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NSR database version of April 11, 2024.

Search: Author = Y.Sakuragi

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2021OG03      Prog.Theor.Exp.Phys. 2021, 103D01 (2021)

K.Ogata, Y.Chiba, Y.Sakuragi

Correspondence between isoscalar monopole strengths and α inelastic cross sections on 24Mg

NUCLEAR REACTIONS 24Mg(α, α'), E=130, 386 MeV; analyzed available data; calculated σ(θ), transition strengths using antisymmetrized molecular dynamics (AMD). Microscopic coupled-channel framework.

doi: 10.1093/ptep/ptab112
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2019SA48      Prog.Theor.Exp.Phys. 109, 101D01 (2019)

K.Sato, T.Furumoto, Y.Kikuchi, K.Ogata, Y.Sakuragi

Large-amplitude quadrupole shape mixing probed by the (p, p') reaction: A model analysis

NUCLEAR REACTIONS 154Sm(p, p'), E=35, 65, 66.5 MeV; calculated σ(θ). Comparison with experimental results.

doi: 10.1093/ptep/ptz095
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2017QU02      Phys.Rev. C 95, 044616 (2017)

W.W.Qu, G.L.Zhang, S.Terashima, T.Furumoto, Y.Ayyad, Z.Q.Chen, C.L.Guo, A.Inoue, X.Y.Le, H.J.Ong, D.Y.Pang, H.Sakaguchi, Y.Sakuragi, B.H.Sun, A.Tamii, I.Tanihata, T.F.Wang, R.Wada, Y.Yamamoto

Repulsive three-body force and channel-coupling effects via 12C+12C scattering at 100A MeV

NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=100 MeV/nucleon; measured scattered 12C using Grand Raiden high-resolution magnetic spectrometer, and 10B, 11C and other particles by the energy loss and time-of-flight (TOF) information, differential cross sections for the ground state, 4.44 MeV, 2+ state, and the sum of the 7.65 MeV, 0+ and the 9.64 MeV, 3- states in 12C using the Ring Cyclotron facility at RCNP-Osaka. Comparison with microscopic coupled-channel calculations, using the double folding method with three different complex G-matrix interactions, the ESC, CEG07b, and MPa.

doi: 10.1103/PhysRevC.95.044616
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2546.


2016FU01      Acta Phys.Pol. B47, 853 (2016)

T.Furumoto, Y.Sakuragi, Y.Yamamoto

Approach to High-density Nuclear Matter via Nucleus-Nucleus Elastic Scattering

NUCLEAR REACTIONS 16O(16O, 16O), E=70 MeV/nucleon; analyzed available data; calculated σ.

doi: 10.5506/APhysPolB.47.853
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2016FU13      Phys.Rev. C 94, 044620 (2016)

T.Furumoto, Y.Sakuragi, Y.Yamamoto

Medium effect in high-density nuclear matter probed by a systematic analysis of nucleus-nucleus elastic scattering

NUCLEAR REACTIONS 16O(16O, 16O), (16O, X), E=70 MeV/nucleon; calculated real and imaginary parts of the double-folding (DF) potential, σ(θ) for elastic scattering and total reaction σ using different interactions. 12C, 28Si, 40Ca, 90Zr, 208Pb(16O, 16O), E=93.9 MeV/nucleon; 12C(12C, 12C), E=84.7, 100, 120.75, 135, 200, 300, 400 MeV; calculated σ(θ). Double-folding (DF) potential with the complex G-matrix interaction including three-body-force (TBF) effect based on multi-Pomeron exchange potential (MPP) model. Comparison with experimental data.

doi: 10.1103/PhysRevC.94.044620
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2015QU02      Phys.Lett. B 751, 1 (2015)

W.W.Qu, G.L.Zhang, S.Terashima, T.Furumoto, Y.Ayyad, Z.Q.Chen, C.L.Guo, A.Inoue, X.Y.Le, H.J.Ong, D.Y.Pang, H.Sakaguchi, Y.Sakuragi, B.H.Sun, A.Tamii, I.Tanihata, T.F.Wang, R.Wada, Y.Yamamoto

Effects of repulsive three-body force in 12C + 12C scattering at 100A MeV

NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=100 MeV/nucleon; measured reaction products; deduced σ(θ). Three double-folding models with complex G-matrix interactions, the CEG07b, MPa, and ESC model calculations.

doi: 10.1016/j.physletb.2015.10.008
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2494.


