NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = S.M.Abecasis Found 21 matches. 1986HE04 Z.Phys. A323, 105 (1986) Structure of 87Y NUCLEAR STRUCTURE 87Y; calculated levels, J, π, δ. Extended cluster-phonon model, quadrupole, octupole vibrations, particle, particle-hole excitations.
1986HE14 Z.Phys. A324, 403 (1986) Proton-Neutron Interactions in Nuclei with A ≈ 90 NUCLEAR STRUCTURE 87,89Sr, 88,90Y; calculated levels, J, π, S, quadrupole moment, μ, T1/2. Extended cluster phonon model.
1983HE05 Phys.Rev. C27, 1765 (1983) Cluster (Quadrupole-Octupole) Phonon Model: Application to 89Y NUCLEAR STRUCTURE 89Y; calculated levels, B(λ), S, quadrupole, magnetic moments, T1/2. Cluster-phonon model.
doi: 10.1103/PhysRevC.27.1765
1983HE15 Phys.Rev. C28, 1843 (1983) Structure of 51Cr NUCLEAR STRUCTURE 51Cr; calculated levels, J, π, B(λ), quadrupole moment, μ, T1/2, S. Cluster-phonon model, particle-hole excitations.
doi: 10.1103/PhysRevC.28.1843
1980AB09 Phys.Rev. C22, 2237 (1980) S.M.Abecasis, J.Davidson, M.Davidson Particle-core Coupling Model Applied to 89Y, 87Sr, and 89Sr NUCLEAR STRUCTURE 89Y, 87,89Sr; calculated levels, J, π, S, B(E2), quadrupole moment, μ. Particle-core coupling model.
doi: 10.1103/PhysRevC.22.2237
1979AB03 Phys.Rev. C19, 1535 (1979) Classical Semimicroscopic Model Applied to Doubly Even Titanium Isotopes NUCLEAR STRUCTURE 44,46,48,52Ti; calculated levels, J, π, B(E2), B(M1), μ, δ, T1/2, branching ratios, quadrupole moment. Classical semi-microscopic model.
doi: 10.1103/PhysRevC.19.1535
1976AB06 Z.Phys. A278, 309 (1976) S.M.Abecasis, O.Civitarese, F.Krmpotic Analysis of Odd-Mass Technetium Isotopes with the Alaga Model NUCLEAR STRUCTURE 95,97,99,101Tc; calculated levels, quadrupole moment, μ, T1/2, B(λ), δ, γ-branching. Alaga model.
doi: 10.1007/BF01437743
1975AB01 Phys.Rev. C11, 1015 (1975) S.M.Abecasis, C.A.Heras, F.Krmpotic Application of the Generalized Semimicroscopic Model to 1f7/2 Nuclei NUCLEAR STRUCTURE 49Ti, 51Cr, 57Co; calculated levels, J, π, S, quadrupole moment, μ, B(λ), γ-mixing, T1/2.
doi: 10.1103/PhysRevC.11.1015
1975BO29 Z.Phys. A273, 373 (1975) H.E.Bosch, J.Davidson, V.Silbergleit, C.A.Heras, S.M.Abecasis Studies on the Nuclear Structure of 115In RADIOACTIVITY 115m,115Cd; measured Eβ, Eγ, Iγ, βγ-, γγ-coin, γγ(θ); deduced Q, β shape factors. 115In deduced levels, δ.
doi: 10.1007/BF01435579
1975HE22 Phys.Rev. C12, 1659 (1975) Structure of 1f7/2 and 1g9/2 Nuclei NUCLEAR STRUCTURE 57Co, 115In; calculated levels, J, π, B(λ), μ, quadrupole moment. Cluster-phonon model.
doi: 10.1103/PhysRevC.12.1659
1975HE23 Can.J.Phys. 53, 1651 (1975) Phenomenological Description of High Spin States in Doubly Even Rare Earths NUCLEAR STRUCTURE 156,158,160,162,164Er, 158,160,162Dy; calculated backbending.
