NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = G.L.Strobel Found 25 matches. 2002ST34 Int.J.Theor.Phys. 41, 903 (2002) Spin Dependent Quark Forces and the Spin Content of the Nucleon NUCLEAR STRUCTURE 1n, 1H; calculated nucleon spin content, related features; deduced possible role of spin-dependent quark forces.
doi: 10.1023/A:1015741125390
1999ST15 Int.J.Theor.Phys. 38, 737 (1999) G.L.Strobel, K.V.Shitikova, A.Chikanian Monopole Excitation of the Nucleon in a Relativistic Three-Quark Model NUCLEAR STRUCTURE 1H; calculated proton density, form factors, monopole excitation features. Relativistic three-quark model.
doi: 10.1023/A:1026619726706
1999ST30 Acta Phys.Pol. B30, 2671 (1999) Flux Tube Constant Determined from Proton Form Factor Analysis NUCLEAR STRUCTURE 1H; analyzed form factors; deduced flux tube constant. Quark shell model.
1998ST31 Int.J.Theor.Phys. 37, 2001 (1998) Rest Frame Properties of the Proton NUCLEAR STRUCTURE 1H; calculated proton charge radius, magnetic moment; deduced quark configuration features. Three-body Dirac equation.
doi: 10.1023/A:1026621415068
1997ST16 Phys.Rev. C56, 551 (1997) Ioffe Current Constant of the Roper Resonance from a Relativistic Three Quark Model
doi: 10.1103/PhysRevC.56.551
1997ST27 Acta Phys.Pol. B28, 1595 (1997) Lagrange Triangle Quark Model of the Proton NUCLEAR STRUCTURE 1H; calculated magnetic moment vs quark mass. Lagrange triangle quark model.
1996ST15 Phys.Rev. C54, 888 (1996) Ioffe Current Constant from a Relativistic Three Quark Model
doi: 10.1103/PhysRevC.54.888
1986BA04 Phys.Rev. C33, 732 (1986) Equivalent Local Dirac Potentials and Nuclear Magnetic Moments NUCLEAR MOMENTS 15N; calculated μ. Equivalent local Dirac scalar-tensor, vector-tensor interactions.
doi: 10.1103/PhysRevC.33.732
1984ST09 Phys.Rev. C29, 2365 (1984) G.L.Strobel, C.A.Pearson, S.H.Chao Two-Step Processes in Tritium Decay RADIOACTIVITY 3H(β-); calculated atomic state excitation probabilities following β-decay. Coulomb interaction, two-step processes.
doi: 10.1103/PhysRevC.29.2365
1983BA33 Phys.Rev. C28, 456 (1983) M.Bawin, C.A.Hughes, G.L.Strobel Magnetic Tests for Nuclear Dirac Wave Functions NUCLEAR STRUCTURE 15N; calculated μ. Dirac equation, vector, scalar Woods-Saxon component.
doi: 10.1103/PhysRevC.28.456
1979ST09 Phys.Rev. C20, 364 (1979) Translationally Invariant Spectral Function for 6Li NUCLEAR STRUCTURE 6Li; calculated spectral function for tightly bound protons, fwhm, mean removal energy. Highly collective wave function, hyperspherical harmonic formalism.
doi: 10.1103/PhysRevC.20.364
1978ST19 Phys.Rev. C18, 2395 (1978) Six-Body Hyperspherical Solution to 6Li Bound States NUCLEAR STRUCTURE 6Li; calculated binding energy of 15.245-MeV state. Hyperspherical method to solve N-body Schrodinger equation.
doi: 10.1103/PhysRevC.18.2395
1976ST17 Nucl.Phys. A271, 162 (1976) A K-Harmonics Description of 16O Breathing Mode NUCLEAR STRUCTURE 16O; calculated breathing mode. K-harmonics calculation.
doi: 10.1016/0375-9474(76)90273-6
1974GE15 Nuovo Cim. 23A, 447 (1974) H.V.Geramb, G.L.Strobel, R.Sprickmann Giant-Dipole-Resonance Effects in the 90Zr(p, p') 0+1 to 0+2 Transition NUCLEAR REACTIONS 90Zr(p, p'), E=12.7, 18.8, 40 MeV; calculated σ(E, Ep', θ).
