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NSR database version of May 24, 2024.

Search: Author = K.Minomo

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2018AD01      Phys.Rev. C 97, 014601 (2018)

S.Adachi, T.Kawabata, K.Minomo, T.Kadoya, N.Yokota, H.Akimune, T.Baba, H.Fujimura, M.Fujiwara, Y.Funaki, T.Furuno, T.Hashimoto, K.Hatanaka, K.Inaba, Y.Ishii, M.Itoh, C.Iwamoto, K.Kawase, Y.Maeda, H.Matsubara, Y.Matsuda, H.Matsuno, T.Morimoto, H.Morita, M.Murata, T.Nanamura, I.Ou, S.Sakaguchi, Y.Sasamoto, R.Sawada, Y.Shimizu, K.Suda, A.Tamii, Y.Tameshige, M.Tsumura, M.Uchida, T.Uesaka, H.P.Yoshida, S.Yoshida

Systematic analysis of inelastic α scattering off self-conjugate A=4n nuclei

NUCLEAR REACTIONS 12C, 16O, 20Ne, 24Mg, 28Si, 40Ca(α, α), (α, α'), E=130, 386 MeV; measured Eα, Iα, elastic and inelastic σ(θ, E) using Grand Raiden (GR) magnetic spectrometer with two multiwire drift chambers and two plastic scintillation counters at the AVF cyclotron of Research Center of Nuclear Physics (RCNP), Osaka University. 12C, 16O, 20Ne, 24Mg, 28Si, 40Ca; deduced levels, J, π, L transfers, EWSR strengths of the isoscalar dipole transitions. DWBA and coupled-channel (CC) analysis of σ(θ) distributions with the density-independent (DI) and density-dependent (DD) α-nucleus interactions.

doi: 10.1103/PhysRevC.97.014601
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2635. Data from this article have been entered in the XUNDL database. For more information, click here.

2017MI16      Phys.Rev. C 96, 024609 (2017)

K.Minomo, M.Kohno, K.Yoshida, K.Ogata

Probing three-nucleon-force effects via (p, 2p) reactions

NUCLEAR REACTIONS 40Ca(p, 2p)39K, E=148.2, 150 MeV; calculated triple differential cross sections as a function of the recoil momentum of the residue, unpolarized in-medium pp cross sections as a function of the relative momentum, with and without three-nucleon-forces, and compared with experimental data. Distorted-wave impulse approximation (DWIA) formalism with a g-matrix interaction based on chiral two- and three-nucleon forces.

doi: 10.1103/PhysRevC.96.024609
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2016LE21      Prog.Theor.Exp.Phys. 2016, 083D01 (2016)

J.Lee, H.Liu, P.Doornenbal, M.Kimura, K.Minomo, K.Ogata, Y.Utsuno, N.Aoi, K.Li, M.Matsushita, H.Scheit, D.Steppenbeck, S.Takeuchi, H.Wang, H.Baba, E.Ideguchi, N.Kobayashi, Y.Kondo, S.Michimasa, T.Motobayashi, H.Sakurai, M.Takechi, Y.Togano

Asymmetry dependence of reduction factors from single-nucleon knockout of 30Ne at ∼ 230 MeV/nucleon

NUCLEAR STRUCTURE 29F, 29,30Ne; calculated structure, energy, spectroscopic factor for proton states in 29F and neutron ones in 29Ne using shell model in sd-pf model space and using AMD (Antisymmetrized Molelcular Dynamics).

NUCLEAR REACTIONS 12C(30Ne, 29F), (30Ne, 29Ne), E≈230 MeV/nucleon; measured 29F, 30Ne residues using ZeroDegree Spectrometer, Eγ, Iγ using detector array DALI2 of 186 NaI(Tl) scintillators; calculated inclusive deeply-bound one-nucleon knock-out σ using eikonal theory with wave functions, densities, spectroscopic factors from shell model and from AMD; deduced σ dependence on separation energy asymmetry and on nuclear radius parameter. Compared with data.

doi: 10.1093/ptep/ptw096
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2587.

