NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = K.Minomo Found 30 matches. 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
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
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
2016MI03 Phys.Rev. C 93, 014607 (2016), Erratum Phys.Rev. C 96, 059906 (2017) 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
2016MI13 Phys.Rev. C 93, 051601 (2016) 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
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
2016YO06 Phys.Rev. C 94, 044604 (2016) 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
2015OG03 Phys.Rev. C 92, 034616 (2015) 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
Back to query form |