1974ST16 Phys.Rev.Lett. 33, 1392 (1974) Isospin-Conservation Violation in Two-Nucleon Transfer Reactions NUCLEAR REACTIONS 16O(p, 3He), (p, t), E=27 MeV; calculated σ(E(3He), θ), σ(Et, θ); deduced isospin conservation violation.
doi: 10.1103/PhysRevLett.33.1392
1974ST18 Phys.Rev. C10, 2153 (1974) Target Correlations in the Continuous (d, 3He) Reaction Spectrum NUCLEAR REACTIONS 12C(d, 3He); calculated 3He spectrum.
doi: 10.1103/PhysRevC.10.2153
1973FA02 Nucl.Phys. A203, 513 (1973) A.Faessler, S.Kusuno, G.L.Strobel The 16O(d, 3He) Excitation Spectrum NUCLEAR REACTIONS 16O(d, 3He); calculated excitation spectrum.
doi: 10.1016/0375-9474(73)90361-8
1973GE01 Nucl.Phys. A199, 545 (1973) H.V.Geramb, R.Sprickmann, G.L.Strobel Excitation of Giant Multipole Resonances L = 1-4 in the 16O(p, p') Spin-Flip Transition NUCLEAR REACTIONS 16O(p, p'), E=23-46 MeV; analyzed σ(E;θ) 17F deduced resonances, level-width.
doi: 10.1016/0375-9474(73)90597-6
1973ST16 Nucl.Phys. A210, 67 (1973) The Continuous 3He Spectrum from Deuterons Incident on 12C NUCLEAR REACTIONS 12C(d, 3He), E=52 MeV; calculated σ(E(3He)).
doi: 10.1016/0375-9474(73)90504-6
1972GE07 Phys.Lett. 39B, 611 (1972) Two Step Process in the 16O(p, 2p)15N Reaction NUCLEAR REACTIONS 16O(p, 2p), E=45 MeV; calculated σ(Ep, θ(p)). 2-step mechanism, core polarization term.
doi: 10.1016/0370-2693(72)90010-X
1972GE16 Lett.Nuovo Cim. 5, 333 (1972) H.V.Geramb, G.L.Strobel, R.Sprickmann Evidence for Core Polarization Exchange Contribution in Inelastic Scattering
1972ST29 Phys.Rev.Lett. 29, 1406 (1972) Energy-Dependent Two-Proton t Matrix in (p, 2p) Reactions NUCLEAR REACTIONS 12C, 16O(p, 2p), E=45, 50 MeV; calculated σ(θ). Energy-dependent t-matrix.
doi: 10.1103/PhysRevLett.29.1406
1972ST33 Phys.Rev. C6, 2039 (1972) Three-Body Model for Proton-Induced Reaction on 12C NUCLEAR REACTIONS 12C(p, 2p), (p, d), E=46, 30 MeV; calculated σ(θ). 3-body model.
doi: 10.1103/PhysRevC.6.2039
1972ST34 Z.Phys. 256, 210 (1972) Boundary Condition Model for Diffractive Elastic Scattering NUCLEAR REACTIONS 63Cu(d, d), E=11.8 MeV; 6Li(d, d), E=19.6 MeV; 6Li(3He, 3He), E=24.6, 27, 34 MeV; 4He(α, α), E=41 MeV; 12C, 14N, 16O(6Li, 6Li), E=30 MeV; 28Si(6Li, 6Li), E=30 MeV; analyzed σ(θ). Boundary condition model, diffractive scattering.
doi: 10.1007/BF01392094
1970DA17 Nucl.Phys. A156, 600 (1970) Nuclear Bremsstrahlung from a Spin-Zero Target NUCLEAR REACTIONS 12C(p, p), (p, p'γ), E=140 MeV; calculated σ(θ), bremsstrahlung spectrum.
doi: 10.1016/0375-9474(70)90255-1
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