2016MI03      Phys.Rev. C 93, 014607 (2016), Erratum Phys.Rev. C 96, 059906 (2017)

K.Minomo, M.Kohno, K.Ogata

Microscopic coupled-channels calculations of nucleus-nucleus scattering including chiral three-nucleon-force effects

NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=30, 85 MeV; 16O(16O, 16O), (16O, 16O'), E=44, 70 MeV; calculated differential σ(E, θ), for elastic and inelastic scattering with and without the chiral three-nucleon force (3NF) effects. Microscopic coupled-channels method. Comparison with experimental data.

doi: 10.1103/PhysRevC.93.014607
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2016MI13      Phys.Rev. C 93, 051601 (2016)

K.Minomo, K.Ogata

Consistency between the monopole strength of the Hoyle state determined by structural calculation and that extracted from reaction observables

NUCLEAR REACTIONS 12C(α, α), (α, α'), E=172.5, 240, 386 MeV; calculated differential σ(θ) data to the ground state and excited 0+ (Hoyle) state in 12C, and compared to experimental data. Microscopic coupled-channels method using resonating group method (RGM) transition density of 12C and Melbourne g-matrix interaction.

doi: 10.1103/PhysRevC.93.051601
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2016NE09      Phys.Rev. C 94, 044619 (2016)

Y.S.Neoh, K.Yoshida, K.Minomo, K.Ogata

Microscopic effective reaction theory for deuteron-induced reactions

NUCLEAR REACTIONS 12C, 25Mg, 27Al, 48Ti, 51V, 54Fe, 58Ni, 89Y, 90Zr, 118Sn, 159Tb, 181Ta, 197Au, 208Pb, 209Bi(d, d), E=56 MeV; 58Ni(d, d), E=21.6, 80, 200, 400 MeV; 16O(d, d), E=52 MeV; analyzed σ(θ) data; calculated σ(θ), neutron removal cross sections, decomposition of elastic breakup cross section into partial wave contributions. Continuum-discretized coupled-channels (CDCC) method, with the eikonal reaction theory (ERT). Comparison with experimental data.

doi: 10.1103/PhysRevC.94.044619
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2016YO06      Phys.Rev. C 94, 044604 (2016)

K.Yoshida, K.Minomo, K.Ogata

Investigating α clustering on the surface of 120Sn via the (p, pα) reaction, and the validity of the factorization approximation

NUCLEAR REACTIONS 120Sn(p, pα)116Cd, E=392 MeV; calculated σ(θ, E). 66Zn(p, pα)62Ni, E=101.5 MeV; calculated energy sharing cross section, α clustering on the nuclear surface. Distorted wave impulse approximation (DWIA) framework, and validity of the factorization approximation. Comparison with experimental data.

doi: 10.1103/PhysRevC.94.044604
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2015OG03      Phys.Rev. C 92, 034616 (2015)

K.Ogata, K.Yoshida, K.Minomo

Asymmetry of the parallel momentum distribution of (p, pN) reaction residues

NUCLEAR REACTIONS 1H(14O, np)13O, 1H(14O, 2p)13N, E=100, 200 MeV/nucleon; 1H(31Ne, np)30Ne, E=200 MeV/nucleon; calculated parallel momentum distributions for the residual nuclei, widths. 12C(p, 2p)11B, E=392 MeV; analyzed triple differential cross section (TDX) and compared to experimental data to test the accuracy of the eikonal DWIA model used in the calculations.

doi: 10.1103/PhysRevC.92.034616
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2015TO08      Phys.Rev. C 91, 064610 (2015)

M.Toyokawa, T.Matsumoto, K.Minomo, M.Yahiro

Microscopic approach to 3He scattering

NUCLEAR REACTIONS 58Ni, 208Pb(3He, 3He), E=30-150 MeV/nucleon; calculated differential and total reaction σ(E, θ), microscopic optical potentials; deduced projectile-breakup and spin-orbit force effects. Double single-folding (DSF) and double-folding with frozen-density approximation (DF-FDA) models by folding the Melbourne g matrix with the target density and localizing the resultant nonlocal folding potential with the Brieva-Rook method. Comparison with experimental data.

doi: 10.1103/PhysRevC.91.064610
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2015TO12      Phys.Rev. C 92, 024618 (2015), Erratum Phys.Rev. C 96, 059905 (2017)

M.Toyokawa, M.Yahiro, Ta.Matsumoto, Ko.Minomo, K.Ogata, M.Kohno

Microscopic calculations based on chiral two- and three-nucleon forces for proton- and 4He-nucleus scattering

