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NSR database version of April 11, 2024.

Search: Author = M.Yahiro

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2023WA03      Phys.Rev. C 107, 024608 (2023)

T.Wakasa, S.Tagami, J.Matsui, M.Takechi, M.Yahiro

Neutron-skin values and matter and neutron radii determined from reaction cross sections of proton scattering on 12C, 40, 48Ca, 58Ni, and 208Pb

NUCLEAR REACTIONS 12C, 40,48Ca, 58Ni, 208Pb(p, p), E=20-180 MeV; calculated proton-, neutron-, and matter densities; analyzed reaction σ(E) from proton scattering data; deduced matter radii, neutron radii and neutron skin thickness.Kyushu g-matrix folding model with the densities scaled from the Gogny-D1S HFB (GHFB) with angular momentum projection (AMP). Comparison of obtained values for neutron skin thickness to the data obtained by different methods.

doi: 10.1103/PhysRevC.107.024608
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2021IS06      Phys.Rev. C 103, 044605 (2021)

M.Ishii, Y.Iseri, M.Yahiro

Prediction of the analyzing power for p(pol) + 6He elastic scattering at 200 MeV from p(pol) + 4He elastic scattering at 200 MeV

NUCLEAR REACTIONS 4,6He(polarized p, p), E=71, 72, 200 MeV; analyzed experimental data for differential σ(E, θ), Ay(E, θ) and form factor F(Q) versus Q using improved valence-target-cutting (VTC) theory and cluster-folding (CF) model.

doi: 10.1103/PhysRevC.103.044605
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2021MA74      Phys.Rev. C 104, 054613 (2021)

M.Matsuzaki, S.Tagami, M.Yahiro

Neutron skin thickness of 208Pb, 116, 120, 124Sn, and 40Ca determined from reaction cross sections of 4He scattering

NUCLEAR REACTIONS 208Pb, 116,120,124Sn, 40Ca(α, X), E=20-50 MeV/nucleon; calculated reaction σ(E), nuclear matter radii, neutron skin thicknesses using double folding model with Kyushu chiral g matrix, and densities from mean-field calculations, further renormalized densities to reproduce observed σ(E), and with D1S-GHFB+AMP and SLy7-HFB Skyrme interactions. Comparison with experimental neutron skin thickness of 208Pb from electron scattering data by PREX-II collaboration, and with other experimental data.

doi: 10.1103/PhysRevC.104.054613
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2021TA25      Phys.Rev. C 104, 024606 (2021)

S.Tagami, T.Wakasa, J.Matsui, M.Yahiro, M.Takechi

Neutron skin thickness of 208Pb determined from the reaction cross section for proton scattering

NUCLEAR REACTIONS 208Pb(p, X), E=30-100 MeV; calculated proton-, neutron-, and matter densities; analyzed reaction σ(E) from proton scattering data; deduced neutron radius and neutron skin thickness. Kyushu g-matrix folding model with the densities calculated with Gogny-D1S HFB (GHFB) with the angular momentum projection (AMP).

doi: 10.1103/PhysRevC.104.024606
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2020TA01      Phys.Rev. C 101, 014620 (2020)

S.Tagami, M.Tanaka, M.Takechi, M.Fukuda, M.Yahiro

Chiral g-matrix folding-model approach to reaction cross sections for scattering of Ca isotopes on a C target

NUCLEAR STRUCTURE 40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57,58,59,60,62,64Ca; calculated β and γ deformation parameters, even and odd driplines, binding energies, charge, proton, neutron and matter radii, neutron skin for the ground states using Gogny-D1S Hartree-Fock-Bogoliubov (GHFB) theory with and without the angular momentum projection (AMP). Comparison with experimental data.