doi: 10.1139/p75-210
1974AB02 Phys.Rev. C9, 2320 (1974) S.M.Abecasis, O.Civitarese, F.Krmpotic Generalized Semimicroscopic Model in Odd-Mass Indium Isotopes NUCLEAR STRUCTURE 115,117In; calculated levels, J, π, B(E2), B(M1), quadrupole moment, μ, S. Generalized semimicroscopic model.
doi: 10.1103/PhysRevC.9.2320
1973AB01 Nucl.Phys. A205, 475 (1973) Extension of the Asymmetric Rotor with Variable-Moment-of-Inertia Model Toward Quasi-Bands NUCLEAR STRUCTURE A=18-210; calculated energy ratios for even-even nuclei.
doi: 10.1016/0375-9474(73)90700-8
1973MA27 Z.Phys. 262, 39 (1973) H.J.Mang, F.Krmpotic, S.M.Abecasis On the Coexistence of Deformed and Spherical States in Odd-Mass Nuclei NUCLEAR STRUCTURE 109,111,113,115,117,119,121,123In; calculated matrix elements, levels, J, π, B(E2).
doi: 10.1007/BF01394806
1972AB01 Nucl.Phys. A180, 485 (1972) Asymmetric Rotor with Variable Moment-of-Inertia Model NUCLEAR STRUCTURE A=118-190; calculated ground-state, γ-vibrational bands. Asymmetric rotor, variable moment-of-inertia model.
doi: 10.1016/0375-9474(72)90874-3
1971AB09 Nuovo Cim. 6A, 365 (1971) S.M.Abecasis, F.Krmpotic, A.Plastino Analysis of 63,65Cu(3He, d)64,66Zn Reaction in the Unified Model NUCLEAR REACTIONS 63,65Cu(3He, d), 64,66Zn(t, α); analyzed data. 64,66Zn 63,65Cu levels deduced S.
doi: 10.1007/BF02728580
1970AB08 Nucl.Phys. A151, 641 (1970); Erratum Nucl.Phys. A166, 675 (1971) Unique First Forbidden β-Transitions RADIOACTIVITY 42K, 86Rb, 90Y, 90Sr, 142Pr, 166Ho; calculated β-spectrum shape factors.
doi: 10.1016/0375-9474(70)90402-1
1968BO04 Nucl.Phys. A108, 209 (1968) H.E.Bosch, A.J.Haverfield, E.Szichman, S.M.Abecasis High-Resolution Studies in the Decay of 133Ba with Semiconductor Counters RADIOACTIVITY 133Ba;measured Eγ, Iγ, I(ce), γγ-, γce-coin, ICC; deduced log ft. 133Cs deduced levels, J, π. Ge(Li) detector.
doi: 10.1016/0375-9474(68)90154-1
1967BO18 Phys.Rev. 159, 1029(1967) H.E.Bosch, M.C.Simon, E.Szichman, L.Gatto, S.M.Abecasis Disintegration of Sn113 NUCLEAR STRUCTURE 113Sn; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.159.1029
1967BO45 LR16 (1967) H.E.Bosch, A.J.Haverfield, E.Szichman, S.M.Abecasis High Resolution Studies in the Decay of Ba133 with Semiconductor Counters RADIOACTIVITY 133Ba; measured Eγ, Iγ, I(ce), ceγ-, γγ-coin, ICC, K/LM ratios; deduced log ft. 133Cs deduced levels, J, π, ICC, γ-mixing, γ-branching.
1964BO24 J. Inorg. Nucl. Chem. 26, 1337 (1964) H.E.Bosch, S.M.Abecasis, E.Ansaldo, A.Jech, M.Mariscotti The Non Existence of the 92m-Nb Isomer NUCLEAR STRUCTURE 92Nb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(64)80112-3
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