NUCLEAR REACTIONS 40Ca, 58Ni, 208Pb(p, p'), E=65 MeV; 58Ni, 208Pb(α, α'), E=72 MeV; calculated differential σ(θ) using standard Brueckner-Hartree-Fock (BHF) method and the g-matrix folding model, the g matrix evaluated from chiral two-nucleon force (2NF) of N3LO and chiral three-nucleon force (3NF) of NNLO; deduced effects of chiral three-nucleon force (3NF) on proton and α scattering. Comparison with experimental data.

doi: 10.1103/PhysRevC.92.024618
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2015TO18      J.Phys.(London) G42, 025104 (2015); Corrigenda J.Phys.(London) G44, 079502 (2017)

M.Toyokawa, K.Minomo, M.Kohno, M.Yahiro

Roles of chiral three-nucleon forces in nucleon-nucleus scattering

NUCLEAR REACTIONS 12C, 16O, 24Mg, 40Ca, 58Ni, 90Zr, 208Pb(p, p), E=65 MeV; calculated σ(θ), vector analyzing powers. Comparison with experimental data.

doi: 10.1088/0954-3899/42/2/025104
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2014EG01      Phys.Rev. C 89, 064611 (2014)

K.Egashira, K.Minomo, M.Toyokawa, T.Matsumoto, M.Yahiro

Microscopic optical potentials for 4He scattering

NUCLEAR REACTIONS 58Ni(α, α), (α, X), E=20.5, 26, 43.12, 60, 72, 85, 96.5, 120, 174.75 MeV/nucleon; analyzed experimental differential cross section data as a function of transfer momentum, total reaction σ(E), R dependence of absolute elastic S-matrix element; deduced optical potentials. 208Pb(α, α), E=26, 34.75, 72, 85, 96.5, 120, 174.75 MeV/nucleon; analyzed experimental differential cross section data as a function of transfer momentum. Calculations performed using double-folding model with the target-density approximation (DF-TDA), frozen-density approximation (DF-FDA), and conventional nucleon-nucleus folding (NAF) model.

doi: 10.1103/PhysRevC.89.064611
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2014MI15      Phys.Rev. C 90, 027601 (2014)

K.Minomo, T.Matsumoto, K.Egashira, K.Ogata, M.Yahiro

Eikonal reaction theory for two-neutron removal reactions

NUCLEAR REACTIONS 12C, 208Pb(6He, 2nα), E=240 MeV/nucleon; 28Si(6He, 2nα), E=52 MeV/nucleon; analyzed σ for breakup, one-, and two-neutron stripping, two-neutron removal channels, total reaction σ by treating 6He as n+n+α system and four-body α+n+n+target system using Eikonal reaction theory. Comparison with Glauber model calculations, and experimental data.

doi: 10.1103/PhysRevC.90.027601
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2014MI22      Phys.Rev. C 90, 051601 (2014), Erratum Phys.Rev. C 96, 059904 (2017)

K.Minomo, M.Toyokawa, M.Kohno, M.Yahiro

Effects of a chiral three-nucleon force on nucleus-nucleus scattering

NUCLEAR REACTIONS 12C(12C, 12C), E=85 MeV/nucleon; 16C(16C, 16C), E=70 MeV/nucleon; calculated folding potential, differential σ(θ); deduced effects of next-to-next-to leading order (NNLO) chiral three-nucleon force (3NF). Brueckner-Hartree-Fock method and the g-matrix folding model. Comparison with experimental data.

doi: 10.1103/PhysRevC.90.051601
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2014TA32      Phys.Rev. C 90, 061305 (2014)

M.Takechi, S.Suzuki, D.Nishimura, M.Fukuda, T.Ohtsubo, M.Nagashima, T.Suzuki, T.Yamaguchi, A.Ozawa, T.Moriguchi, H.Ohishi, T.Sumikama, H.Geissel, N.Aoi, R.-J.Chen, D.-Q.Fang, N.Fukuda, S.Fukuoka, H.Furuki, N.Inabe, Y.Ishibashi, T.Itoh, T.Izumikawa, D.Kameda, T.Kubo, M.Lantz, C.S.Lee, Y.-G.Ma, K.Matsuta, M.Mihara, S.Momota, D.Nagae, R.Nishikiori, T.Niwa, T.Ohnishi, K.Okumura, M.Ohtake, T.Ogura, H.Sakurai, K.Sato, Y.Shimbara, H.Suzuki, H.Takeda, S.Takeuchi, K.Tanaka, M.Tanaka, H.Uenishi, M.Winkler, Y.Yanagisawa, S.Watanabe, K.Minomo, S.Tagami, M.Shimada, M.Kimura, T.Matsumoto, Y.R.Shimizu, M.Yahiro

