NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.C.Nemes Found 14 matches. 2006HI01 Nucl.Phys. A769, 53 (2006) B.Hiller, A.L.Mota, M.C.Nemes, A.A.Osipov, M.Sampaio The role of hidden ambiguities in the linear sigma model with fermions
doi: 10.1016/j.nuclphysa.2006.02.002
1999MO18 Nucl.Phys. A652, 73 (1999) A.L.Mota, M.C.Nemes, B.Hiller, H.Walliser Meson Properties in a Renormalizable Version of NJL Model
doi: 10.1016/S0375-9474(99)00147-5
1997CA14 Nucl.Phys. A617, 464 (1997) H.C.G.Caldas, D.H.T.Franco, A.L.Mota, F.A.Oliveira, M.C.Nemes Simple Parametrizations of Light Meson Properties in Hot or Dense Matter
doi: 10.1016/S0375-9474(96)00435-6
1996BA47 Nucl.Phys. A604, 406 (1996) B.Bajc, A.H.Blin, B.Hiller, M.C.Nemes, A.A.Osipov, M.Rosina Low-Energy Dynamics of the γγ → ππ Reaction in the NJL Model
doi: 10.1016/0375-9474(96)00167-4
1995BR03 Nucl.Phys. A582, 717 (1995) Nuclear Coherent Versus Incoherent Effects in Peripheral RHI Collisions NUCLEAR REACTIONS 27Al, C, Cu, Sn, Pb(28Si, X), E=14.5 GeV/nucleon; analyzed projectile one-nucleon removal data; deduced nuclear coherent vs incoherent effects role, peripheral relativistic heavy ion collisions.
doi: 10.1016/0375-9474(94)00479-7
1995FL05 Z.Phys. A352, 197 (1995) S.P.Flego, A.H.Blin, B.Hiller, M.C.Nemes Pion, Sigma and Nucleon Propagators in the Linear σ-Model
doi: 10.1007/BF01298908
1994BA90 Z.Phys. A350, 229 (1994) B.Bajc, A.H.Blin, B.Hiller, M.C.Nemes, M.Rosina Momentum Dependent Vertices σγγ, σργ and σρρ: The NJL scalar hidden by chiral symmetry
doi: 10.1007/BF01289587
1994EI01 J.Phys.(London) G20, 261 (1994) On Nucleon-Nucleus Scattering and the Relativistic Eikonal Approximation
doi: 10.1088/0954-3899/20/2/006
1987GO23 Phys.Rev. C35, 2341 (1987) L.Gonzaga Ferreira Filho, M.C.Nemes Nuclear Photabsorption Cross Section: Collective and quasi-deuteron contributions NUCLEAR REACTIONS 208Pb(γ, X), E ≤ 139 MeV; calculated photoabsorption σ(E); deduced collective, quasideuteron contributions characteristics. Phenomenological model.
doi: 10.1103/PhysRevC.35.2341
1985MO02 Nucl.Phys. A433, 671 (1985) E.Moeller, M.C.Nemes, D.H.E.Gross Monte Carlo Simulation of Carbon Fragmentation at High Energies NUCLEAR REACTIONS 12C(p, X), E=high; calculated target fragmentation; deduced dominant decay channels, Coulomb interaction role. Monte Carlo simulation.
doi: 10.1016/0375-9474(85)90024-7
1983GR26 Phys.Lett. 130B, 131 (1983) Remarkable Long-Range-Systematics in the Binding Energies of α-Nuclei NUCLEAR STRUCTURE A=4-72; calculated two-nucleon separation energy; deduced evidence for α-structure.
doi: 10.1016/0370-2693(83)91026-2
1983KR16 Z.Phys. A314, 23 (1983) H.J.Krappe, K.Mohring, M.C.Nemes, H.Rossner On the Interpretation of Heavy-Ion Sub-Barrier Fusion Data NUCLEAR REACTIONS, ICPND 10B(10B, X), E(cm) ≈ 2-4 MeV; 14N(10B, X), E(cm) ≈ 2.75-7 MeV; 12C(16O, X), E(cm)=4-12 MeV; 14N(16O, X), E(cm)=5.5-12 MeV; 20Ne(12C, X), E(cm)=6-15 MeV; 9Be(16O, X), E(cm)=2.5-5 MeV; 12C(12C, X), E(cm)=2.5-5.5 MeV; 14N(12C, X), E(cm)=3.5-10 MeV; 14N(14N, X), E(cm)=4.5-11 MeV; 16O(16O, X), E(cm)=7-14.5 MeV; 110Pd(12C, X), E(cm)=30-50 MeV; 64,58Ni(58Ni, X), 64Ni(64Ni, X), E(cm)=90-110 MeV; 122Sn(40Ar, X), E=102.5-130 MeV; calculated fusion σ(E); deduced subbarrier fusion characteristics, neck formation role. Two-dimensional tunneling model.
doi: 10.1007/BF01411825
1980MC05 Z.Phys. A295, 177 (1980) Direct-Reaction Contributions to Projectile-Fragment Spectra at 10-20 MeV/Nucleon NUCLEAR REACTIONS 208Pb(16O, 15N), (16O, 12C), E=140-315 MeV; calculated σ(E(12C)), σ(E(15N)), spectral widths; deduced energy dependence of reaction mechanism. Direct reaction model.
doi: 10.1007/BF01413075
1979FR11 Phys.Lett. 87B, 179 (1979) W.A.Friedman, K.W.McVoy, M.C.Nemes A Resonant Interpretation of Gross Structure in 12C + 12C and 16O + 16O Inelastic Scattering NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=10-30 MeV; 16O(16O, 16O'), E(cm)=24-30 MeV; calculated σ(E). Barrier-top-resonance model.
doi: 10.1016/0370-2693(79)90959-6
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