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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)

K.-I.Kubo

High Energy Hadron Spin Observables

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

2001KU26      Pramana 57, 379 (2001)

K.-I.Kubo

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)

K.-I.Kubo

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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

doi: 10.1007/BF01435841
Citations: PlumX Metrics
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)

K.-I.Kubo

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
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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
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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)

K.-I.Kubo

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