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Search: Author = K.I.Kubo

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2002KU46      Acta Phys.Hung.N.S. 16, 131 (2002)

K.-I.Kubo, K.Suzuki, N.Nakajima

Spin Physics in the High Energy Hadron Productions - A Systematic Study of the Spin Asymmetries Induced by pp, γp, ep, and νp Collisions

NUCLEAR REACTIONS 1H(p, X), (K-, X), (γ, X), (ν, X), E=high; calculated hyperon spin polarization. Quark rearrangement collision model, comparison with data.

doi: 10.1556/APH.16.2002.1-4.15
Citations: PlumX Metrics

2001KU03      Nucl.Phys. A680, 312c (2001)


High Energy Hadron Spin Observables

doi: 10.1016/S0375-9474(00)00435-8
Citations: PlumX Metrics

2001KU26      Pramana 57, 379 (2001)


Nuclear and Hadronic Reaction Mechanisms Producing Spin Asymmetry

NUCLEAR REACTIONS 1H(polarized p, X), E at 200 GeV/c; analyzed hyperon production associated asymmetries; deduced spin transfer mechanism, related reaction mechanism features.

doi: 10.1007/s12043-001-0047-3
Citations: PlumX Metrics

2000KI17      Prog.Theor.Phys.(Kyoto) 103, 1173 (2000)

Y.Kitsukawa, K.-I.Kubo

Hadron Spin Polarization Produced by a Dynamical Spin-Orbit Interaction

NUCLEAR REACTIONS 1H(p, X), (K-, X), E at 12, 32, 176 GeV/c; calculated hyperon spin polarization, transverse momentum dependence; deduced dynamical spin-orbit interaction. Quark recombination model, comparisons with data.

doi: 10.1143/PTP.103.1173
Citations: PlumX Metrics

2000NA08      Nucl.Phys. A663-664, 573c (2000)

N.Nakajima, K.Suzuki, H.Toki, K.-I.Kubo

Analyzing Powers in Inclusive Pion Production at High Energy and Nucleon Spin Structure

NUCLEAR REACTIONS 1H(polarized p, π-X), (polarized p, π0X), (polarized p, π+X), (polarized p, K+X), (polarized p, K0X), E=0.75 GeV; calculated analyzing powers. Quark recombination model, comparisons with data.

doi: 10.1016/S0375-9474(99)00659-4
Citations: PlumX Metrics

1999KU18      Prog.Theor.Phys.(Kyoto) 101, 615 (1999)

K.-I.Kubo, Y.Yamamoto, H.Toki

New Mechanisms for the Anomalous Spin Observables in High Energy Hyperon Productions

NUCLEAR REACTIONS 1H(polarized p, X), E=high; calculated hyperon spin observables; deduced primary ud quark mechanism.

doi: 10.1143/PTP.101.615
Citations: PlumX Metrics

1997YA15      Prog.Theor.Phys.(Kyoto) 98, 95 (1997)

Y.Yamamoto, K.-I.Kubo, H.Toki

Quark Recombination Model for Spin Polarization in High Energy Inclusive Hadron Reactions

doi: 10.1143/PTP.98.95
Citations: PlumX Metrics

1994KA06      Nucl.Phys. A568, 499 (1994)

T.Kajihara, Y.Yamamoto, K.-I.Kubo

The (p, α) Reaction (I). The Left-Right Asymmetry, the j-Dependence and the Cross-Section Magnitude

NUCLEAR REACTIONS 19F(polarized p, α), E=14 MeV; 116Sn(polarized p, α), E=22 MeV; 60Ni(α, p), E=18 MeV; 19F(p, α), E=14-38 MeV; 90Zr, 27Al(p, α), E=35 MeV; 40Ca(p, α), E=42.5 MeV; 118Sn, 208Pb, 62Ni(p, α), E=22 MeV; 16O(α, α), E=54.1 MeV; analyzed σ(θ); deduced reaction mechanisms systematics.