2014FU09      Phys.Rev. C 90, 041601 (2014)

T.Furumoto, Y.Sakuragi, Y.Yamamoto

Medium effect in the high-density region probed by nucleus-nucleus elastic scattering

NUCLEAR REACTIONS 16O(16O, 16O), E=70 MeV/nucleon; calculated double-folding potential dependency on density, elastic σ(θ) using double-folding model with the complex G-matrix interaction and three-body-force (TBF) effect. Investigated medium effect dependency on density. Comparison with experimental results.

doi: 10.1103/PhysRevC.90.041601
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2013FU01      Phys.Rev. C 87, 014618 (2013)

T.Furumoto, Y.Sakuragi

Channel coupling effect and important role of imaginary part of coupling potential for high-energy heavy-ion scatterings

NUCLEAR REACTIONS 12C(12C, X), (12C, 12C), E=100-400 MeV/nucleon, calculated folding potential, coupling potential, elastic σ(E), dynamical polarization potential, inelastic σ(E). Microscopic coupled channel (MCC) method using the complex G-matrix interaction CEG07.

doi: 10.1103/PhysRevC.87.014618
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2012FU04      Phys.Rev. C 85, 044607 (2012); Erratum Phys.Rev. C 85, 069901 (2012)

T.Furumoto, W.Horiuchi, M.Takashina, Y.Yamamoto, Y.Sakuragi

Global optical potential for nucleus-nucleus systems from 50 MeV/u to 400 MeV/u

NUCLEAR REACTIONS 16O(16O, 16O), E=21.9, 30, 44, 70 MeV/nucleon; 12C(16O, 16O), E=20.6, 38, 93.9 MeV/nucleon; 12C(12C, 12C), E=25, 30, 84.7, 120.75, 135, 200 MeV/nucleon; 28Si, 40Ca, 208Pb(16O, 16O), E=93.9 MeV/nucleon; 60Ni, 120Sn, 208Pb(40Ar, 40Ar), E=44 MeV/nucleon; 40Ca(14C, 14C), (16C, 16C), (18C, 18C), (20C, 20C), (22C, 22C)(18O, 18O), (20O, 20O), (22O, 22O), (24O, 24O), E=100 MeV/nucleon; 40Ca(30Ne, 30Ne), (70Ca, 70Ca), E=100, 200, 300, 400 MeV/nucleon; calculated folding-model potentials (FMPs) elastic scattering cross sections as a function of momentum transfer. New global optical potential (GOP) in 50-400 MeV/nucleon range from microscopic CEG07 folding model with Sao Paulo density. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.044607
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2012FU09      Prog.Theor.Phys.(Kyoto), Suppl. 196, 219 (2012)

T.Furumoto, Y.Sakuragi, Y.Yamamoto

Dynamical Evolution of Heavy-Ion Scattering in the High-Energy Region

NUCLEAR REACTIONS 12C(12C, 12C), E=100, 200, 300, 400 MeV; calculated Rutherford ratio of elastic σ, σ(θ); deduced dynamical polarization potential.

doi: 10.1143/PTPS.196.219
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2012FU13      J.Phys.:Conf.Ser. 381, 012092 (2012)

T.Furumoto, Y.Sakuragi, Y.Yamamoto

Prediction of repulsive potential for high-energy heavy-ion scatterings

NUCLEAR REACTIONS 12C(12C, 12C), E=100, 200, 300, 400 MeV/nucleon; calculated σ(q) and its decomposition into near- and far-side using DFM (double-folding model) potentials with G-matrix NN interactions CEG07.

doi: 10.1088/1742-6596/381/1/012092
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2011FU16      J.Phys.:Conf.Ser. 312, 082022 (2011)

