NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.Leon Found 11 matches. 2014CL04 Nucl.Instrum.Methods Phys.Res. B 332, 191 (2014) A.Climent-Font, R.Caballero, E.Punzon-Quijorna, J.M.Merino, M.Leon Deviations from Rutherford elastic scattering cross sections for Cu and Zn with He ions NUCLEAR REACTIONS Cu(α, α), Zn(α, α), E=7.3-10 MeV; measured products, Cu, Zn; deduced σ(θ). Data were imported from EXFOR entry O2227.
doi: 10.1016/j.nimb.2014.02.059
1992LE23 Z.Phys. C56, S203 (1992) Muon-catalyzed fusion theory
doi: 10.1007/BF02426797
1986KA08 Phys.Rev.Lett. 56, 2368 (1986) W.Kanert, F.J.Hartmann, H.Daniel, E.Moser, G.Schmidt, T.von Egidy, J.J.Reidy, M.Nicholas, M.Leon, H.Poth, G.Buche, A.D.Hancock, H.Koch, Th.Kohler, A.Kreissl, U.Raich, D.Rohmann, M.Chardalas, S.Dedoussis, M.Suffert, A.Nilsson First Observation of the E2 Nuclear-Resonance Effect in Antiprotonic Atoms ATOMIC PHYSICS 92,94,95,98,100Mo(p-bar, X), E at 200, 300 MeV/c; measured antiprotonic X-ray spectra; deduced strong interaction widths, shifts, effective (p-bar)-nucleon scattering length, E2 nuclear resonance effect.
doi: 10.1103/PhysRevLett.56.2368
1985RE12 Phys.Rev. C32, 1646 (1985) J.J.Reidy, M.Nicholas, J.N.Bradbury, P.A.M.Gram, R.L.Hutson, M.Leon, M.E.Schillaci, F.J.Hartmann, A.R.Kunselman Measurements of the E2 Resonance Effect in Pionic Atoms NUCLEAR REACTIONS 48Ti, 104Ru, 110Pd, 111,112Cd, 125Te, 150Sm(π, X), E at rest; measured pionic X-rays; deduced E2 resonance effect, X-ray attenuation due to level mixing. 111Cd deduced level energy. ATOMIC PHYSICS, Mesic-Atoms 48Ti, 104Ru, 110Pd, 111,112Cd, 125Te, 150Sm(π, X), E at rest; measured pionic X-rays; deduced E2 resonance effect, X-ray attenuation due to level mixing.
doi: 10.1103/PhysRevC.32.1646
1981LE05 Nucl.Phys. A352, 477 (1981) Relativistic Corrections to Perturbation Theory for Pionic and Kaonic Atoms ATOMIC PHYSICS, Mesic-Atoms Ho, Re; calculated relativistic corrections to pionic level energies. Perturbation theory.
doi: 10.1016/0375-9474(81)90424-3
1979BA07 Phys.Lett. 81B, 165 (1979) C.J.Batty, S.F.Biagi, E.Friedman, S.D.Hoath, J.D.Davies, C.J.Pyle, G.T.A.Squier, D.M.Asbury, M.Leon Pionic X-Rays and the Neutron Radius of 44Ca ATOMIC PHYSICS, Mesic-Atoms 40,44Ca; measured pionic X-rays for 3d→2p; deduced isotopic dependence of strong interaction shifts, rms neutron radii. Effective pion-nucleus potential.
doi: 10.1016/0370-2693(79)90513-6
1979LE13 Nucl.Phys. A322, 397 (1979) M.Leon, J.N.Bradbury, P.A.M.Gram, R.L.Hutson, M.E.Schillaci, C.K.Hargrove, J.J.Reidy Observation of the E2 Nuclear Resonance Effect in Some Pionic Atoms ATOMIC PHYSICS, Fission 48,50Ti, 104,101Ru, 110,108Pd, 112,111,110Cd, 150,152Sm(π-, X-ray), E=at rest; measured I(X-ray); deduced attenuation due to nuclear E2 resonance effect.
doi: 10.1016/0375-9474(79)90434-2
1976LE08 Nucl.Phys. A260, 461 (1976) Hadronic Atoms and Ticklish Nuclei: The E2 Nuclear Resonance Effect NUCLEAR STRUCTURE, Mesic-Atoms 122Cd, 150Sm, 110Pd, 104Ru, 48Ti; calculated E2 resonance effects for pionic atoms. 94,96,98,100Mo, 96Ru, 122Sn, 138Ba, 198Hg; calculated E2 resonance effects for kaonic atoms. 74Ge, 74,78,80,82Se, 102Ru, 104,106Pd, 112,114Cd, 126,128Te, 130Ba, 168Er, 194Pt, 200Hg, 204Pb; calculated E2 resonance effects for hyperonic atoms. 76Se, 94,100Mo, 104Ru, 130Te, 148Nd, 150Sm, 196Pt, 200Hg; calculated E2 resonance effects for antiprotonic atoms.
doi: 10.1016/0375-9474(76)90057-9
1974LE15 Phys.Lett. 50B, 425 (1974) Quadrupole Mixing in Hadronic Atoms: An Additional Probe of the Hadron-Nucleus Interaction NUCLEAR STRUCTURE 98Mo, 96Ru, 122Sn, 138Ba, 198Pt, 198Hg; calculated kaonic X-ray intensity ratios, quadrupole mixing effects.
doi: 10.1016/0370-2693(74)90251-2
1974LE26 Phys.Lett. 53B, 141 (1974) E2 Nuclear Resonance Effect in Pionic Atoms NUCLEAR STRUCTURE, Mesic-Atoms 112Cd, 150Sm, 110Pd, 48Ti, 104Ru; calculated quadrupole resonance effects.
doi: 10.1016/0370-2693(74)90514-0
1962LE21 Phys.Rev. 127, 636 (1962) Negative Meson Absorption in Liquid Hydrogen NUCLEAR REACTIONS H(π-, X), (K-, X), E not given; calculated Auger rates, Stark mixing.
doi: 10.1103/PhysRev.127.636
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