doi: 10.1016/0375-9474(94)90391-3
Citations: PlumX Metrics

1994YA01      Phys.Rev. C49, 360 (1994)

Y.Yamamoto, K.-I.Kubo

Enormous Spin Polarization in Heavy-Ion-Induced One-Nucleon Transfer Reactions

NUCLEAR REACTIONS 12C(13C, 12C), E=20, 60, 140 MeV; 12C(12C, 13C), E=140, 300 MeV; calculated σ(θ), residual nucleus spin polarization vs θ. 54Fe(13C, 12C), E=60 MeV; calculated (12C)γ(θ). Direct reaction theory, near-side, far-side components.

doi: 10.1103/PhysRevC.49.360
Citations: PlumX Metrics

1993YA01      Phys.Rev. C47, 846 (1993)

Y.Yamamoto, T.Kajino, K.-I.Kubo

Reaction Mechanism of 7Li(3He, p)9Be and 7Li(3H, n)9Be and Primordial Nucleosynthesis of 9Be

NUCLEAR REACTIONS, ICPND 7Li(t, n), (3He, p), E(cm) ≤ 2 MeV; calculated σ(θ), astrophysical S-factor; deduced reaction mechanism, 9Be primordial abundance. Astrophysical implications.

doi: 10.1103/PhysRevC.47.846
Citations: PlumX Metrics

1992HI08      Z.Phys. A343, 471 (1992)

S.Hirenzaki, F.Iseki, K.-I.Kubo

Lambda Polarization in 12C(π-, Lambda) Reactions at p(π) = 4 GeV/c

NUCLEAR REACTIONS 12C(π-, X), E at 4 GeV/c; calculated inclusive lambda production σ vs E(lambda). Regge pole amplitudes approach.

doi: 10.1007/BF01289825
Citations: PlumX Metrics

1992KA25      Phys.Lett. 285B, 5 (1992)

T.Kajihara, K.-I.Kubo, K.Kimura, T.Nakashima

The Universal Phase Relation in the Left-Right Asymmetry of the (p(pol), α) Simultaneous Pickup Mechanism

NUCLEAR REACTIONS 19F(polarized p, α), E=14 MeV; 116Sn(polarized p, α), E=22 MeV; analyzed σ(θ); deduced left, right σ usefulness in understanding asymmetry.

doi: 10.1016/0370-2693(92)91291-G
Citations: PlumX Metrics

1992KU04      Nucl.Phys. A539, 500 (1992)

K.-I.Kubo, M.Yabe, I.J.Thompson

Extended DWBA Prescription and Angular Momentum Mismatched Reactions

NUCLEAR REACTIONS 40,42Ca(16O, 15N), E=56 MeV; calculated σ(θ); deduced matching condition dynamics. Extended DWBA.

doi: 10.1016/0375-9474(92)90290-Z
Citations: PlumX Metrics

1991KU13      Nucl.Phys. A534, 381 (1991)


Dynamical Polarization Potential and (A)Ca + 16O (A = 40, 42, 44 and 48) Optical Model Potentials

NUCLEAR REACTIONS 40,42,44,48Ca(16O, 16O), (16O, X), E=56 MeV; analyzed data analyses; deduced absorptive potential vs mass number. Dynamical polarization potential.

doi: 10.1016/0375-9474(91)90507-3
Citations: PlumX Metrics

1991KU14      Nucl.Phys. A534, 393 (1991)

K.-I.Kubo, P.Manyum, P.E.Hodgson

The Spin Distribution in Heavy-Ion Fusion

NUCLEAR REACTIONS 64Ni(32S, X), E=88 MeV; 40Ca(16O, X), E=55.6, 60 MeV; 40,42,44,48Ca(16O, X), E=56 MeV; calculated elastic, inelastic dynamical polarization, optical imaginary potentials; deduced heavy-ion fusion spin-distribution.

doi: 10.1016/0375-9474(91)90508-4
Citations: PlumX Metrics

1989BO20      Nucl.Phys. A499, 381 (1989)

