NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = B.Sorensen Found 30 matches. 1980JA13 Nucl.Phys. A344, 315 (1980) The (α, 6He) Reaction and Other Two-Neutron Transfer Reactions Leading to 24Mg and 152Sm NUCLEAR REACTIONS 26Mg(α, 6He), E=35.5, 40 MeV; 154Sm(α, 6He), E=49.7 MeV; 26Mg(p, t), E=27 MeV; 26Mg(16O, 16O), E=60 MeV; analyzed σ(θ). 24Mg levels deduced population mechanism. Deformed nucleus model, direct, multistep inelastic processes.
doi: 10.1016/0375-9474(80)90681-8
1977SO01 Phys.Lett. 66B, 119 (1977) Interference Phenomena in Heavy Ion Induced Two-Nucleon Transfer Reactions NUCLEAR REACTIONS 148Sm(18O, 16O), 150Sm(16O, 18O); calculated σ(θ).
doi: 10.1016/0370-2693(77)90154-X
1974AS05 Nucl.Phys. A226, 454 (1974) R.J.Ascuitto, C.H.King, L.J.McVay, B.Sorensen One-Nucleon Transfer Reactions in Deformed Nuclei NUCLEAR REACTIONS 171Yb(d, p), E=11.20, 16.00 MeV; calculated σ(Ep, θ). 172Yb(p, d), E=17.00 MeV; 172Yb(d, d'), E=12.00 MeV; 186W(p, d), E=18.00 MeV; calculated σ(Ed, θ). 171,172Yb, 185W deduced levels, J, π, L.
doi: 10.1016/0375-9474(74)90495-3
1974ER03 Phys.Rev.Lett. 33, 1102 (1974) K.A.Erb, D.L.Hanson, R.J.Ascuitto, B.Sorensen, J.S.Vaagen, J.J.Kolata Observation of Multistep Inelastic Processes in Heavy-Ion-Induced Two-Neutron Transfer Reactions on Rare-Earth Nuclei NUCLEAR REACTIONS 186W(12C, 14C), E=70 MeV; measured σ(E(14C), θ). 184W levels deduced form factors.
doi: 10.1103/PhysRevLett.33.1102
1974SO02 Phys.Lett. 49B, 109 (1974) Pairing and Hexadecapole Fields in Deformed Samarium Isotopes as Probed by Two-Nucleon Transfer Reactions NUCLEAR REACTIONS 154Sm(t, p), E=12 MeV; measured nothing, calculated σ(θ). 156Sm levels deduced effect of pairing, hexadecapole fields on σ(θ).
doi: 10.1016/0370-2693(74)90484-5
1974SO09 Phys.Lett. 52B, 285 (1974) Light and Heavy Ion Transfer Reactions among Light Nuclei NUCLEAR REACTIONS 26Mg(t, n), E=5.7 MeV; 26Mg(16O, 14C), E=45 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(74)90042-2
1974SO14 Nucl.Phys. A236, 29 (1974) On the Uranium K = 0 Bands Seen in Two-Nucleon Transfer Reactions NUCLEAR REACTIONS 234,236,238U(p, t), E=17 MeV; calculated σ(Et, θ). 234,236U(t, p), E=15 MeV; 238U(t, p), E=16 MeV; calculated σ(Ep, θ).
doi: 10.1016/0375-9474(74)90218-8
1973SO07 Nucl.Phys. A211, 565 (1973) The 6.05 MeV 0+ State in 16O; A Shape Isomer NUCLEAR REACTIONS 18O(p, t), E=50 MeV; calculated σ(θ). 16O deduced level, B(E2).
doi: 10.1016/0375-9474(73)90444-2
1973SO13 Nucl.Phys. A217, 505 (1973) On the Description of Fermion Systems in Boson Representations (V). A Boson Variational Approach to Collective Motion NUCLEAR STRUCTURE 106,108,110,112,114,116Cd, 122,124,126,128,130Te; calculated quadrupole moment.
