NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.P.Davidson Found 13 matches. 1978CL03 Phys.Rev. C17, 1433 (1978) D.A.Close, J.J.Malanify, J.P.Davidson Nuclear Charge Distributions Deduced from the Muonic Atoms of 232Th, 235U, 238U, and 239Pu ATOMIC PHYSICS, Mesic-Atoms 232Th, 235,238U, 239Pu(μ-, X-ray); measured muonic X-rays; deduced nuclear charge distribution, quadrupole moment.
doi: 10.1103/PhysRevC.17.1433
1976CL04 Nuovo Cim. 34A, 301 (1976) D.A.Close, J.J.Malanify, J.P.Davidson Nuclear Polarization Deduced from Muonic 208Pb Measurements ATOMIC PHYSICS, Mesic-Atoms 208Pb(μ-, X-ray); measured muonic X-rays; deduced charge distribution, nuclear polarization.
doi: 10.1007/BF02786993
1974DA03 Phys.Rev.Lett. 32, 337 (1974) J.P.Davidson, D.A.Close, J.J.Malanify Evidence for Higher Shape Deformations in Muonic X Rays NUCLEAR REACTIONS 232Th, 238U(μ, X-ray); measured muonic X-rays. 232Th, 238U, 152Sm, 162Dy, 170Er, 182W deduced deformation parameters.
doi: 10.1103/PhysRevLett.32.337
1972KA04 Nucl.Phys. A180, 638 (1972) Excitation of Deformation Vibrations by Radiationless Muonic Transitions NUCLEAR STRUCTURE 182W; analyzed resonances between muonic, nuclear states.
doi: 10.1016/0375-9474(72)90885-8
1972MA11 Nucl.Phys. A183, 371 (1972) A Single-Particle Model Calculation of Total Energy Surfaces in Heavy Nuclei NUCLEAR STRUCTURE, Fission 236U, 230,232Th, 234,236,238U, 246,248,250,252Cf, 238,240,242,244Am, 236,238,240,242,244Pu, 240,242,244,246,248,250Cm; calculated total energy surfaces, fission barriers. Single-particle model.
doi: 10.1016/0375-9474(72)90665-3
1971KA13 Phys.Rev.Lett. 27, 158 (1971) Possible Resonance in Muonic W182 ATOMIC PHYSICS, Mesic-Atoms 182W; calculated μ-mesic resonance excitation probability. 182W; calculated μ-mesic resonance excitation probability.
doi: 10.1103/PhysRevLett.27.158
1970AV04 Phys.Rev. C2, 1934 (1970) Higher-Order Deformations and Electric Monopole Transitions in Deformed Nuclei NUCLEAR STRUCTURE 152Sm, 168Yb, 174,178Hf; calculated E0 transition parameters. Higher-order deformations.
doi: 10.1103/PhysRevC.2.1934
1970BE87 Can.J.Phys. 48, 2542 (1970) D.A.Bell, C.A.Aveledo, M.G.Davidson, J.P.Davidson Table of E0 Conversion Probability Electronic Factors NUCLEAR STRUCTURE Z=40-102; calculated E0 conversion probability electronic factors. Relativistic calculations, finite nuclear size, bound state atomic screening effects included.
doi: 10.1139/p70-318
1968DA28 Collective Models of the Nucleus, Chapt.4, P57, Pure and Applied Physics Vol.29, Academic Press, New York (1968) Models of Odd-A Nuclei
1965DA13 Rev.Mod.Phys. 37, 105 (1965) Rotations and Vibrations in Deformed Nuclei NUCLEAR STRUCTURE 24,26Mg, 42Ca, 56Fe, 82Kr, 96Mo, 102Ru, 106Pd, 134Ba, 150,152,154Sm, 154,156Gd, 160Dy, 166,168Er, 172Yb, 182,184,186W, 184,186,188,190,192Os, 192,194,196Pt, 200Hg, 214Po, 228Th, 232,234U, 238Pu, 250Cf, 254Fm; analyzed available data; deduced systematics of a rigid top, nuclear properties.
doi: 10.1103/revmodphys.37.105
1963CH02 Phys.Rev. 131, 366 (1963) Asymmetric Core Collective Model for Odd A Nuclei with Applications to the 2s-1d Shell
doi: 10.1103/PhysRev.131.366
1957DA09 Bull.Am.Phys.Soc. 2, No.7, 351, N12 (1957) J.P.Davidson, A.P.Patro, R.Woldseth γ, 2p Reaction in Aluminum
1951DA33 Phys.Rev. 82, 48 (1951) The First Forbidden Shape Factor and the f(n)t Products for Beta-Decay
doi: 10.1103/PhysRev.82.48
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