NUCLEAR REACTIONS 12C(40Ca, X), (41Ca, X), (42Ca, X), (43Ca, X), (44Ca, X), (45Ca, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (51Ca, X), (52Ca, X), (53Ca, X), (54Ca, X), (55Ca, X), (56Ca, X), (57Ca, X), (58Ca, X), (59Ca, X), (60Ca, X), (62Ca, X), (64Ca, X), E=280, 250.7 MeV; calculated reaction σ(E) using chiral g-matrix double-folding model (DFM), and compared with GHFB+AMP density, and available experimental data. 9Be, 12C, 27Al(12C, X), E=30-400 MeV; calculated reaction σ(E) using chiral g-matrix double-folding model (DFM). Comparison with results from t-matrix DFM densities, and experimental data.

doi: 10.1103/PhysRevC.101.014620
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2019GU07      Phys.Rev. C 99, 034602 (2019)

H.Guo, Y.Watanabe, T.Matsumoto, K.Nagaoka, K.Ogata, M.Yahiro

Analysis of nucleon and triton emissions from nucleon-7Li collisions below 20 MeV

NUCLEAR REACTIONS 7Li(n, n), (n, n'), E=4.08, 5.1, 6.1, 6.97, 7.97, 9, 10, 11, 12, 13, 14, 15.4, 18 MeV; calculated σ(θ, E) and compared with experimental data. 7Li(p, t), E=14 MeV; 7Li(n, t), E=11.5, 14, 14.2, 18 MeV; calculated t-α scattering phase shifts, double-differential σ(E, θ) of break-up and reaction channels, and integrated neutron induced σ using continuum discretized coupled-channels (CDCC) method, final-state interaction model, and sequential decay model. Comparison with experimental and evaluated data.

doi: 10.1103/PhysRevC.99.034602
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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
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2016SH21      Phys.Rev. C 93, 064314 (2016)

M.Shimada, S.Watanabe, S.Tagami, T.Matsumoto, Y.R.Shimizu, M.Yahiro

Simultaneous analysis of matter radii, transition probabilities, and excitation energies of Mg isotopes by angular-momentum-projected configuration-mixing calculations

NUCLEAR STRUCTURE 24,26,28,30,32,34,36,38,40Mg; calculated potential-energy curves, level energies, rms matter radii, B(E2), β2, and probability distributions for the first 2+ and 4+ states. Beyond-mean-field (BMF) calculations with angular-momentum-projected configuration mixing with respect to the axially symmetric β2 deformation. Comparison with experimental data.

doi: 10.1103/PhysRevC.93.064314
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2016YA05      Phys.Rev. C 93, 064609 (2016)

M.Yahiro, S.Watanabe, M.Toyokawa, T.Matsumoto

Proposal of a directly measurable parameter quantifying the halo nature of one-neutron nuclei

NUCLEAR REACTIONS 12C(p, X), (15C, X), (31Ne, X), E<1000 MeV; analyzed reaction σ(E) data to determine halo parameters. 11Be, 12,15,17,19C, 31Ne, 37Mg; deduced halo parameters. Calculations based on the eikonal+adiabatic approximation using Glauber formula.

doi: 10.1103/PhysRevC.93.064609
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2015FU01      Phys.Rev. C 91, 014604 (2015)

T.Fukui, K.Ogata, M.Yahiro

Breakup and finite-range effects on the 8B (d, n) 9C reaction

NUCLEAR REACTIONS 8B(d, n)9C, E=14.4 MeV/nucleon; analyzed σ as function of neutron emission angle, breakup effects of d and 9C on the cross section. 8B(p, γ)9C; deduced asymptotic normalization coefficient (ANC), astrophysical S18(0) factor at zero energy. Interference between Elastic transfer (ET) and breakup transfer (BT). Three body continuum discretized coupled-channels (CDCC) Born approximation.

doi: 10.1103/PhysRevC.91.014604
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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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2015WA32      Phys.Rev. C 92, 044611 (2015)

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

Four-body dynamics in 6Li elastic scattering

NUCLEAR REACTIONS 209Bi(6Li, X), E=24-50 MeV; 208Pb(6Li, X), E(cm)=29-210 MeV; calculated σ(θ, E), total σ(E), distribution of dα probability in excitation spectrum, Dominant d+α channel for 6Li breakup in elastic scattering. Four-body (n+p+α+target) model of the continuum-discretized coupled channels method (CDCC). Comparison to experimental data.

doi: 10.1103/PhysRevC.92.044611
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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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2014GU12      Nucl.Data Sheets 118, 254 (2014)

