016/0375-9474(88)90512-X
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1988KA09      Nucl.Phys. A480, 323 (1988)

K.Katori, T.Shimoda, T.Fukuda, S.Shimoura, A.Sakaguchi, M.Tanaka, T.Yamagata, N.Takahashi, H.Ogata, M.Kamimura, Y.Sakuragi

Breakup Effects of 6,7Li on Elastic and Inelastic Scattering from 12C at 18-28 MeV/Nucleon

NUCLEAR REACTIONS 12C(6Li, 6Li), (6Li, 6Li'), E=123.5, 168.6 MeV; 12C(7Li, 7Li), (7Li, 7Li'), E=131.8 MeV; measured σ(θ); deduced reaction mechanism. Double-folding model, coupled-discretized continuum channels model.

doi: 10.1016/0375-9474(88)90400-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1229.


1988SA10      Nucl.Phys. A480, 361 (1988)

Y.Sakuragi, M.Yahiro, M.Kamimura, M.Tanifuji

Effects of Projectile Breakup and Target Excitation in Scattering of Polarized 7Li

NUCLEAR REACTIONS 12C(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=21 MeV; 26Mg(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=44 MeV; analyzed σ(θ), vector, tensor analyzing power. Projectile breakup, double folding interaction, coupled-channels.

doi: 10.1016/0375-9474(88)90402-2
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1988SA15      Phys.Lett. 205B, 204 (1988)

Y.Sakuragi, M.Kamimura, K.Katori

Effects of 6Li → α + d and 12C → 3α Breakup Processes in 6Li + 12C Scattering

NUCLEAR REACTIONS 12C(6Li, 6Li), (6Li, 6Li'), E=124, 169 MeV; analyzed σ(θ); deduced projectile, target breakup role. Coupled discretized continuum channels.

doi: 10.1016/0370-2693(88)91650-4
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1987SA04      Nucl.Phys. A462, 173 (1987)

Y.Sakuragi, M.Yahiro, M.Kamimura, M.Tanifuji

Scattering of Polarized 7Li by 120Sn and Projectile-Target Spin-Dependent Interactions

NUCLEAR REACTIONS 120Sn(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=44 MeV; 58Ni(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=20.3 MeV; calculated σ(θ), analyzing powers, form factors; deduced spin-orbit interaction, projectile virtual excitation effects, invariant amplitudes vs tensor interactions. Coupled-channels model, cluster-, double-folding interactions.

doi: 10.1016/0375-9474(87)90385-X
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1987TA21      Phys.Rev. C36, 2146 (1987)

M.Tanaka, T.Yamagata, S.Nakayama, M.Inoue, Y.Sakuragi, M.Kamimura, K.Goto, K.Katori, M.Yanagi, H.Ogata

Observation of Vector Analyzing Power in Elastic Scattering of 150-MeV 6Li on 12C

NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), E=150 MeV; measured σ(θ), left-right asymmetry; deduced iT11(θ). Cluster folding coupled channel calculations, projectile excitations.

doi: 10.1103/PhysRevC.36.2146
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1132.


1987YA06      Nucl.Phys. A463, 435c (1987)

M.Yahiro, Y.Iseri, H.Kameyama, M.Kamimura, M.Kawai, M.Tanifuji

Deuteron Breakup Effects on Deuteron Elastic Scattering

NUCLEAR REACTIONS 58Ni, 208Pb(polarized d, d), E=56, 400 MeV; calculated σ(θ), analyzing powers; deduced deuteron breakup effects. Coupled discretized continuum channels method.

doi: 10.1016/0375-9474(87)90687-7
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1986SA15      Phys.Lett. 175B, 105 (1986)

Y.Sakuragi, M.Kamimura, M.Yahiro, M.Tanifuji

Roles of Folding Spin-Orbit Potentials in 6,7Li(pol) Scattering

NUCLEAR REACTIONS 12C(polarized 7Li, 7Li), E=21.1 MeV; analyzed iT11(θ). 120Sn(polarized 7Li, 7Li), E=44 MeV; calculated σ(θ), vector analyzing power vs θ; deduced folding spin-orbit potentials role.

doi: 10.1016/0370-2693(86)90696-9
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1986YA11      Phys.Lett. 182B, 135 (1986)

M.Yahiro, H.Kameyama, Y.Iseri, M.Kamimura, M.Kawai

Coupled-Channel Approach to Deuteron Elastic Scattering at Intermediate Energy

NUCLEAR REACTIONS 40Ca(polarized p, p), E=200 MeV; analyzed σ(θ), analyzing power vs θ; deduced proton optical potentials; 58Ni(polarized d, d), E=400 MeV; calculated σ(θ), vector, tensor analyzing powers. Coupled channels method.

doi: 10.1016/0370-2693(86)91563-7
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1985KU23      Phys.Lett. 163B, 75 (1985)

S.Kubono, M.Sugitani, M.H.Tanaka, K.Morita, Y.Sakuragi, M.Kamimura

3α-Breakup Induced Dynamical Polarization Potential of 12C at E/A ≥ 10 MeV

NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=139.5, 158.8 MeV; measured σ(θ); deduced breakup process role. 12C level deduced α-breakup. Coupled-channels analysis.

doi: 10.1016/0370-2693(85)90195-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1188.