R.Bonetti, F.Crespi, K.-I.Kubo

The 58Ni(p, α) Reaction Mechanism through a Study of the Analyzing Power

NUCLEAR REACTIONS 58Ni(polarized p, α), E=22, 72 MeV; calculated σ(θ), analyzing power vs θ. DWBA analysis, knock out, pick up contributions.

doi: 10.1016/0375-9474(89)90053-5
Citations: PlumX Metrics

1988KA02      Phys.Rev. C37, 512 (1988)

T.Kajino, G.F.Bertsch, Ken-ichi Kubo

E1 Polarizability of 7Li and Astrophysical S Factor for 4He(t, γ)7Li

NUCLEAR REACTIONS, ICPND 58Ni, 120Sn(polarized 7Li, 7Li), E=sub-Coulomb; calculated T20(θ); deduced electric dipole polarizability. 4He(t, γ), E(cm) ≈ 0-1.5 MeV; calculated radiative capture σ, channel dipole polarizability; deduced astrophysical S-factor S(0).

doi: 10.1103/PhysRevC.37.512
Citations: PlumX Metrics

1988KA07      Phys.Lett. 202B, 475 (1988)

T.Kajino, H.Toki, K.-I.Kubo, I.Tanihata

Nuclear-Matter Radii of 7Be and 7Li and Astrophysical S-Factors for Radiative Alpha-Capture Reactions

NUCLEAR REACTIONS, ICPND 3H, 3He(α, γ), E=low; calculated capture σ, capture reaction astrophysical factor S(E).

doi: 10.1016/0370-2693(88)91846-1
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1987EJ02      Phys.Rev. C36, 1435 (1987)

H.Ejiri, T.Fukuda, T.Shibata, H.Bando, K.-I.Kubo

Spin Polarization and Spin Alignment in Hypernuclei

NUCLEAR REACTIONS 12C, 56Fe(π+, K+), E at 1.05 GeV/c; 12C, 56Fe(π+, K+), E at 0.72 GeV/c; calculated spin polarization, spin alignment. DWBA method.

doi: 10.1103/PhysRevC.36.1435
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1987HI06      Phys.Lett. 194B, 20 (1987)

S.Hirenzaki, T.Kajino, K.-I.Kubo, H.Toki, I.Tanihata

Pionic Atoms of Unstable Nuclei

ATOMIC PHYSICS, Mesic-Atoms K, Cl(Ar, X), E=800 MeV/nucleon; calculated pionic atoms formation σ, energy shifts, widths; deduced pion-nucleus optical potentials.

NUCLEAR REACTIONS K, Cl(Ar, X), E=800 MeV/nucleon; calculated pionic atoms formation σ, energy shifts, widths; deduced pion-nucleus optical potentials.

doi: 10.1016/0370-2693(87)90762-3
Citations: PlumX Metrics

1987IS03      Phys.Rev. C35, 1037 (1987)

F.Iseki, K.-I.Kubo, H.Toki

Cascade Model Calculations of p(bar) + 12C → n(bar) + X at 590 MeV/c

NUCLEAR REACTIONS 12C(p-bar, n-barX), E at 590 MeV/c; calculated σ(θ); deduced Pauli effect role. Cascade model.

doi: 10.1103/PhysRevC.35.1037
Citations: PlumX Metrics

1987KA09      Phys.Rev. C35, 1370 (1987)

T.Kajino, H.Toki, K.-I.Kubo

Pionic Fusion and the Clustering Correlation

NUCLEAR REACTIONS 4He(3He, π0), 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca(3He, π+), E=88.8 MeV/nucleon; calculated pionic fusion σ. Microscopic cluster model.

doi: 10.1103/PhysRevC.35.1370
Citations: PlumX Metrics

1985HO22      Nucl.Phys. A444, 76 (1985)

