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NSR database version of April 25, 2024.

Search: Author = M.Takashina

Found 23 matches.

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2021FU07      Phys.Rev. C 103, 044602 (2021)

T.Furumoto, M.Takashina

Relation between transition density and proton inelastic scattering by 12C target at Ep = 65 and 200 MeV

NUCLEAR REACTIONS 12C(polarized p, p), (polarized p, p'), E=65, 200 MeV; analyzed experimental data for σ(Ε, θ) and analyzing power Ay(E, θ) for ground state and Hoyle state using microscopic coupled channel (MCC) method with potentials from folding a complex G-matrix effective nucleon-nucleon interaction, and transition density from modified Algebraic Cluster Model (ACM) wave function.

doi: 10.1103/PhysRevC.103.044602
Citations: PlumX Metrics


2013ON02      Phys.Lett. B 725, 277 (2013)

H.J.Ong, I.Tanihata, A.Tamii, T.Myo, K.Ogata, M.Fukuda, K.Hirota, K.Ikeda, D.Ishikawa, T.Kawabata, H.Matsubara, K.Matsuta, M.Mihara, T.Naito, D.Nishimura, Y.Ogawa, H.Okamura, A.Ozawa, D.Y.Pang, H.Sakaguchi, K.Sekiguchi, T.Suzuki, M.Taniguchi, M.Takashina, H.Toki, Y.Yasuda, M.Yosoi, J.Zenihiro

Probing effect of tensor interactions in 16O via (p, d) reaction

NUCLEAR REACTIONS 16O(p, d), E=198, 295, 392 MeV; measured reaction products; deduced σ(θ), tensor interaction in one-nucleon transfer reactions.

doi: 10.1016/j.physletb.2013.07.038
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2436. Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


2011KI11      Int.J.Mod.Phys. E20, 843 (2011)

Y.Kikuchi, K.Kato, T.Myo, M.Takashina, K.Ikeda

Two-neutron correlations in halo nuclei via Coulomb breakup reactions

doi: 10.1142/S0218301311018812
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2011KI40      Phys.Rev. C 84, 064610 (2011)

Y.Kikuchi, N.Kurihara, A.Wano, K.Kato, T.Myo, M.Takashina

Three-body model analysis of α+d$ elastic scattering and the 2H(α, γ)6Li reaction in complex-scaled solutions of the Lippmann-Schwinger equation

NUCLEAR REACTIONS 2H(α, α), E(cm)<6 MeV; calculated elastic phase shifts, deuteron breakup effect on resonances. 2H(α, γ)6Li, E<6 MeV; calculated E2 transition strengths, σ(E) for radiative capture. 2H(α, γ)6Li, E<6 MeV; calculated σ(E) for photodisintegration. Complex-scaled solutions of the Lippmann-Schwinger equation (CSLS) for α+d scattering. Comparison with experimental data.

NUCLEAR STRUCTURE 6Li; calculated levels, widths, ∼, π, rms matter and charge radii, quadrupole moment, considering α+p+n three-body structure of 6Li, and using Lippmann-Schwinger equation. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.064610
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2010AO01      Phys.Lett. B 692, 302 (2010)

N.Aoi, S.Kanno, S.Takeuchi, H.Suzuki, D.Bazin, M.D.Bowen, C.M.Campbell, J.M.Cook, D.-C.Dinca, A.Gade, T.Glasmacher, H.Iwasaki, T.Kubo, K.Kurita, T.Motobayashi, W.F.Mueller, T.Nakamura, H.Sakurai, M.Takashina, J.R.Terry, K.Yoneda, H.Zwahlen

Enhanced collectivity in 74Ni

NUCLEAR REACTIONS 1H(74Ni, 74Ni'), E=81 MeV/nucleon; measured Eγ, Iγ; 74Ni; deduced J, π, level energy, σ, deformation length and parameter.

doi: 10.1016/j.physletb.2010.07.052
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1814. Data from this article have been entered in the XUNDL database. For more information, click here.