H.Guo, K.Nagaoka, Y.Watanabe, T.Matsumoto, K.Ogata, M.Yahiro

Application of the Continuum Discretized Coupled Channels Method to Nucleon-induced Reactions on 6, 7Li for Energies up to 150 MeV

NUCLEAR REACTIONS 6Li(p, x), E=5-150 MeV; calculated reaction σ. 6Li(n, n'), E=14.1 MeV;7Li(p, p'), E=5-50 MeV;7Li(p, p'), (p, t), E=14 MeV; calculated σ(Eout, θ). CDCC with folding of complex JLM effective nucleon-nucleon forces. Compared with available data.

doi: 10.1016/j.nds.2014.04.051
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2014MA79      Phys.Rev. C 90, 041602 (2014)

T.Matsumoto, M.Yahiro

Antihalo effects on reaction cross sections for 14, 15, 16C isotopes

NUCLEAR REACTIONS 12C(14C, X), (15C, X), (16C, X), E=83 MeV/nucleon; analyzed reaction cross sections, spectroscopic factors using the Melbourne g-matrix double-folding model. Investigated antihalo effects on reaction σ and projectile breakup effect on the mass-number dependence with the continuum-discretized coupled-channel method.

doi: 10.1103/PhysRevC.90.041602
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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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2013GU06      Phys.Rev. C 87, 024610 (2013)

H.Guo, Y.Watanabe, T.Matsumoto, K.Ogata, M.Yahiro

Systematic analysis of nucleon scattering from 6, 7Li with the continuum discretized coupled channels method

NUCLEAR REACTIONS 6,7Li(n, n), (n, n'), (p, p), (p, p'), E=0-150 MeV; analyzed total σ(E), reaction σ(E), σ(θ, E). Continuum discretized coupled channels method (CDCC).

doi: 10.1103/PhysRevC.87.024610
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2013OG06      Phys.Rev. C 88, 024616 (2013)

K.Ogata, T.Myo, T.Furumoto, T.Matsumoto, M.Yahiro

Interplay between the 02+ resonance and the nonresonant continuum of the drip-line two-neutron halo nucleus 22C

NUCLEAR REACTIONS 12C(22C, X), E=250 MeV/nucleon; calculated double differential breakup cross section, breakup energy distribution for low-lying resonances and non-resonant continuum. Four-body continuum-discretized coupled-channels (CCDC) method with the cluster-orbital shell model (COSM) wave functions.

doi: 10.1103/PhysRevC.88.024616
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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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2011YE05      J.Korean Phys.Soc. 59, 871s (2011)

T.Ye, S.Hashimoto, Y.Watanabe, K.Ogata, M.Yahiro

Analysis of Inclusive (d, χn) and (d, χp) Reactions for Energies up to 100 MeV

NUCLEAR REACTIONS 9Be, 12C, 27Al, 58Ni, 93Nb, 181Ta, 208Pb, 238U(d, xp), E=100 MeV; calculated σ(θ=80, Ep); 58Ni(d, xp), E=100 MeV; calculated σ(Ep, θ=6, 8, 10, 12, 15, 200); 7Li(d, xn), E=25 MeV; calculated σ(En, θ-0, 5, 10, 150). CDCC plus Glauber model with and without Coulomb breakup. Comparison with data.

doi: 10.3938/jkps.59.871
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2011YE06      Phys.Rev. C 84, 054606 (2011)

T.Ye, S.Hashimoto, Y.Watanabe, K.Ogata, M.Yahiro

Analysis of inclusive (d, xp) reactions on nuclei from 9Be to 238U at 100 MeV

NUCLEAR REACTIONS 9Be, 12C, 27Al, 58Ni, 93Nb, 181Ta, 208Pb, 238U(d, xp), E=100 MeV; analyzed double-differential cross sections as function of proton energy and proton emission angle, energy integrated proton angular distributions, total-proton-production cross sections as function of the atomic number Z. Comparison of CDCC calculations with and without Coulomb breakup of deuteron. Continuum discretized coupled-channels (CDCC) theory and the Glauber model.

doi: 10.1103/PhysRevC.84.054606
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2010MA61      Phys.Rev. C 82, 051602 (2010)