T.Furumoto, Y.Sakuragi, Y.Yamamoto

Role of Three-Body Forces in Proton and Heavy-Ion Scatterings

NUCLEAR REACTIONS 12C(p, p), E=122 MeV; calculated σ(θ), analyzing power. 12C, 28Si, 40Ca(16O, 16O), E=93.9 MeV/nucleon;16O(16O, 16O), E=70 MeV/nucleon;12C(12C, 12C), E=135 MeV/nucleon; calculated σ(θ). Complex G-matrix CEG-07 with three-body forces. Compared with data.

doi: 10.1088/1742-6596/312/4/082022
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2010FU12      Phys.Rev. C 82, 044612 (2010)

T.Furumoto, Y.Sakuragi, Y.Yamamoto

Repulsive nature of optical potentials for high-energy heavy-ion scattering

NUCLEAR REACTIONS 12C(12C, 12C), 16O(16O, 16O), E=100, 200, 300, 400 MeV/nucleon; calculated differential σ, σ(θ), and potential energies using double-folding model (DFM) with complex G-matrix interaction.

doi: 10.1103/PhysRevC.82.044612
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2010FU14      Nucl.Phys. A835, 362c (2010)

T.Furumoto, Y.Sakuragi, Y.Yamamoto

Hyperon-nucleus folding potentials in the complex G-matrix approach

NUCLEAR REACTIONS 28Si(Σ0, Σ0), E=50-200 MeV; calculated σ(θ), analyzing power using G-matrix models ESC08 (Extended Soft-Core Model) and ESC04a.

doi: 10.1016/j.nuclphysa.2010.01.219
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2010HO08      Phys.Rev. C 81, 061602 (2010)

K.Horii, M.Takashina, T.Furumoto, Y.Sakuragi, H.Toki

Elastic scattering of 8B from 12C with internal three-cluster structure of 8B

NUCLEAR REACTIONS 12C(8B, 8B), E=95 MeV; calculated σ, σ(θ) using adiabatic recoil and cluster folding calculations. 12C, 14N(7Be, 7Be), E=87 MeV; calculated σ(θ). Comparison with experimental data.

doi: 10.1103/PhysRevC.81.061602
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2010TA06      Phys.Rev. C 81, 047605 (2010)

M.Takashina, T.Furumoto, Y.Sakuragi

16O+16O inelastic scattering studied by a complex G-matrix interaction

NUCLEAR REACTIONS 16O(16O, 16O'), E=1120 MeV; analyzed σ(θ) using microscopic coupled-channel (CC) method with complex G-matrix interaction.

doi: 10.1103/PhysRevC.81.047605
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2009EL03      Phys.Rev. C 79, 011302 (2009)

Z.Elekes, Zs.Dombradi, T.Aiba, N.Aoi, H.Baba, D.Bemmerer, B.A.Brown, T.Furumoto, Zs.Fulop, N.Iwasa, A.Kiss, T.Kobayashi, Y.Kondo, T.Motobayashi, T.Nakabayashi, T.Nannichi, Y.Sakuragi, H.Sakurai, D.Sohler, M.Takashina, S.Takeuchi, K.Tanaka, Y.Togano, K.Yamada, M.Yamaguchi, K.Yoneda

Persistent decoupling of valence neutrons toward the dripline: Study of 20C by γ spectroscopy

NUCLEAR REACTIONS 208Pb(20C, 20C'), E=37.6 MeV/nucleon; 1H(20C, 20C'), E=41.4 MeV/nucleon; measured Eγ, Iγ. 20C; deduced levels, J, π, charge and neutron transition probabilities, B(E2). Comparison with shell model calculations.

doi: 10.1103/PhysRevC.79.011302
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2399. Data from this article have been entered in the XUNDL database. For more information, click here.