doi: 10.1016/0375-9474(73)90408-9
1972AS05 Nucl.Phys. A183, 60 (1972) R.J.Ascuitto, N.K.Glendenning, B.Sorensen The Importance of Indirect Transitions on (p, t) Reactions on Deformed Nuclei NUCLEAR REACTIONS 176Yb, 208Pb, 154Sm(p, t), E=19 MeV; calculated σ(θ); included indirect contributions.
doi: 10.1016/0375-9474(72)90931-1
1972AS06 Nucl.Phys. A186, 641 (1972) Coupling Effects in 208Pb NUCLEAR STRUCTURE 208Pb; calculated levels; analyzed coupling effects. NUCLEAR REACTIONS 206Pb(t, p), 210Pb(p, t), E=20, 20.6 MeV; calculated σ(θ); analyzed 208Pb coupling effects.
doi: 10.1016/0375-9474(72)90988-8
1972AS09 Nucl.Phys. A190, 297 (1972) Spectroscopy with Two-Nucleon Transfer Reactions in Deformed Nuclei (I). Form Factors
doi: 10.1016/0375-9474(72)90143-1
1972AS10 Nucl.Phys. A190, 309 (1972) Spectroscopy with Two-Nucleon Transfer Reactions in Deformed Nuclei (II). Rare-Earth K = 0 Bands Studied with the (p, t) Reaction NUCLEAR REACTIONS 160Gd, 186W(p, t), E=18 MeV; 174,176Yb(p, t), E=19 MeV; analyzed σ(θ). 154Sm, 158,160Gd, 172,174,176Yb, 182,184,186W; calculated levels, B(E2).
doi: 10.1016/0375-9474(72)90144-3
1972KI05 Phys.Rev.Lett. 29, 71 (1972) C.H.King, R.J.Ascuitto, N.Stein, B.Sorensen Evidence for Strong Inelastic Processes in (p, t) Reactions on Deformed Nuclei NUCLEAR REACTIONS 186W(p, t), E=18 MeV; measured σ(θ); deduced inelastic contributions.
doi: 10.1103/PhysRevLett.29.71
1972SH21 Phys.Rev. C6, 1082 (1972) J.D.Sherman, B.G.Harvey, D.L.Hendrie, M.S.Zisman, B.Sorensen Strong and Weak 0+ Excitations in the 142Ce(p, t)140Ce and 140Ce(p, t)138Ce Reactions NUCLEAR REACTIONS 142Ce(p, t), 140Ce(p, t), E=30 MeV; measured σ(Et, θ). 138,140Ce deduced levels, L.
doi: 10.1103/PhysRevC.6.1082
1971AS02 Phys.Lett. 34B, 17 (1971) R.J.Ascuitto, N.K.Glendenning, B.Sorensen Confirmation of Strong Second Order Processes in (p, t) Reactions on Deformed Nuclei NUCLEAR REACTIONS 176Yb(p, t), E=19 MeV; calculated σ(θ); deduced second-order processes.
doi: 10.1016/0370-2693(71)90493-X
1971AS04 Nucl.Phys. A170, 65 (1971) R.J.Ascuitto, N.K.Glendenning, B.Sorensen Twice Double-Transfer in Inelastic Proton Scattering Processes Involving Collective Pairing States, Studied in a Coupled Channels Formalism NUCLEAR REACTIONS 48Ca(p, p'), (p, p), E=12, 18, 30 MeV; calculated σ(θ). Coupled-channel formalism.
doi: 10.1016/0375-9474(71)90683-X
1971SO03 Phys.Lett. 35B, 8 (1971) Can Phenomenological Particle-Particle and Particle-Hole Forces Be Distinguished (Question) NUCLEAR STRUCTURE 210Pb; calculated levels, σ(θ) for 208Pb(t, p).