A.Hosaka, K.-I.Kubo, H.Toki

G-Matrix Effective Interaction with the Paris Potential

NUCLEAR STRUCTURE 16O, 40Ca, 90Zr; calculated G-matrix elements; deduced Landau-Migdal parameter. Effective interaction from Paris nucleon-nucleon force.

doi: 10.1016/0375-9474(85)90292-1
Citations: PlumX Metrics

1985KU04      Nucl.Phys. A435, 708 (1985)

K.-I.Kubo, H.Toki, M.Igarashi

Optical-Potential Description of Antiproton-Nucleus Scattering at 46.8 MeV

NUCLEAR REACTIONS 12C(p-bar, p-bar), E=46.8 MeV; calculated elastic, inelastic σ(θ), p-bar polarization; deduced (p-bar)-nucleus potential parameters. Optical model.

doi: 10.1016/0375-9474(85)90183-6
Citations: PlumX Metrics

1985KU08      Phys.Lett. 153B, 195 (1985)

K.-I.Kubo, F.Iseki, H.Toki

A Strong Absorptive Potential as the Preferential Antiproton-Nucleus Optical Potential

NUCLEAR REACTIONS 12C(p-bar, p-bar), (p-bar, p-bar'), E=46.8 MeV; measured σ(θ); deduced strong nuclear interior damping.

doi: 10.1016/0370-2693(85)90529-5
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1985TO03      Phys.Rev.Lett. 54, 1203 (1985)

H.Toki, K.-I.Kubo

Comment on ' High-Spin-State Spectroscopy with the Reaction 88Sr(p(pol), π-)89Zr '

NUCLEAR REACTIONS 88Sr(polarized p, π-), E not given; analyzed asymmetry vs θ; deduced short-range interaction, pion distortion role.

doi: 10.1103/PhysRevLett.54.1203
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1985YA03      Phys.Rev. C31, 676 (1985)

K.Yagi, Y.Aoki, K.Hashimoto, H.Iida, H.Sakamoto, Y.Tagishi, M.Matoba, M.Igarashi, K.-I.Kubo

Analyzing Power as a Probe for Clarifying Nuclear Reaction Mechanisms: Study of the two-step unbound channel contribution

NUCLEAR REACTIONS 208Pb(polarized p, t), E=22, 35, 50 MeV; measured σ(θ), analyzing power vs θ; deduced two-step unbound channel role. First-, second-order finite range DWBA analysis.

doi: 10.1103/PhysRevC.31.676
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1118.

1985YA10      Prog.Theor.Phys.(Kyoto) 73, 1165 (1985)

M.Yabe, A.Hosaka, K.-I.Kubo, H.Toki

On the Central-Odd Components in the G-Matrix Interactions and the Low Energy (p, p') and (p, n) Reactions

NUCLEAR REACTIONS 16O(p, n), E=35 MeV; calculated σ(θ). 48Ca(p, p'), E=65 MeV; calculated σ(θ). 58Ni(p, p'), (polarized p, p'), E=65 MeV; calculated σ(θ), analyzing power vs θ.

doi: 10.1143/PTP.73.1165
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1984BO19      Nucl.Phys. A420, 109 (1984)

R.Bonetti, L.Colombo, K.-I.Kubo

Inelastic α-Scattering to the Continuum: A probe of α-clustering in nuclei

NUCLEAR REACTIONS 90Zr(α, α'), E=140 MeV; measured σ(θ, Eα'); deduced α-clustering proability. Statistical multi-step direct theory.

doi: 10.1016/0375-9474(84)90660-2
Citations: PlumX Metrics

1984NI01      Nucl.Phys. A415, 230 (1984)

H.Nishioka, J.A.Tostevin, R.C.Johnson, K.-I.Kubo

Projectile Excitation and Structure Effects in 6Li and 7Li Scattering

NUCLEAR REACTIONS 58Ni(polarized 6Li, 6Li), (polarized 7Li, 7Li), E(cm)=18.1 MeV; calculated σ(θ), analyzing power vs θ; deduced projectile excitation, structure effects. Coupled-channels calculations, cluster wave functions.

