NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = Ken-ichi Kubo Found 60 matches. 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
2001KU03 Nucl.Phys. A680, 312c (2001) High Energy Hadron Spin Observables
doi: 10.1016/S0375-9474(00)00435-8
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
2000KI17 Prog.Theor.Phys.(Kyoto) 103, 1173 (2000) 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
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
1999KU18 Prog.Theor.Phys.(Kyoto) 101, 615 (1999) 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
1997YA15 Prog.Theor.Phys.(Kyoto) 98, 95 (1997) Quark Recombination Model for Spin Polarization in High Energy Inclusive Hadron Reactions
doi: 10.1143/PTP.98.95
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
1994YA01 Phys.Rev. C49, 360 (1994) 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
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
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
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
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
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
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
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
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
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
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
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
1987IS03 Phys.Rev. C35, 1037 (1987) 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
1987KA09 Phys.Rev. C35, 1370 (1987) 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
1985HO22 Nucl.Phys. A444, 76 (1985) 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
1985KU04 Nucl.Phys. A435, 708 (1985) 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
1985KU08 Phys.Lett. 153B, 195 (1985) 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
1985TO03 Phys.Rev.Lett. 54, 1203 (1985) 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
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
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
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
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
1982IG01 Phys.Rev. C25, 2144 (1982) 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
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
1981KU03 Phys.Lett. 100B, 453 (1981) 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
1981KU09 Nucl.Phys. A366, 320 (1981) 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
1981YA08 Phys.Lett. 104B, 343 (1981) 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
1979AM03 Phys.Rev. C19, 2403 (1979) 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
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
1978KU03 Phys.Rev. C17, 1271 (1978) 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
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
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
1977NA09 Phys.Rev. C15, 1774 (1977) 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
1977SU04 Nucl.Phys. A288, 493 (1977) 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
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
1977TR02 Nucl.Phys. A282, 269 (1977) 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
1976AM01 Nucl.Phys. A266, 521 (1976) 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
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
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
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
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
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
1975SE09 Phys.Rev.Lett. 35, 357 (1975) 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
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
1974KU07 Nucl.Phys. A224, 573 (1974) 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
1973DE02 Phys.Rev.Lett. 30, 325 (1973) 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
1973KA29 Z.Phys. 262, 439 (1973) 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
1973KU12 Phys.Lett. 45B, 299 (1973) 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
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
1972KU12 Nucl.Phys. A187, 186 (1972) 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
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
1972SA12 Nucl.Phys. A185, 217 (1972) 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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