NSR Query Results
Output year order : Descending NSR database version of May 22, 2024. Search: Author = L.Jaqua Found 6 matches. 1994BA24 Nucl.Phys. A570, 23c (1994) B.R.Barrett, D.C.Zheng, L.Jaqua, J.P.Vary, R.J.McCarthy Realistic Microscopic Calculations for the Light Nuclei A = 2 to 7 NUCLEAR STRUCTURE ^{4,5}He, ^{6,7}Li; calculated levels. Realistic microscopic calculation.
doi: 10.1016/0375-9474(94)90266-6
1994JA08 Nucl.Phys. A571, 242 (1994) L.Jaqua, P.Halse, B.R.Barrett, J.P.Vary Effective Shell-Model Interaction for No-Core Model Spaces NUCLEAR STRUCTURE ^{4}He; calculated binding energy vs intermediate state excitation energy; deduced model convergence features. Effective shell-model interaction, no-core model spaces.
doi: 10.1016/0375-9474(94)90059-0
1993JA11 Phys.Rev. C48, 1765 (1993) L.Jaqua, D.C.Zheng, B.R.Barrett, J.P.Vary Effects of the Single-Particle Potential Insertions in the Effective Interaction NUCLEAR STRUCTURE ^{4}He, ^{6}Li; calculated levels. Different ways of single particle potential insertions in effective interaction.
doi: 10.1103/PhysRevC.48.1765
1993ZH15 Phys.Rev. C48, 1083 (1993) D.C.Zheng, B.R.Barrett, L.Jaqua, J.P.Vary, R.J.McCarthy Microscopic Calculations of the Spectra of Light Nuclei NUCLEAR STRUCTURE ^{4,5}He, ^{6,7}Li; calculated ground state energies, levels. Large shell model space, realistic interactions, G-matricies.
doi: 10.1103/PhysRevC.48.1083
1992JA13 Phys.Rev. C46, 2333 (1992) L.Jaqua, M.A.Hasan, J.P.Vary, B.R.Barrett Kinetic-Energy Operator in the Effective Shell-Model Interaction NUCLEAR STRUCTURE ^{16,17}O; calculated single-particle energies; deduced center-of-mass kinetic energy role in relating these to observed removal energies. Effective shell model interactions.
doi: 10.1103/PhysRevC.46.2333
1991CO12 Phys.Rev. C44, 203 (1991) Wave Function Effects and the Elastic Magnetic Form Factor of ^{17}O NUCLEAR REACTIONS ^{17}O(e, e), E not given; calculated magnetic form factor; deduced valence neutron radial wave function model dependence.
doi: 10.1103/PhysRevC.44.203
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