doi: 10.1016/0375-9474(84)90622-5
Citations: PlumX Metrics

1982IG01      Phys.Rev. C25, 2144 (1982)

M.Igarashi, Ken-ichi Kubo

Predominance of the Sequential Pickup Mechanism in the 208Pb(p, t)206Pb 3+ Transition

NUCLEAR REACTIONS 208Pb(p, t), (polarized p, t), E=22, 35 MeV; calculated σ(θ), A(θ); deduced reaction mechanism. Finite-range DWBA, realistic interactions.

doi: 10.1103/PhysRevC.25.2144
Citations: PlumX Metrics

1982NI03      Phys.Rev.Lett. 48, 1795 (1982)

H.Nishioka, R.C.Johnson, J.A.Tostevin, K.-I.Kubo

Spin-Orbit Interaction Induced by Heavy-Ion Projectile Excitation

NUCLEAR REACTIONS 58Ni(6Li, 6Li), (polarized 6Li, 6Li), E(cm)=20.7 MeV; 58Ni(7Li, 7Li), (polarized 7Li, 7Li), E(cm)=18.1 MeV; analyzed σ(θ), iT11(θ); deduced effective spin-orbit interaction, projectile excitation. Coupled-channels analysis.

doi: 10.1103/PhysRevLett.48.1795
Citations: PlumX Metrics

1981KU03      Phys.Lett. 100B, 453 (1981)

K.-I.Kubo, P.E.Hodgson

Equivalent Bare Optical Potentials in Heavy-Ion Inelastic Scattering

NUCLEAR REACTIONS 40Ca(16O, 16O'), E=60 MeV; 40Ca(13C, 13C'), E=68 MeV; calculated σ(θ). Equivalent bare optical potentials.

doi: 10.1016/0370-2693(81)90603-1
Citations: PlumX Metrics

1981KU09      Nucl.Phys. A366, 320 (1981)

K.-I.Kubo, P.E.Hodgson

Exit-Channel Distorting Potentials in Heavy-Ion Inelastic Scattering and the Equivalent Bare Optical Potential

NUCLEAR REACTIONS 40Ca(16O, 16O'), E=60 MeV; 40Ca(13C, 13C'), E=68 MeV; 208Pb(11B, 11B'), E=72.2 MeV; 208Pb(16O, 16O'), E=80-180 MeV; calculated σ(θ). Equivalent local bare potential.

doi: 10.1016/0375-9474(81)90291-8
Citations: PlumX Metrics

1981YA08      Phys.Lett. 104B, 343 (1981)

M.Yabe, A.Mori, K.-I.Kubo

Interference Effects in the Strong Isospin Dependence of the Polarization Asymmetry in 12C(p, p')12C* 1+ Transitions

NUCLEAR REACTIONS 12C(p, p'), E=65 MeV; analyzed σ(θ), analyzing power vs θ; deduced one-step, two-step interference effects. DWBA, successive nucleon transfer mechanism.

doi: 10.1016/0370-2693(81)90693-6
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1979AM03      Phys.Rev. C19, 2403 (1979)

H.Amakawa, K.-i.Kubo

Analyzing Power of Two-Step (p, t) Reaction Leading to the Unnatural-Parity State

NUCLEAR REACTIONS 18O(polarized p, t), E=24.4 MeV; calculated σ(θ), A(θ). Second-order DWBA analysis.

doi: 10.1103/PhysRevC.19.2403
Citations: PlumX Metrics

1979YA09      Phys.Rev.Lett. 43, 1087 (1979)

K.Yagi, S.Kunori, Y.Aoki, K.Nagano, Y.Toba, K.-I.Kubo

Anomalous Analyzing Powers for Strong(pol p, t) Ground-State Transitions and Interference between Direct and (p, d)(d, t) Sequential Process

NUCLEAR REACTIONS 100Ru, 104,110Pd, 116Cd, 118Sn, 122,128,130Te, 144Nd(polarized p, t), E=22 MeV; measured σ(θ), A(θ); deduced interference effects between two-step, one-step processes.

doi: 10.1103/PhysRevLett.43.1087
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE0084.

