NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.T.Pena Found 36 matches. 2016MA09 J.Phys.(London) G43, 023002 (2016) L.E.Marcucci, F.Gross, M.T.Pena, M.Piarulli, R.Schiavilla, I.Sick, A.Stadler, J.W.Van Orden, M.Viviani Electromagnetic structure of few-nucleon ground states NUCLEAR REACTIONS 2,3H, 3,4He(E, E), E not given; analyzed available data; deduced experimental form factors of the hydrogen and helium isotopes, extracted from an up-to-date global analysis of σ and polarization observables measured in elastic electron scattering from these systems.
doi: 10.1088/0954-3899/43/2/023002
2014BI17 Few-Body Systems 55, 705 (2014) E.P.Biernat, F.Gross, M.T.Pena, A.Stadler Quark Mass Functions and Pion Structure in Minkowski Space
doi: 10.1007/s00601-014-0863-x
2014ST20 Few-Body Systems 55, 701 (2014) A.Stadler, S.Leitao, M.T.Pena, E.P.Biernat Singularity-Free Two-Body Equation with Confining Interactions in Momentum Space
doi: 10.1007/s00601-013-0746-6
2008GA30 Eur.Phys.J. A 38, 209 (2008) np → ηd near threshold and the s-wave ηN amplitude NUCLEAR REACTIONS 1H(n, dX), E(cm)=0-60 MeV; calculated η-meson production σ. Relativistic three-body model.
doi: 10.1140/epja/i2008-10662-x
2008GR02 Phys.Rev. C 77, 015202 (2008) Pure S-wave covariant model for the nucleon
doi: 10.1103/PhysRevC.77.015202
2008GR06 Phys.Rev. C 77, 035203 (2008) Fixed-axis polarization states: covariance and comparisons
doi: 10.1103/PhysRevC.77.035203
2008RA16 Eur.Phys.J. A 36, 329 (2008) A covariant model for the nucleon and the Δ
doi: 10.1140/epja/i2008-10599-0
2006MA70 Phys.Rev. C 74, 042201 (2006) V.Malafaia, M.T.Pena, Ch.Elster, J.Adam, Jr. Charged- and neutral-pion production in the S-matrix approach NUCLEAR REACTIONS 1H(p, pπ0), (p, pπ+), (n, pπ-), E=280-330 MeV; calculated pion production σ. S-matrix approach, comparison with data.
doi: 10.1103/PhysRevC.74.042201
2006PE19 Acta Phys.Slovaca 56, 261 (2006) Study of the np → ηd reaction within a three-body model NUCLEAR REACTIONS 1H(n, dX), E ≈ threshold; calculated η-meson production σ. Three-body model.
2006RA17 Few-Body Systems 39, 123 (2006) G.Ramalho, A.Arriaga, M.T.Pena Solution of the Spectator Equation for Relativistic NN Scattering Without Partial Wave Expansion NUCLEAR REACTIONS 1H(n, n'), E=99-319 MeV; calculated scattering amplitudes, σ(θ). Solution to covariant spectator equation without partial wave expansion.
doi: 10.1007/s00601-006-0161-3
2005GA27 Phys.Rev. C 72, 014003 (2005) Relativistic description of the np → ηd reaction near threshold NUCLEAR REACTIONS 1H(n, dX), E(cm)=0-120 MeV; calculated η-meson production σ; deduced role of final state interaction, relativistic effects, related features. Comparisons with data.
doi: 10.1103/PhysRevC.72.014003
2005MA20 Phys.Rev. C 71, 034002 (2005) V.Malafaia, J.Adam, Jr., M.T.Pena Pion rescattering operator in the S-matrix approach
doi: 10.1103/PhysRevC.71.034002
2004AD11 Phys.Rev. C 69, 034008 (2004) J.Adam, Jr., M.T.Pena, A.Stadler Short-range three-nucleon forces and low-energy constants NUCLEAR STRUCTURE 3H; calculated binding energies, three-nucleon force contributions, parameter dependences. Several models compared.
doi: 10.1103/PhysRevC.69.034008
2004GR07 Phys.Rev. C 69, 034007 (2004) Electromagnetic interactions of three-body systems in the covariant spectator theory
doi: 10.1103/PhysRevC.69.034007
2004MA13 Phys.Rev. C 69, 024001 (2004) Pion rescattering in π0 production NUCLEAR REACTIONS 1H(p, pπ0), E ≈ 290-440 MeV; calculated σ, pion rescattering effects, pion-nucleon amplitude. Non-relativistic reductions.
doi: 10.1103/PhysRevC.69.024001
2002GA36 Phys.Rev. C66, 034606 (2002) The Reaction np → ηd Near Threshold NUCLEAR REACTIONS 1H(n, X)2H, E(cm)=0-120 MeV; calculated η meson production σ; deduced reaction mechanism features. Comparison with data.