doi: 10.1016/0370-2693(71)90425-4
1971SO04 Phys.Lett. 35B, 101 (1971) Static Quadrupole Moment of the Collective Octupole Vibration in 208Pb NUCLEAR MOMENTS 208mPb; calculated quadrupole moment. Anharmonic couplings.
doi: 10.1016/0370-2693(71)90229-2
1971SO10 Nucl.Phys. A177, 465 (1971) Fractionation of the Pair Vibrational State in Zirconium NUCLEAR STRUCTURE 90Zr; calculated levels, wave functions, coupling between pairing vibration, 2-phonon p-H excitation.
doi: 10.1016/0375-9474(71)90304-6
1970SO01 Nucl.Phys. A142, 392 (1970) On the Description of Fermion Systems in Boson Representations (III). Normal Mode Construction and the Derivation of Kinetic and Potential Energy Expansion NUCLEAR STRUCTURE 116Sn, 152Sm; calculated levels. Boson representation.
doi: 10.1016/0375-9474(70)90538-5
1970SO02 Nucl.Phys. A142, 411 (1970) On the Description of Fermion Systems in Boson Representations (IV). Numerical Calculation of Quadrupole Excitations in Cd, Sn, Te, Sm and Pb NUCLEAR STRUCTURE 114Cd, 116,120Sn, 122Te, 148,150,152Sm, 206,208,210Pb; calculated levels, equipotential surfaces. Pairing+quadrupole model, boson expansion method.
doi: 10.1016/0375-9474(70)90539-7
1969SO02 Phys.Letters 28B, 633 (1969) A Comment on the Reaction 10B(t, p)12B NUCLEAR REACTIONS 10B(t, p), E not given; measured σ(θ); deduced reaction mechanism. 12B deduced J, π, L.
doi: 10.1016/0370-2693(69)90206-8
1969SO08 Nucl.Phys. A134, 1(1969) Neutron Pairing States in Doubly Even Nuclei NUCLEAR STRUCTURE He, C, O, Ne, Mg, Si, S, Ar, Ca, Ti, Cr, Fe, Ni, Zn, Sr, Zr, Cd, Sn, Te, Ce, Nd, Sm, Pb, U isotopes; calculated neutron pairing states.
doi: 10.1016/0375-9474(69)90682-4
1968BR06 Nucl.Phys. A109, 353 (1968) R.A.Broglia, A.Molinari, B.Sorensen Spin Vibrational 1+ States in 208Pb NUCLEAR STRUCTURE 208Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0375-9474(68)90599-X
1968BR13 Nucl.Phys. A115, 273 (1968) R.A.Broglia, C.Riedel, B.Sorensen, T.Udagawa The Pairing Vibrational Model and the Analysis of the 116,118Sn(t, p) Reactions
doi: 10.1016/0375-9474(68)90004-3
1967SO03 Phys.Letters 24B, 328 (1967) Microscopic Boson Description of Vibrational States in 114Cd
doi: 10.1016/0370-2693(67)90234-1
1960RE09 Phys.Rev. 119, 2017 (1960) R.B.Regier, W.H.Burgus, R.L.Tromp, B.H.Sorensen Ratio of Asymmetric to Symmetric Fission of Pu239 and Pu241 as a Function of Neutron Energy NUCLEAR REACTIONS 239Pu(n, f), 241Pu(n, f), E=0.06-0.36 eV; measured products, 115Cd, 99Mo, 121Sn, 125Sn; deduced yields. Data were imported from EXFOR entry 14078.
doi: 10.1103/PhysRev.119.2017
1953AM08 Phys.Rev. 91, 68 (1953) D.P.Ames, M.E.Bunker, L.M.Langer, B.M.Sorensen The Disintegration of Sr91 and Y91m
doi: 10.1103/PhysRev.91.68
1950SO57 Phys.Rev. 79, 1007 (1950) B.N.Sorensen, B.M.Dale, J.D.Kurbatov Disintegration Scheme of Scandium
doi: 10.1103/PhysRev.79.1007
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