1978KU03      Phys.Rev. C17, 1271 (1978)

K.-i.Kubo, H.Amakawa

Energy Dependence of Two-Step (p, t) Cross Sections

NUCLEAR REACTIONS 18O(p, t), E=20.0-43.6 MeV; calculated σ(θ).

doi: 10.1103/PhysRevC.17.1271
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1978MA13      Phys.Lett. 74B, 187 (1978)

M.Makowska-Rzeszutko, P.Egelhof, D.Kassen, E.Steffens, W.Weiss, D.Fick, W.Dreves, K.-I.Kubo, T.Suzuki

Transfer Reactions Initiated on 12C by Vector Polarized 6Li

NUCLEAR REACTIONS 12C(polarized 6Li, d), (polarized 6Li, α), E=20.0 MeV; measured A(θ).

doi: 10.1016/0370-2693(78)90549-X
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1978TR01      Phys.Rev.Lett. 40, 13 (1978)

R.E.Tribble, J.D.Cossairt, K.-I.Kubo, D.P.May

Evidence of a Direct Process in the (4He, 8He) Reaction

NUCLEAR REACTIONS 64Ni(α, 8He), E=80 MeV; measured σ(E(8He), θ); deduced reaction mechanism.

doi: 10.1103/PhysRevLett.40.13
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1977NA09      Phys.Rev. C15, 1774 (1977)

K.G.Nair, K.-I.Kubo

Apparent Puzzles in the Analyses of the 30Si(16O, 15N)31P Reaction Data

NUCLEAR REACTIONS 30Si(16O, 15N), E=60, 73.5 MeV; analyzed data, σ(θ). 31P levels deduced S.

doi: 10.1103/PhysRevC.15.1774
Citations: PlumX Metrics

1977SU04      Nucl.Phys. A288, 493 (1977)

T.Suzuki, A.Arima, K.-I.Kubo

Mixing of the Og Orbit in 20Ne and the Analysis of a One-Step Forbidden Transition

NUCLEAR REACTIONS 20Ne(e, e'); analyzed data. 20Ne deduced configuration admixture.

doi: 10.1016/0375-9474(77)90346-3
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1977TO02      Phys.Rev. C15, 281 (1977); Erratum Phys.Rev. C15, 1607 (1977)

C.W.Towsley, P.K.Bindal, K.-I.Kubo, K.G.Nair, K.Nagatani

Common Optical Potential and Peripheral Processes between 1p-Shell Nuclei

NUCLEAR REACTIONS 12C, 16O(10B, 10B), (10B, 10B'), E=100 MeV; 12C, 16O(14N, 14N), (14N, 14N'), E=155 MeV; measured σ(θ); deduced optical potentials. 12C, 16O levels deduced β.

doi: 10.1103/PhysRevC.15.281
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1977TR02      Nucl.Phys. A282, 269 (1977)

R.E.Tribble, K.-I.Kubo

Charge Asymmetry in (d, t) and (d, 3He) Reactions and Optimum Q-Value Conditions

NUCLEAR REACTIONS 28Si, 32S(d, 3He), (d, t), E=28 MeV; measured σ(θ). 27Si, 27Al, 31S, 31P analog states deduced S. DWBA analysis.

doi: 10.1016/0375-9474(77)90215-9
Citations: PlumX Metrics

1976AM01      Nucl.Phys. A266, 521 (1976)

H.Amakawa, K.-I.Kubo

Spin-Orbit Potential in Heavy-Ion Collisions

NUCLEAR REACTIONS 12C(6Li, 6Li), (6Li, 6Li'), (14N, 14N), (14N, 14N'); calculated spin-orbit potentials, σ, polarization. Folding model.