2009FU01      Phys.Rev. C 79, 011601 (2009)

T.Furumoto, Y.Sakuragi, Y.Yamamoto

Three-body-force effect on nucleus-nucleus elastic scattering

NUCLEAR REACTIONS 16O(16O, 16O), E=70 MeV/nucleon; calculated σ(θ). Three-body force. Comparison with experimental data.

doi: 10.1103/PhysRevC.79.011601
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2009FU11      Phys.Rev. C 80, 044614 (2009); Erratum Phys.Rev. C 82, 029908 (2010)

T.Furumoto, Y.Sakuragi, Y.Yamamoto

Effect of repulsive and attractive three-body forces on nucleus-nucleus elastic scattering

NUCLEAR REACTIONS 16O(16O, 16O), E=21.875, 70, 100, 200, 300, 400 MeV/nucleon; 12C, 28Si, 40Ca(16O, 16O), E=93.9 MeV/nucleon; 12C(12C, 12C), E=135 MeV/nucleon; calculated σ, σ(θ), folding model potentials, and rms radii using Brueckner theory for nucleon-nucleon effective interaction in complex G-matrix formalism. Investigated the effects of the three-body force (TBF) in nucleon-nucleus elastic scattering.

doi: 10.1103/PhysRevC.80.044614
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2009TA18      Phys.Rev. C 80, 014605 (2009)

M.Takashina, Y.Sakuragi

Multistep effect in 16O+16O inelastic scattering

NUCLEAR REACTIONS 16O(16O, 16O'), E=350, 1120 MeV; analyzed σ(θ) for first 2+ and 3- states using microscopic coupled-channel calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.014605
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2008FU13      Phys.Rev. C 78, 044610 (2008)

T.Furumoto, Y.Sakuragi, Y.Yamamoto

New complex G-matrix interactions derived from two- and three-body forces and application to proton-nucleus elastic scattering

NUCLEAR REACTIONS 12C, 40Ca, 90Zr, 208Pb(p, p), E=65-200 MeV; calculated σ, σ(θ), analyzing powers, neutron densities. Complex G-matrix interactions with three-body force.

doi: 10.1103/PhysRevC.78.044610
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2006FU11      Phys.Rev. C 74, 034606 (2006)

T.Furumoto, Y.Sakuragi

Application of the Jeukenne-Lejeune-Mahaux folding model to α-nucleus elastic scattering

NUCLEAR REACTIONS 12C, 16O, 28Si, 40Ca(α, α), E ≈ 40-240 MeV; calculated σ(θ). Folding model, comparison with data.

doi: 10.1103/PhysRevC.74.034606
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2006TA27      Phys.Rev. C 74, 054606 (2006)

M.Takashina, Y.Sakuragi

α + 12C inelastic angular distribution and nuclear size of 12C(O+2)

NUCLEAR REACTIONS 12C(α, α'), E=139-240 MeV; analyzed σ(E, θ), sensitivity to excited state radius.

doi: 10.1103/PhysRevC.74.054606
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2005TA12      Phys.Rev. C 71, 054602 (2005)

M.Takashina, Y.Kanada-En'yo, Y.Sakuragi

16C inelastic scattering studied with the microscopic coupled-channels method

NUCLEAR REACTIONS 208Pb(16C, 16C'), E=52.7 MeV/nucleon; calculated σ(θ). Microscopic coupled-channels method, comparison with data.

doi: 10.1103/PhysRevC.71.054602
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2005TA34      Eur.Phys.J. A 25, Supplement 1, 273 (2005)

M.Takashina, Y.Sakuragi, Y.Iseri

Effect of halo structure on 11Be + 12C elastic scattering

NUCLEAR REACTIONS 12C(11Be, 11Be), E=49.3 MeV/nucleon; calculated σ(θ). Continuum-discretized coupled-channels method, comparison with data.

doi: 10.1140/epjad/i2005-06-077-1
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2004TA21      Nucl.Phys. A738, 352 (2004)

M.Takashina, M.Ito, Y.Kubo, S.Okabe, Y.Sakuragi

12C + 12C → 8Beg.s. + 16Og.s. resonance reactions and multi-cluster states of highly excited 24Mg nucleus

NUCLEAR REACTIONS 12C(12C, 8Be), E(cm)=20-37 MeV; calculated σ(θ), excitation function; deduced resonance structure. 24Mg deduced molecular rotational band. Coupled channels Born approximation.

doi: 10.1016/j.nuclphysa.2004.04.060
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2003TA01      Phys.Rev. C 67, 014609 (2003)