Evidence of halo structure in 37Mg observed via reaction cross sections and intruder orbitals beyond the island of inversion

NUCLEAR REACTIONS 12C(24Mg, X), (25Mg, X), (26Mg, X), (27Mg, X), (28Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), (34Mg, X), (35Mg, X), (36Mg, X), (37Mg, X), (38Mg, X), E=240 MeV/nucleon, [secondary Mg beams from 9Be(48Ca, X), E=345 MeV/nucleon primary reaction]; measured spectra and TOF of outgoing particles, precise reaction σ using BigRIPS spectrometer at RIBF-RIKEN facility. Comparison with theoretical deformation parameter β2 versus mass plot using double-folding model (DFM) calculation combined with antisymmetrized molecular dynamics (AMD) calculation. 37Mg; deduced deformed halo effect from observed enhanced cross section, comparison with DFM calculation based on the deformed Woods-Saxon (DWS) model; collapse of N=28 magic shell for neutrons.

doi: 10.1103/PhysRevC.90.061305
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2471.

2014WA14      Phys.Rev. C 89, 044610 (2014)

S.Watanabe, K.Minomo, M.Shimada, S.Tagami, M.Kimura, M.Takechi, M.Fukuda, D.Nishimura, T.Suzuki, T.Matsumoto, Y.R.Shimizu, M.Yahiro

Ground-state properties of neutron-rich Mg isotopes

NUCLEAR REACTIONS 12C(24Mg, X), (25Mg, X), (26Mg, X), (27Mg, X), (28Mg, X), (29Mg, X), (30Mg, X), (31Mg, X), (32Mg, X), (33Mg, X), (34Mg, X), (35Mg, X), (36Mg, X), (37Mg, X), (38Mg, X), E=240 MeV/nucleon; calculated reaction σ; deduced rms matter radii from reaction cross sections. Antisymmetrized molecular dynamics (AMD) with folding model and deformed Woods-Saxon model. Comparison with experimental data, and with other theoretical calculations.

NUCLEAR STRUCTURE 24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40Mg; calculated ground state binding J, π, S(n), S(2n) for 40Mg, β and γ deformation parameters, proton, neutron and matter radii, neutron skin thickness. 37Mg; calculated levels, J, π, neutron single-particle energies. Antisymmetrized molecular dynamics (AMD) with folding model and deformed Woods-Saxon model. Comparison with experimental data.

doi: 10.1103/PhysRevC.89.044610
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2014YO03      Prog.Theor.Exp.Phys. 2014, 053D03 (2014)

K.Yoshida, T.Fukui, K.Minomo, K.Ogata

Extracting the electric dipole breakup cross section of one-neutron halo nuclei from inclusive breakup observables

NUCLEAR REACTIONS 12C, 208Pb(11Be, n), (15C, n), (19C, n), (31Ne, n), E=250 MeV/nucleon; analyzed available data; calculated σ, scaling factor.

doi: 10.1093/ptep/ptu063
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2013KI08      Phys.Rev. C 88, 021602 (2013)

Y.Kikuchi, T.Matsumoto, K.Minomo, K.Ogata

Two neutron decay from the 2+1 State of 6He

NUCLEAR REACTIONS 12C(6He, 6He), E=240 MeV/nucleon; calculated the double-differential 6He breakup cross section (DDBUX), invariant mass spectra for α-n and n-n subsystems. 6He; deduced two neutron decay modes of first 2+ resonant state, simultaneous and correlated emission of two neutrons, and emission of two neutrons in opposite directions. Existence of dineutron in first 2+ state of 6He. Continuum-discretized coupled-channels (CDCC) method for formation of resonant first 2+ state in 6He, and complex-scaled solutions (CSS) of the Lippmann-Schwinger equation for its decay.

doi: 10.1103/PhysRevC.88.021602
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2013SA41      Phys.Rev. C 88, 037602 (2013)