1985NA05      Prog.Theor.Phys.(Kyoto) 73, 512 (1985)

S.Nagata, M.Kamimura, N.Yamaguchi

On a Calculational Method of Folding Model Potential with Density-Dependent Effective Interactions

NUCLEAR REACTIONS 40Ca(α, α), E=141.7 MeV; calculated folding potential real part. 40Ca(p, p), E=30 MeV; calculated exchange potential real, imaginary terms. Density-dependent effective interactions.

doi: 10.1143/PTP.73.512
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1985OH01      Phys.Lett. 150B, 25 (1985)

S.Ohkubo, M.Kamimura

The Dynamically Induced Spin-Orbit Interaction of the 19F Projectile

NUCLEAR REACTIONS 28Si(19F, 19F), E=60 MeV; calculated σ(θ), P(θ); deduced spin-orbit potential dynamical component. Coupled-channels formalism.

doi: 10.1016/0370-2693(85)90130-3
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1985SA13      Phys.Lett. 153B, 372 (1985)

Y.Sakuragi, M.Kamimura, M.Yahiro, M.Tanifuji

Folding Interactions in the Scattering of Soft Heavy Ions by Light Nuclei

NUCLEAR REACTIONS 12C(polarized 7Li, 7Li), E=21.1 MeV; 16O(polarized 6Li, 6Li), E=22.8 MeV; analyzed σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced Coulomb barrier, reaction mechanism dependences. Coupled-channels method.

doi: 10.1016/0370-2693(85)90475-7
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1985SA36      Z.Phys. A322, 627 (1985)

Y.Sakuragi, M.Kamimura, S.Micek, H.Rebel, H.J.Gils

6Li Break-Up Effect on Elastic and Inelastic Scattering of 6Li + 6Li at 156 MeV

NUCLEAR REACTIONS 6Li(6Li, 6Li), (6Li, 6Li'), E=156 MeV; measured σ(θ). 6Li deduced breakup channel coupling role. Coupled, discretized continuum channels model.

doi: 10.1007/BF01415144
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1984OH01      Nucl.Phys. A415, 271 (1984)

H.Ohnishi, M.Tanifuji, M.Kamimura, Y.Sakuragi, M.Yahiro

Tensor Interactions and Polarization Phenomena in Heavy-Ion Scattering

NUCLEAR REACTIONS 58Ni(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=14.2, 20.3 MeV; calculated σ(θ), analyzing power vs θ. Coupled-channels method, cluster-folding interactions.

doi: 10.1016/0375-9474(84)90623-7
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1984SA31      Phys.Lett. 149B, 307 (1984)

Y.Sakuragi, M.Kamimura

12C → 3α Breakup Effect on the Scattering of 16O + 12C and 13C + 12C

NUCLEAR REACTIONS 12C(16O, 16O), E=168, 216, 311 MeV; 12C(13C, 13C), E=260 MeV; calculated dynamical polarization potential, σ(θ). Microscopic α-breakup, coupled-channels method.

doi: 10.1016/0370-2693(84)90412-X
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1984YA01      Phys.Lett. 141B, 19 (1984)

M.Yahiro, Y.Iseri, M.Kamimura, M.Nakano

A Coupled-Channel Approach to Deuteron Projectile Breakup

NUCLEAR REACTIONS 12C, 51V, 118Sn(d, np), E=56 MeV; calculated σ(θn, θp, Ep), σ(breakup). Three-body model, discretized continuum coupled channels.

doi: 10.1016/0370-2693(84)90549-5
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1983SA39      Prog.Theor.Phys.(Kyoto) 70, 1047 (1983)

Y.Sakuragi, M.Yahiro, M.Kamimura

Elastic Scattering and Breakup of 6Li - A New Type of Dynamical Polarization Potential

NUCLEAR REACTIONS 4He(d, d), E(cm)=0-15 MeV; calculated phase shifts. Cluster model. 6Li(e, e), (e, e'), E not given; calculated charge form factors. 28Si(6Li, 6Li), E=99 MeV; 40Ca(6Li, 6Li), E=156 MeV; calculated σ(θ). Cluster model, projectile breakup, microscopic coupled-channels methods.

doi: 10.1143/PTP.70.1047
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1982OH09      Phys.Lett. 118B, 16 (1982)

H.Ohnishi, M.Tanifuji, M.Kamimura, M.Yahiro

Effects of Tensor Interactions and Projectile Excitations in the Scattering of 7Li