doi: 10.1016/0375-9474(76)90372-9
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1976KU06      Phys.Rev.Lett. 37, 222 (1976)

K.-I.Kubo, K.G.Nair, K.Nagatani

Anomalous Angular Distributions and the Unique Structure of the l = 1 Transition Amplitude

NUCLEAR REACTIONS 12C(7Li, 6Li), E=36 MeV; 12C(10B, 9Be), (14N, 13N), E=100 MeV; 16O(14N, 13N), E=79 MeV; 12C(14N, 13C), E=155 MeV; 26Mg(11B, 10Be), E=114 MeV; analyzed anomalous σ(θ).

doi: 10.1103/PhysRevLett.37.222
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1976WE10      Phys.Lett. 61B, 237 (1976)

W.Weiss, P.Egelhof, K.D.Hildenbrand, D.Kassen, M.Makowska-Rzeszutko, D.Fick, H.Ebinghaus, E.Steffens, A.Amakawa, K.I.Kubo

Elastic Scattering of Vector Polarized 6Li

NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), E=20, 22.8 MeV; 16O, 28Si, 58Ni(polarized 6Li, 6Li), E=22.8 MeV; measured σ(θ), analyzing power A(θ).

doi: 10.1016/0370-2693(76)90138-6
Citations: PlumX Metrics

1975BO18      Z.Phys. A273, 211 (1975)

H.G.Bohlen, K.D.Hildenbrand, A.Gobbi, K.I.Kubo

The (18O, 16O) Reaction on Even Tin Isotopes

NUCLEAR REACTIONS 112,116,118,120,122,124Sn(18O, 18O), E=57, 60 MeV; measured σ(θ). 112,116,118,120,122,124Sn(18O, 16O), E=57, 60 MeV; measured σ(E(16O), θ).

doi: 10.1007/BF01435841
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1673.

1975BO61      Z.Phys. A 273, 211 (1975)

H.G.Bohlen, K.D.Hildenbrand, A.Gobbi, K.I.Kubo

The (18O, 16O) reaction on even tin isotopes

NUCLEAR REACTIONS 112Sn(18O, 16O), 112Sn(18O, 18O), 116Sn(18O, 16O), 116Sn(18O, 18O), 118Sn(18O, 16O), 118Sn(18O, 18O), 120Sn(18O, 16O), 120Sn(18O, 18O), 122Sn(18O, 16O), 122Sn(18O, 18O), 124Sn(18O, 16O), 124Sn(18O, 18O), E=57-60 MeV; measured products, 112Sn, 116Sn, 118Sn, 120Sn, 122Sn, 124Sn, 114Sn, 16O, 126Sn; deduced σ(θ). Data were imported from EXFOR entry O1673.

doi: 10.1007/BF01435841
Citations: PlumX Metrics

1975KU08      Nucl.Phys. A246, 246 (1975)


Nucleon-Exchange Type Charge-Exchange Process and the Spin-Forbidden (6Li, 6He) Transitions

NUCLEAR REACTIONS 26Mg, 42,48Ca(6Li, 6He), E=34 MeV; calculated σ.

doi: 10.1016/0375-9474(75)90575-8
Citations: PlumX Metrics

1975SE09      Phys.Rev.Lett. 35, 357 (1975)

H.Segawa, K.-I.Kubo, A.Arima

Two-Step Analysis of the 18O(p, t)16O 2- Excitation and Phase Relations in the Nonorthogonal Term

NUCLEAR REACTIONS 18O(p, t), E=24.2 MeV; calculated σ(Et, θ).

doi: 10.1103/PhysRevLett.35.357
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1974DU15      Phys.Lett. 48B, 1 (1974)

H.H.Duhm, H.Hafner, R.Renfordt, M.Goldschmidt, O.Dragun, K.-I.Kubo

Charge Exchange (6Li, 6He) and the Two-Step Pick-up Stripping (6Li, 7Li)(7Li, 6He) Excitation Mode

NUCLEAR REACTIONS 18O, 26Mg(6Li, 6He) measured σ(E(6He), θ).

doi: 10.1016/0370-2693(74)90441-9
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1943.