S.Sasabe, T.Matsumoto, S.Tagami, N.Furutachi, K.Minomo, Y.R.Shimizu, M.Yahiro

Reaction mechanism in odd-even staggering of reaction cross sections

NUCLEAR REACTIONS 12C(14C, X), (15C, X), (16C, X), E=83 MeV/nucleon; calculated matter radii, reaction σ, absorption probability, odd-even staggering parameter for reaction σ. Microscopic continuum discretized coupled-channels (CDCC) method, including projectile-breakup and nuclear-medium effects. Black-sphere scattering (BSS), and pairing anti-halo effects. Comparison with experimental data.

doi: 10.1103/PhysRevC.88.037602
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2013TO16      Phys.Rev. C 88, 054602 (2013)

M.Toyokawa, K.Minomo, M.Yahiro

Mass-number and isotope dependence of local microscopic optical potentials for polarized proton scattering

NUCLEAR REACTIONS 4He, 40Ca, 208Pb(polarized p, p), E=65, 200 MeV; 6He(polarized p, p), E=71, 200 MeV; calculated σ(θ) and vector analyzing powers. 4He(p, X), E=47.9 MeV; 12C, 16O, 40Ca, 208Pb(p, X), E=65.5 MeV; 20Ne(p, X), E=47.0 MeV; 24Mg(p, X), E=48.0 MeV; 90Zr(p, X), E=60.8 MeV; calculated reaction σ. 20,21,22,23,24,25,26,27,28,29,30,31,32Ne(p, X), E=65 MeV; calculated reaction σ, mass dependence of volume integral and rms radius. 22Ne(p, p'), E=35 MeV; 30Ne(p, p'), 31Ne(p, p), E=65 MeV; calculated σ(θ). 22Ne(p, n)22F, E=35 MeV; analyzed charge exchange reaction to IAS. Investigated systematic properties of the microscopic optical potentials obtained with Melbourne g-matrix NN interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.88.054602
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2012FU07      Phys.Rev. C 86, 022801 (2012)

T.Fukui, K.Ogata, K.Minomo, M.Yahiro

Determination of the 8B(p, γ)9C reaction rate from 9C breakup

NUCLEAR REACTIONS 208Pb(9C, p8B)208Pb, E=65 MeV/nucleon; calculated breakup spectrum as a function of the relative energy between p and 8B. 12C, 27Al(9C, p8B), E=285 MeV/nucleon; calculated cross sections, asymptotic normalization coefficients (ANC). Analyzed elastic breakup of 9C. 8B(p, γ)9C; calculated astrophysical factor at zero energy. Continuum discretized coupled-channels method (CDCC), eikonal reaction theory (ERT). Comparison with experimental data.

doi: 10.1103/PhysRevC.86.022801
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2012MI01      Phys.Rev.Lett. 108, 052503 (2012)

K.Minomo, T.Sumi, M.Kimura, K.Ogata, Y.R.Shimizu, M.Yahiro

Determination of the Structure of 31Ne by a Fully Microscopic Framework

NUCLEAR REACTIONS 12C(28Ne, 28Ne'), (29Ne, 29Ne'), (30Ne, 30Ne'), (31Ne, 31Ne'), (32Ne, 32Ne'), E=240 MeV/nucleon; analyzed reaction σ. 28,29,30,31,32Ne; calculated deformed projectile density. Comparison with experimental data.

NUCLEAR STRUCTURE 28,29,30,31,32Ne; calculated J, π, deformation, neutron separation energy, ground state properties and halo structures. Comparison with experimental data.

doi: 10.1103/PhysRevLett.108.052503
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2012MI22      Prog.Theor.Phys.(Kyoto), Suppl. 196, 358 (2012)

K.Minomo, S.Watanabe, T.Sumi, M.Kimura, K.Ogata, Y.R.Shimizu, M.Yahiro

Deformation Effect on Total Reaction Cross Sections for Neutron-Rich Ne-Isotopes

NUCLEAR REACTIONS 12C(28Ne, 28Ne'), (29Ne, 29Ne'), (30Ne, 30Ne'), (31Ne, 31Ne'), (32Ne, 32Ne'), E=240 MeV/nucleon; analyzed available data. 28,29,30,31,32Ne; deduced σ using antisymmetrized molecular dynamics. Comparison with available data.

doi: 10.1143/PTPS.196.358
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2012SU09      Phys.Rev. C 85, 064613 (2012)