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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2010KI06      Phys.Rev. C 81, 044308 (2010)

Y.Kikuchi, K.Kato, T.Myo, M.Takashina, K.Ikeda

Two-neutron correlations in 6He in a Coulomb breakup reaction

NUCLEAR STRUCTURE 6He; calculated two-neutron density distribution, coulomb breakup cross-section of halo nucleus via α+n+n channel, E1 strength distributions, invariant mass spectra using Complex Scaling Lippmann-Schwinger method. Comparison with experimental data.

doi: 10.1103/PhysRevC.81.044308
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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.


2009TA08      Phys.Rev. C 79, 054319 (2009)

S.Takeuchi, N.Aoi, T.Motobayashi, S.Ota, E.Takeshita, H.Suzuki, H.Baba, T.Fukui, Y.Hashimoto, K.Ieki, N.Imai, H.Iwasaki, S.Kanno, Y.Kondo, T.Kubo, K.Kurita, T.Minemura, T.Nakabayashi, T.Nakamura, T.Okumura, T.K.Onishi, H.Sakurai, S.Shimoura, R.Sugou, D.Suzuki, M.K.Suzuki, M.Takashina, M.Tamaki, K.Tanaka, Y.Togano, K.Yamada

Low-lying states in 32Mg studied by proton inelastic scattering

NUCLEAR REACTIONS 1H(32Mg, 32Mg'), E=46.5 MeV/nucleon; measured Eγ, Iγ, scattered particle spectra, σ, σ(θ). 32Mg; deduced levels, J, π, deformation lengths, rms radii.Coupled-channel analysis of angular distribution cross sections. 24,26,28,30,32,34Mg; level systematics.

doi: 10.1103/PhysRevC.79.054319
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2147. Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


2008KI22      Int.J.Mod.Phys. E17, 2368 (2008)

Y.Kikuchi, K.Kato, T.Myo, M.Takashina, K.Ikeda

Analysis on two-neutron correlation through Dalitz plot of Coulomb breakup reaction for 6He

NUCLEAR STRUCTURE 6He; calculated the energy and Dalitz distributions of E1 transition strength; deduced dominance of sequential decay process. Lippmann-Schwinger equation.

doi: 10.1142/S021830130801163X
Citations: PlumX Metrics


2008TA02      Phys.Rev. C 77, 014604 (2008)

M.Takashina, Y.Kanada-Enyo

Inelastic proton scattering and neutron quadrupole transitions of 12Be

NUCLEAR REACTIONS p(10Be, 10Be), (10Be, 10Be'), E=59.2 MeV/nucleon; p(12Be, 12Be), (12Be, 12Be'), E=55 MeV/nucleon; calculated density distributions, radii, transition strengths, single-particle transition densities, σ(θ). 10,12Be; deduced levels, J, π.12C(p, p), E=50 MeV; calculated σ(θ).

doi: 10.1103/PhysRevC.77.014604
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2008TA21      Phys.Rev. C 78, 014602 (2008)

M.Takashina

Interpretation of a diffraction phenomenon observed in the angular distribution of α inelastic scattering on 12C exciting the 0+2 state

NUCLEAR REACTIONS 12C(α, α'), E=240 MeV; calculated σ(θ). Eikonal wave Born approximation.

doi: 10.1103/PhysRevC.78.014602
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2007WA32      Phys.Lett. B 653, 173 (2007)

T.Wakasa, E.Ihara, K.Fujita, Y.Funaki, K.Hatanaka, H.Horiuchi, M.Itoh, J.Kamiya, G.Ropke, H.Sakaguchi, N.Sakamoto, Y.Sakemi, P.Schuck, Y.Shimizu, M.Takashina, S.Terashima, A.Tohsaki, M.Uchida, H.P.Yoshida, M.Yosoi

New candidate for an alpha cluster condensed state in 16O(α, α') at 400 MeV

NUCLEAR REACTIONS 16O(α, α'), E=400 MeV; analyzed elastic and inelastic σ(θ). Comparison with model calculations. Evidence for cluster structure.

doi: 10.1016/j.physletb.2007.08.016
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2060.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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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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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