M.Takashina, M.Ito, Y.Kudo, S.Okabe, Y.Sakuragi

12C+12C → 8Beg.s.+16Og.s. resonance reaction around Ec.m. = 32.5 MeV

NUCLEAR REACTIONS 12C(12C, 8Be), E(cm) ≈ 27-36 MeV; calculated σ(θ), excitation function; deduced resonance features. Coupled-channels Born approximation, comparison with data.

doi: 10.1103/PhysRevC.67.014609
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2003TA04      Phys.Rev. C 67, 037601 (2003)

M.Takashina, S.Takagi, Y.Sakuragi, Y.Iseri

Continuum-discretized coupled-channels study of the 11Be → 10Be+n breakup effect on 11Be elastic scattering

NUCLEAR REACTIONS 12C(11Be, 11Be), E=49.3 MeV/nucleon; calculated σ(θ), contribution of projectile breakup effect; deduced dynamical polarization potential. Continuum-discretized coupled-channels approach, comparison with data.

doi: 10.1103/PhysRevC.67.037601
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2002IT05      Phys.Rev. C66, 034307 (2002)

M.Ito, Y.Hirabayashi, Y.Sakuragi

Multicluster Configuration in Highly Excited States of 24Mg

NUCLEAR STRUCTURE 24Mg; calculated cluster structure, molecular band features. Microscopic coupled-channels approach.

NUCLEAR REACTIONS 12C(12C, 12C'), E(cm) ≈ 20-40 MeV; analyzed resonance features, molecular band structure. Microscopic coupled-channels approach, band crossing model.

doi: 10.1103/PhysRevC.66.034307
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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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2002KA21      Prog.Theor.Phys.(Kyoto) 107, 377 (2002)

M.Katsuma, Y.Sakuragi, S.Okabe, Y.Kondo

Coupled-Channels Study of the Nuclear Rainbow Phenomena for the 16O + 16O System

NUCLEAR REACTIONS 16O(16O, 16O), (16O, 16O'), E=124, 145, 250, 350 MeV; calculated σ(θ); deduced reaction mechanism features. Microscopic coupled-channels method.

doi: 10.1143/PTP.107.377
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2002TA31      Prog.Theor.Phys.(Kyoto), Suppl. 146, 630 (2002)

S.Takagi, M.Takashina, Y.Sakuragi, Y.Iseri

A CDCC Study of 11Be → 10Be + n Breakup Effect on the 11Be Elastic Scattering

NUCLEAR REACTIONS 12C(11Be, 11Be), E=49.3 MeV/nucleon; calculated σ(θ), breakup channel contribution. Continuum-discretized coupled-channels method, comparison with data.

doi: 10.1143/PTPS.146.630
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2001IT02      Phys.Rev. C63, 064303 (2001)

M.Ito, Y.Sakuragi, Y.Hirabayashi

Properties of Microscopic Nucleus-Nucleus Interaction for Molecular Resonance Formation in 12C + 12C and 3α + 3α Systems

NUCLEAR REACTIONS 12C(12C, X), E not given; calculated microscopic interaction potentials, molecular resonance features.

doi: 10.1103/PhysRevC.63.064303
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2001IT05      Acta Phys.Hung.N.S. 13, 157 (2001)

M.Ito, Y.Sakuragi

Molecular States in Highly-Excited 12Be and 10Be

NUCLEAR STRUCTURE 10,12Be; calculated molecular states energy, spin. Coupled-channels approach.

doi: 10.1556/APH.13.2001.1-3.19
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2000IT07      Phys.Rev. C62, 064310 (2000)

M.Ito, Y.Sakuragi

6He + 6He Molecular Resonances as Highly Excited States of 12Be

NUCLEAR REACTIONS 6He(6He, 6He), E(cm) < 16 MeV; calculated total σ partial wave components; deduced molecular resonances. 12Be deduced resonance features. Coupled-channels approach.

doi: 10.1103/PhysRevC.62.064310
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2000SA57      Prog.Theor.Phys.(Kyoto), Suppl. 140, 51 (2000)