T.Sumi, K.Minomo, S.Tagami, M.Kimura, T.Matsumoto, K.Ogata, Y.R.Shimizu, M.Yahiro

Deformation of Ne isotopes in the region of the island of inversion

NUCLEAR REACTIONS 12C(28Ne, 28Ne), (29Ne, 29Ne), (30Ne, 30Ne), (31Ne, 31Ne), (32Ne, 32Ne), E=240 MeV/nucleon; calculated σ. 12C(12C, 12C), E=74.25, 135 MeV/nucleon; calculated σ(E, θ). Double folding model with Melbourne g-matrix interaction and the nuclear densities calculated by antisymmetrized molecular dynamics (AMD). Effects of pairing correlation. Comparison with experimental data.

NUCLEAR STRUCTURE 20,21,22,23,24,25,26,27,28,29,30,31,32Ne; calculated ground state J, π, deformation parameters β2, β4 and γ, S(n), total binding energy, matter rms radii, neutron and proton rms radii and density profiles, pairing effects on total binding energy. AMD, spherical Gogny-HF and -HFB calculations. 31Ne; halo nucleus.

doi: 10.1103/PhysRevC.85.064613
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2012WA28      Phys.Rev. C 86, 031601 (2012)

S.Watanabe, T.Matsumoto, K.Minomo, K.Ogata, M.Yahiro

Effects of four-body breakup on 6Li elastic scattering near the Coulomb barrier

NUCLEAR REACTIONS 209Bi(6Li, 6Li), E=29.9, 32.8 MeV; 209Bi(n, n), E=5 MeV; 209Bi(d, d), E=12.8 MeV; analyzed σ(θ) using three-body (d+α+209Bi) and four-body (p+n+α+209Bi) continuum-discretized coupled-channels (CDCC) model. Projectile breakup effects.

doi: 10.1103/PhysRevC.86.031601
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2012YA15      Prog.Theor.Phys.(Kyoto), Suppl. 196, 87 (2012)

M.Yahiro, T.Matsumoto, K.Minomo, T.Sumi, S.Watanabe

Recent Development of CDCC

NUCLEAR REACTIONS 208Pb(31Ne, n), (31Ne, 2n), E=234 MeV/nucleon; 12C(31Ne, n), (31Ne, 2n), E=230 MeV/nucleon; calculated partial σ. Comparison with available data.

doi: 10.1143/PTPS.196.87
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2011HA22      Phys.Rev. C 83, 054617 (2011)

S.Hashimoto, M.Yahiro, K.Ogata, K.Minomo, S.Chiba

Effective radii of deuteron-induced reactions

NUCLEAR REACTIONS 9Be, 27Al, 58Ni, 93Nb, 208Pb(d, X), E=200 MeV/nucleon; 7Li(d, n), E=40 MeV; calculated cross sections, σ(θ), effective radius and width, proton and neutron stripping, elastic breakup, total fusion. Continuum-discretized coupled-channels (CDCC) method and eikonal reaction theory (ERT). Comparison with Glauber model calculations and experimental data.

doi: 10.1103/PhysRevC.83.054617
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2011MI13      Phys.Rev. C 84, 034602 (2011)

K.Minomo, T.Sumi, M.Kimura, K.Ogata, Y.R.Shimizu, M.Yahiro

Deformation effect on total reaction cross sections for neutron-rich Ne isotopes

NUCLEAR REACTIONS 12C(28Ne, X), (29Ne, X), (30Ne, X), (31Ne, X), (32Ne, X), E=240 MeV/nucleon; analyzed cross sections, and matter rms radii. Double-folding model with the Melbourne g matrix, density of the projectile from the mean-field model with the deformed Woods-Saxon potential, deformation evaluated by antisymmetrized molecular dynamics. Effect of deformation on cross section.

doi: 10.1103/PhysRevC.84.034602
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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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2008YA18      Prog.Theor.Phys.(Kyoto) 120, 767 (2008)

M.Yahiro, K.Minomo, K.Ogata, M.Kawai

A New Glauber Theory Based on Multiple Scattering Theory

NUCLEAR REACTIONS 1H(11Be, X), (40Ca, X), E=300 MeV/nucleon; calculated cross sections a reformulation of Glauber theory for intermediate energies.

doi: 10.1143/PTP.120.767
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