T.Matsumoto, K.Kato, M.Yahiro

New description of the four-body breakup reaction

NUCLEAR REACTIONS 58Ni(d, np), E=80 MeV; 12C(6He, 2nα), E=229.8, 240 MeV; 208Pb(6He, 2nα), E=240 MeV/Nucleon; calculated break-up cross sections and σ(θ). Continuum discretized coupled-channel (CDCC) method. Comparison with experimental data.

doi: 10.1103/PhysRevC.82.051602
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2009EG01      Prog.Theor.Phys.(Kyoto) 121, 789 (2009)

T.Egami, T.Matsumoto, K.Ogata, M.Yahiro

Description of Four-Body Breakup Reaction with the Method of Continuum-Discretized Coupled-Channels

doi: 10.1143/PTP.121.789
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2009OG04      J.Phys.Soc.Jpn. 78, 084201 (2009)

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

Properties of Nuclear and Coulomb Breakup of 8B

NUCLEAR REACTIONS 12C, 16O, 40Ca, 58Ni, 90Zr, 152Sm, 208Pb(8B, p7Be), E=65 MeV/nucleon; calculated dependence of breakup σ on target mass; deduced nuclear-Coulomb interference. Continuum-discretized coupled-channels (CDCC) method.

doi: 10.1143/JPSJ.78.084201
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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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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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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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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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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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2003IC02      Nucl.Phys. A718, 383c (2003)

K.Ichiki, M.Yahiro, T.Kajino, M.Orito, G.J.Mathews

Constraints on the Nature of Cosmological Constant - from Big Bang Nucleosynthesis and CMB anisotropies -

doi: 10.1016/S0375-9474(03)00805-4
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2003IC03      Nucl.Phys. A718, 386c (2003)

K.Ichiki, M.Yahiro, T.Kajino, M.Orito, G.J.Mathews

Observational Constraints on Dark Radiation in Brane Cosmology

doi: 10.1016/S0375-9474(03)00811-X
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2003MA43      Nucl.Phys. A718, 15c (2003)

G.J.Mathews, K.Ichiki, T.Kajino, M.Orito, M.Yahiro

New Paradigms for Primordial Nucleosynthesis

doi: 10.1016/S0375-9474(03)00674-2
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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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2003OR02      Nucl.Phys. A719, 1c (2003)

M.Orito, T.Kajino, K.Ichiki, M.Yahiro, G.J.Mathews, Y.Wang

BBN and CMB constraints on universal lepton asymmetry, quintessential inflation, and brane world cosmology

doi: 10.1016/S0375-9474(03)00950-3
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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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1996AU02      Phys.Rev. C53, 314 (1996)

N.Austern, M.Kawai, M.Yahiro

Three-Body Reaction Theory in a Model Space

doi: 10.1103/PhysRevC.53.314
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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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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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1989YA01      Phys.Rev.Lett. 62, 133 (1989)

M.Yahiro, J.A.Tostevin, R.C.Johnson

Three-Body Treatment of the Final State in the (3He, pp) Reaction on Medium-Mass Nuclei

NUCLEAR REACTIONS 28Si(polarized 3He, 2p), E=33, 52 MeV; analyzed σ(θ), analyzing power vs E(2p). Three-body approach to final state.

doi: 10.1103/PhysRevLett.62.133
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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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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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1987KA42      Phys.Lett. 199B, 21 (1987)

H.Kameyama, M.Yahiro

Relativistic Dynamics of Deuteron-Nucleus Scattering at Intermediate Energies

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

doi: 10.1016/0370-2693(87)91456-0
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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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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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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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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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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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1983IS06      Prog.Theor.Phys.(Kyoto) 69, 1038 (1983)

Y.Iseri, M.Yahiro, M.Nakano

Investigation of Adiabatic Approximation of Deuteron-Breakup Effect on (d, p) Reactions

NUCLEAR REACTIONS 58Ni(d, d), (d, p), E=80 MeV; analyzed σ(θ); deduced adiabatic approximation limitation, breakup wave function role.

doi: 10.1143/PTP.69.1038
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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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