Y.Sakuragi

Heavy-Ion Resonance and Multi-Cluster Structure of Nuclei

NUCLEAR REACTIONS 12C(12C, X), (12C, 12C'), (12C, 8Be), (12C, 3α), E(cm)=20-40 MeV; 16O(16O, X), (16O, 16O'), (16O, α12C), E(cm)=20-40 MeV; analyzed σ, σ(E); deduced reaction mechanism features. 24Mg, 32S deduced multi-cluster resonance features. Coupled-channels, Born approximation.

doi: 10.1143/PTPS.140.51
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2000SC11      Eur.Phys.J. A 7, 367 (2000)

K.Schwarz, C.Samanta, M.Fujiwara, H.Rebel, R.De Leo, N.Matsuoka, H.Utsunomiya, H.Akimune, I.Daito, H.Fujimura, F.Ihara, K.Ishibashi, Y.Maeda, T.Yamanaka, H.Yoshida, A.Okihana, T.Yoshimura, P.K.J.van Aarle, W.A.T.Uijen, M.Ito, Y.Sakuragi

Reaction Mechanism of 6Li Scattering at 600 MeV

NUCLEAR REACTIONS 12C, 58Ni, 90Zr, 208Pb(6Li, 6Li), (6Li, dα), E= 600 MeV; measured elastic and breakup σ(θ), particle spectra. Comparison with theoretical calculations.

doi: 10.1007/PL00013619
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1725.


1999IT02      Eur.Phys.J. A 5, 373 (1999)

M.Ito, Y.Sakuragi, Y.Hirabayashi

Dynamic Polarization Potential of 12C + 12C System at Molecular-Resonance Energies

NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=10-50 MeV; calculated σ(q), potentials, wave functions, quadrupole transition densities, σ(E, l), rotational bands. Dynamic polarization potential. Coupled channel calculations.

doi: 10.1007/s100500050300
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1998SA18      Nucl.Instrum.Methods Phys.Res. A402, 347 (1998)

Y.Sakuragi, M.Katsuma

Spin-Orbit Interactions for 3He-Nucleus Scattering at Intermediate Energies

NUCLEAR REACTIONS 58Ni, 208Pb(polarized 3He, 3He), E=72, 150 MeV/nucleon; calculated σ(θ), A(y)(θ); deduced spin-orbit potential. Single-, double-folding models.

doi: 10.1016/S0168-9002(97)00861-9
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1997OK02      Phys.Lett. 393B, 301 (1997)

D.O'Kelly, T.Botting, B.Hurst, R.P.Schmitt, Y.-W.Lui, Y.Hirabayashi, S.Okabe, Y.Sakuragi, H.Utsunomiya, T.Yamagata, M.Ohta

Breakup of 30 MeV/u-16O in Nuclear and Coulomb Fields of 120Sn and 208Pb Nuclei

NUCLEAR REACTIONS 120Sn, 208Pb(16O, α12C), E=30 MeV/nucleon; measured α12C-coin, σ(θ, θ(α12C)); deduced nuclear, Coulomb-breakup interference role. Coupled channels approach, orthogonality condition model.

doi: 10.1016/S0370-2693(96)01636-X
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1997SA57      J.Phys.(London) G23, 1697 (1997)

C.Samanta, Y.Sakuragi, M.Ito, M.Fujiwara

Energy Dependence of the 6Li-Nucleus Interactions at Intermediate Energies

NUCLEAR REACTIONS 12C, 28Si, 58Ni, 120Sn, 208Pb(6Li, 6Li)E=20, 100 MeV/nucleon; calculated σ(θ); deduced projectile breakup channel energy dependence. Coupled channels calculations, energy, density dependent interaction. Other models compared.

doi: 10.1088/0954-3899/23/11/017
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1997SA69      Prog.Theor.Phys.(Kyoto) 98, 521 (1997)

Y.Sakuragi, M.Ito, Y.Hirabayashi, C.Samanta

Breakup Effect on the 6Li Elastic Scattering from 28Si at E/A = 35 and 53 MeV

NUCLEAR REACTIONS 28Si(6Li, 6Li), E=35, 53 MeV/nucleon; analyzed σ(θ); deduced projectile breakup channel role. Double-folding model interactions.