1974KU07      Nucl.Phys. A224, 573 (1974)

K.I.Kubo, F.Nemoto, H.Bando

Investigation of the 16O(7Li, t)20Ne and 15N(7Li, t)19F Reactions with Microscopic α-Cluster Plus Core Wave Functions

NUCLEAR REACTIONS 16O, 15N(7Li, t); calculated σ(θ). 19F, 20Ne levels deduced S.

doi: 10.1016/0375-9474(74)90557-0
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1973DE02      Phys.Rev.Lett. 30, 325 (1973)

R.M.DeVries, K.I.Kubo

Recoil Effects in Single-Nucleon-Transfer Heavy-Ion Reactions

NUCLEAR REACTIONS 12C(14N, 13C), E=78 MeV; calculated σ(θ); analyzed recoil effects. DWBA.

doi: 10.1103/PhysRevLett.30.325
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1973KA29      Z.Phys. 262, 439 (1973)

T.Kammuri, K.-I.Kubo, T.Une

Two-Nucleon Transfer Reactions between Heavy Ions

NUCLEAR REACTIONS 26Mg(18O, 16O), E=33.5, 35.7 MeV; measured nothing, calculated σ(θ). 28Mg levels calculated S, deformation parameters.

doi: 10.1007/BF01394543
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1973KU12      Phys.Lett. 45B, 299 (1973)

K.-I.Kubo, H.H.Duhm, N.Ueta

Cluster Model DWBA Analysis of Lithium Induced Single Nucleon Transfer Reactions

NUCLEAR REACTIONS 12C(7Li, 6Li), E=36 MeV; calculated σ(θ), cluster model DWBA analysis.

doi: 10.1016/0370-2693(73)90038-5
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1973SC26      Nucl.Phys. A212, 573 (1973)

P.Schumacher, N.Ueta, H.H.Duhm, K.-I.Kubo, W.J.Klages

Lithium Elastic and Inelastic Scattering and Lithium-Induced Single Nucleon Transfer Reactions

NUCLEAR REACTIONS 12C, 13C, 16O, 26Mg, 28Si(6Li, 6Li), (6Li, 6Li'), (7Li, 7Li), (7Li, 7Li'), (6Li, 7Li), (7Li, 6Li), (7Li, 6He), (7Li, 8Li), E=34, 36 MeV; measured σ(θ). Deduced optical model parameters, FRDWBA analysis.

doi: 10.1016/0375-9474(73)90824-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1929.

1972KU12      Nucl.Phys. A187, 186 (1972)

K.-I.Kubo, M.Hirata

DWBA Treatment of Cluster Transfer Reactions

NUCLEAR REACTIONS 12C(6Li, d), E=18 MeV; 12C, 16O(7Li, t), E=15, 16 MeV; analyzed σ(θ). Finite-range DWBA.

doi: 10.1016/0375-9474(72)90083-8
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1972KU13      Nucl.Phys. A187, 205 (1972)


Finite-Range DWBA Analysis of the 16O(7Li, t)20Ne and 15N(7Li, t)19F Reactions

NUCLEAR REACTIONS 16O, 15N(7Li, t), E=15 MeV; analyzed σ(θ). Finite-range DWBA.

doi: 10.1016/0375-9474(72)90084-X
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1972SA12      Nucl.Phys. A185, 217 (1972)

M.Sakai, K.-I.Kubo

Deeply Bound Neutron Hole States Studied by (p, d) Reactions

NUCLEAR REACTIONS 118Sn, 140Ce, 206,208Pb(p, d), E not given; calculated σ(Ed). 98Mo, 118Sn, 90Zr, 140Ce, 206,208Pb(p, d), E not given; calculated σ(θ).

doi: 10.1016/0375-9474(72)90562-3
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Note: The following list of authors and aliases matches the search parameter K.I.Kubo: , K.I.KUBO