NUCLEAR REACTIONS 58Ni(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=20.3 MeV; analyzed σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced tensor interaction, projectile excitation roles. Coupled-channels method, folding model interactions.

doi: 10.1016/0370-2693(82)90592-5
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1982SA16      Prog.Theor.Phys.(Kyoto) 68, 322 (1982)

Y.Sakuragi, M.Yahiro, M.Kamimura

Projectile Breakup Effect on 6Li Elastic Scattering from 28Si and 40Ca Studied by Microscopic Coupled-Channels Method

NUCLEAR REACTIONS 40Ca(6Li, 6Li), E=156 MeV; 28Si(6Li, 6Li), E=99 MeV; calculated σ(θ); deduced projectile breakup effect. Discretized continuum, coupled-channels method, cluster model.

doi: 10.1143/PTP.68.322
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1982YA03      Prog.Theor.Phys.(Kyoto) 67, 1467 (1982)

M.Yahiro, M.Nakano, Y.Iseri, M.Kamimura

Coupled-Discretized-Continuum-Channels Method for Deuteron Breakup Reactions Based on Three-Body Model - Justification of the Method for Truncation and Discretization of the p-n Continuum -

NUCLEAR REACTIONS, ICPND 58Ni(d, d), (d, np), E=80 MeV; calculated σ(elastic), breakup σ. Coupled-channels method, continuum discretization.

doi: 10.1143/PTP.67.1467
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1981KA03      Nucl.Phys. A351, 456 (1981)

M.Kamimura

Transition Densities between the 0+1, 2+1, 4+1, 0+2, 2+2, 1-1 and 3-1 States in 12C Derived from Three-Alpha Resonating-Group Wave Functions

NUCLEAR REACTIONS 12C(e, e), E=30-750 MeV; calculated form factors. Microscopic 3 α resonating group wave function.

NUCLEAR STRUCTURE 12C; calculated multipole transition densities. Microscopic 3 α resonating group wave function.

doi: 10.1016/0375-9474(81)90182-2
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1981NO13      Prog.Theor.Phys.(Kyoto) 66, 1906 (1981)

T.Nojiri, M.Kamimura, M.Sano, M.Wakai, K.Yoro

Coupled-Channel Study of Proton Inelastic Scattering from the Second 01 State in 12C by use of the 3α Resonating-Group Wave Function

NUCLEAR REACTIONS 12C(p, p'), E=65 MeV; calculated σ(θ). Coupled-channel method, three alpha resonating group wave functions.

doi: 10.1143/PTP.66.1906
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1976MI17      Progr.Theor.Phys. 56, 583 (1976)

Y.Mito, M.Kamimura

The Generator Coordinate Method for Composite-Particle Scattering Based on the Kohn-Hulthen Variational Principle. Application to α-α, 16O-α and 16O-16O Scattering

NUCLEAR REACTIONS 4He(α, α), 16O(16O, 16O), (α, α), E(cm) ≤ 60 MeV; calculated wave functions, phase shifts. Generator coordinate method.

doi: 10.1143/PTP.56.583
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1975MA26      Progr.Theor.Phys. 53, 706 (1975)

T.Matsuse, M.Kamimura, Y.Fukushima

Study of the Alpha-Clustering Structure of 20Ne Based on the Resonating Group Method for 16O + α - Analysis of Alpha-Decay Widths and the Exchange Kernel

NUCLEAR STRUCTURE 20Ne; calculated α-clustering, levels, B(E2).

doi: 10.1143/PTP.53.706
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1973MA50      Progr.Theor.Phys. 49, 1765 (1973)

T.Matsuse, M.Kamimura

A Study of α-Widths of 20Ne Based on 16O and α-Cluster Model

NUCLEAR STRUCTURE 20Ne; calculated levels, level-width.

doi: 10.1143/PTP.49.1765
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1972KA39      Prog.Theor.Phys. 47, 1537 (1972)

M.Kamimura, T.Matsuse, K.Takada

Alpha-Like Spatial Four-Body Correlations in Light Nuclei

NUCLEAR STRUCTURE 20Ne; calculated levels; analyzed spatial correlations, higher-shell mixing effects. α-like spatial 4-body correlations.

doi: 10.1143/PTP.47.1537
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1972KA67      Progr.Theor.Phys.Suppl. 52, 282 (1972)

M.Kamimura, T.Marumori, K.Takada

Alpha-Like Four-Body Correlations and Molecular Aspects in Nuclei. Chapter VI. Many-Body Theoretical Description of Alpha-Like Four-Body Correlations

NUCLEAR STRUCTURE 19F, 20,21Ne; calculated α-cluster structure.

doi: 10.1143/PTPS.52.282
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1967KA05      Nucl.Phys. A95, 129 (1967)

M.Kamimura, K.Ikeda, A.Arima

Giant Dipole States and Excited Giant Dipole States in 12C

doi: 10.1016/0375-9474(67)90156-X
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