doi: 10.1143/PTP.98.521
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1995HI21      Phys.Rev.Lett. 74, 4141 (1995)

Y.Hirabayashi, Y.Sakuragi, Y.Abe

3α + 3α and 3α + 12C Configurations in 24Mg

NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=29.5-33 MeV; analyzed σ(θ). 24Mg deduced resonance three α-particle character. Band crossing model.

doi: 10.1103/PhysRevLett.74.4141
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1995SA33      Nucl.Phys. A588, 65c (1995)

Y.Sakuragi, S.Funada, Y.Hirabayashi

Coulomb Dissocation of 6He and 11Li and Its Effect on the Elastic Scattering

NUCLEAR REACTIONS 208Pb(11Li, X), (6He, X), E ≤ 80 MeV/nucleon; analyzed total reaction, Coulomb+dissocation σ(E); 208Pb(11Li, 11Li), E=10 MeV/nucleon; 208Pb(6He, 6He), E=10, 30 MeV/nucleon; analyzed σ(θ); deduced Coulomb dissociation role. Microscopic coupled-channels formalism.

doi: 10.1016/0375-9474(95)00100-F
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1994FU04      Nucl.Phys. A575, 93 (1994)

S.Funada, H.Kameyama, Y.Sakuragi

Halo Structure and Soft Dipole Mode of the 6He Nucleus in the α + n + n Cluster Model

NUCLEAR STRUCTURE 6He; calculated ground state, soft dipole mode properties. Cluster model, coupled-rearrangement channel variational method.

doi: 10.1016/0375-9474(94)90140-6
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1993HI13      Phys.Lett. 318B, 32 (1993)

Y.Hirabayashi, Y.Sakuragi, M.Tanifuji

Single-Folding Interaction in Scattering of 6Li and 7Li from Nuclei

NUCLEAR REACTIONS 26Mg, 120Sn(polarized 7Li, 7Li), (polarized 7Li, 7Li'), 26Mg(polarized 6Li, 6Li), (polarized 6Li, 6Li'), E=44 MeV; analyzed σ(θ), tensor analyzing power vs θ; deduced model interactions form factors. Single-folding interactions.

doi: 10.1016/0370-2693(93)91779-M
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1993SA23      Nucl.Phys. A560, 945 (1993)

Y.Sakuragi, M.Tanifuji

Sudden Approximation for Elastic Scattering of Composite Projectiles at Intermediate Energies

NUCLEAR REACTIONS 40Ca(polarized d, d), E=200-700 MeV; 16O(polarized d, d), E=400 MeV; calculated σ(θ), vector analyzing power vs θ. 58Ni(polarized d, d), E=200-700 MeV; calculated σ(θ), vector, tensor analyzing power vs θ. Sudden approximation.

doi: 10.1016/0375-9474(93)90139-O
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1992HI02      Nucl.Phys. A536, 375 (1992)

Y.Hirabayashi, Y.Sakuragi

Coupled-Channels Study of Polarized 6Li Scattering at 44 MeV

NUCLEAR REACTIONS 26Mg, 120Sn(polarized 6Li, 6Li), E=44 MeV; analyzed σ(θ), vector, tensor analyzing power vs θ. Coupled-channels theory.

doi: 10.1016/0375-9474(92)90389-2
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1992HI11      Phys.Rev.Lett. 69, 1892 (1992)

Y.Hirabayashi, Y.Sakuragi

Evidence for Strong Nuclear-Breakup Contribution to 6Li → α + d Breakup by 208Pb at Forward Angles

NUCLEAR REACTIONS 208Pb(6Li, 6Li'), E=156 MeV; analyzed σ(θ); deduced strong breakup contribution. Continuum discretized coupled-channels method.

doi: 10.1103/PhysRevLett.69.1892
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1991HI07      Phys.Lett. 258B, 11 (1991)

Y.Hirabayashi, Y.Sakuragi

Anomalous Renormalization of Cluster-Folding Interactions for 6Li-Nucleus Scattering at Low Energies

NUCLEAR REACTIONS 16O(6Li, 6Li), E=22.8 MeV; 26Mg(6Li, 6Li), E=44 MeV; 58Ni(6Li, 6Li), E=73.7 MeV; 40Ca(6Li, 6Li), E=90, 156 MeV; 28Si(6Li, 6Li), E=154 MeV; analyzed σ(θ). Three-body model, cluster folding interactions.

doi: 10.1016/0370-2693(91)91200-F
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1990SA18      J.Phys.(London) G16, 639 (1990)

Y.Sakuragi, N.Rowley, M.A.Nagarajan

Symmetry Properties of Nearside and Farside Amplitudes in Polarized Heavy-Ion Scattering

NUCLEAR REACTIONS 26Mg(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=44 MeV; calculated σ(θ), analyzing powers vs θ. Nearside, farside component treatment.

doi: 10.1088/0954-3899/16/4/014
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1989HI06      Phys.Lett. 221B, 227 (1989)

Y.Hirabayashi, S.Okabe, Y.Sakuragi

Projectile Breakup Effect in Elastic Scattering of 9Be

NUCLEAR REACTIONS 16O, 27Al, 40Ca(9Be, 9Be), E=158 MeV; calculated σ(θ); deduced potential parameters, projectile breakup effect. Coupled-channels analysis, microscopic cluster model.

doi: 10.1016/0370-2693(89)91702-4
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1989SA08      Phys.Lett. 220B, 22 (1989)

Y.Sakuragi

Breakup Effect on 6Li-Nucleus Scattering at Intermediate Energies

NUCLEAR REACTIONS 58Ni(6Li, 6Li), E=600 MeV; calculated σ(θ), iT11(θ); deduced breakup role. Continuum discretized coupled-channels method.

doi: 10.1016/0370-2693(89)90006-3
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1989SA36      J.Phys.(London) G15, L209 (1989)

Y.Sakuragi, M.A.Nagarajan

Effect of Coulomb Excitation on Tidal Symmetry in the Scattering of Polarised Projectiles

NUCLEAR REACTIONS 208Pb(polarized 23Na, 23Na), (polarized 23Na, 23Na'), E=170 MeV; calculated σ(θ), analyzing power vs θ; deduced tidal symmetry role.

doi: 10.1088/0954-3899/15/10/003
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1989SA46      J.Phys.(London) G15, 1855 (1989)

Y.Sakuragi, M.A.Nagarajan, N.Rowley

Coupled-Channels Calculation for the System 23Na + 208Pb: A test of tidal symmetry

NUCLEAR REACTIONS 208Pb(polarized 23Na, 23Na), (23Na, 23Na'), E=170 MeV; calculated σ(θ), vector, tensor analyzing power vs θ; deduced Coulomb excitation effects. Coupled-channels formalism.

doi: 10.1088/0954-3899/15/12/011
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1989YA02      Phys.Rev. C39, 873 (1989)

T.Yamagata, K.Yuasa, N.Inabe, M.Nakamura, M.Tanaka, S.Nakayama, K.Katori, M.Inoue, S.Kubono, T.Itahashi, H.Ogata, Y.Sakuragi

Elastic Scattering of the Unstable Nucleus 7Be on 12C at 140 MeV

NUCLEAR REACTIONS 12C(7Be, 7Be), E=140 MeV; measured σ(θ); deduced reaction mechanism. Double-folding model, coupled-discretized continuum channels model analyses. Secondary beam projectiles.

doi: 10.1103/PhysRevC.39.873
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1232.


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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1987SA21      Phys.Rev. C35, 2161 (1987)

Y.Sakuragi

Energy and Target Dependence of Projectile Breakup Effect in Elastic Scattering of 6Li

NUCLEAR REACTIONS 12C, 28Si, 40,48Ca, 58Ni, 208Pb(6Li, 6Li), E=40-170 MeV; calculated σ(θ); deduced dynamical polarization potentials. Coupled-channels method.

doi: 10.1103/PhysRevC.35.2161
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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.


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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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.


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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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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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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