doi: 10.1103/PhysRevC.66.034606
2002RA08 Phys.Rev. C65, 034008 (2002) G.Ramalho, A.Arriaga, M.T.Pena Relativistic Effects and Quasipotential Equations
doi: 10.1103/PhysRevC.65.034008
2001DI20 Phys.Rev. C64, 044603 (2001) J.Dias de Deus, M.T.Pena, J.C.Seixas Multiplicity Distributions Associated to Subthreshold Events in Heavy-Ion Collisions NUCLEAR REACTIONS 12C(12C, π0X), E ≈ 30-90 MeV/nucleon; analyzed σ. 27Al(36Ar, π0X), (36Ar, X), E not given; analyzed fragment multiplicities; deduced subthreshold meson production mechanism features.
doi: 10.1103/PhysRevC.64.044603
2001GA06 Phys.Rev. C63, 021001 (2001) Nonexistence of a ηNN Quasibound State NUCLEAR STRUCTURE 2H; calculated η meson elastic scattering σ, scattering lengths; deduced no quasibound state. Solution of Fadeev equations.
doi: 10.1103/PhysRevC.63.021001
2001PE03 Nucl.Phys. A683, 322 (2001) M.T.Pena, H.Garcilazo, D.O.Riska The Reaction pp → ppη and the eta-Nucleon and Nucleon-Nucleon Interactions NUCLEAR REACTIONS 1H(p, pX), E=1260-1340 MeV; calculated η meson production σ, meson exchange contributions; deduced coupling constant. Comparison with data.
doi: 10.1016/S0375-9474(00)00449-8
2001RA26 Nucl.Phys. A689, 511c (2001) G.Ramalho, A.Arriaga, M.T.Pena Relativistic NN Scattering Equations without Partial-Wave Decomposition NUCLEAR REACTIONS 1H(p, p), (n, n), E=300, 800 MeV; calculated scattering amplitudes.
doi: 10.1016/S0375-9474(01)00893-4
2000GA28 Phys.Rev. C61, 064010 (2000) ηd Scattering in the Region of the S11 Resonance
doi: 10.1103/PhysRevC.61.064010
2000GA29 Phys.Rev. C62, 011002 (2000) πd → ηNN Reaction Near Threshold NUCLEAR REACTIONS 2H(π, nX), (π, pX), E at 630-746 MeV/c; calculated η production associated σ, σ(θ); deduced no quasibound state. Comparisons with data.
doi: 10.1103/PhysRevC.62.011002
1999GA14 Phys.Rev. C59, 2389 (1999) Pion-Induced η Production in the Deuteron NUCLEAR REACTIONS 2H(π-, 2nX), E=threshold-1500 MeV; calculated η production σ, σ(θ); deduced reaction mechanism features. Fully covariant formalism. Comparison with data.
doi: 10.1103/PhysRevC.59.2389
1999PE16 Phys.Rev. C60, 045201 (1999) M.T.Pena, D.O.Riska, A.Stadler Nucleon Resonance Effects in pp → ppπ0 Near Threshold NUCLEAR REACTIONS 1H(p, pπ0), E=280-320 MeV; calculated σ; deduced resonance contributions. Comparisons with data.
doi: 10.1103/PhysRevC.60.045201
1999RA21 Phys.Rev. C60, 047001 (1999) G.Ramalho, A.Arriaga, M.T.Pena Two-Pion Exchange and Strong Form Factors in Covariant Field Theories
doi: 10.1103/PhysRevC.60.047001
1998AD02 Nucl.Phys. A631, 570c (1998) J.Adam, Jr., A.Stadler, M.T.Pena, F.Gross Relativistic Dynamics in pp → ppπ0 Near Threshold NUCLEAR REACTIONS 1H(p, pπ0), E=280-300 MeV; calculated σ. Relativistic calculations. Comparison with data.
doi: 10.1016/S0375-9474(98)00069-4
1997AD14 Phys.Lett. 407B, 97 (1997) J.Adam, Jr., A.Stadler, M.T.Pena, F.Gross Effects of Relativistic Dynamics in pp → ppπ0 Near Threshold NUCLEAR REACTIONS 1H(p, p'X), E=280-300 MeV; analyzed total σ vs E; deduced NN-interaction related features. Several models compared.
doi: 10.1016/S0370-2693(97)00732-6
1996PE24 Phys.Rev. C54, 2235 (1996) Two-Pion-Exchange Potential and the πN Amplitude
doi: 10.1103/PhysRevC.54.2235
1995CO27 Phys.Rev. C52, 2925 (1995) Repulsive Short-Range Three-Nucleon Interaction
doi: 10.1103/PhysRevC.52.2925
1994VA03 Phys.Rev. C49, 1799 (1994) A.Valcarce, F.Fernandez, H.Garcilazo, M.T.Pena, P.U.Sauer Effects of a Quark-Model-Based Nucleon-Δ Potential on the Two-Nucleon System Above Pion Threshold NUCLEAR REACTIONS 1H(p, X), (p, π+), E=300-900 MeV; 2H(π+, π+), E ≤ 300 MeV; analyzed σ(E). 1H(p, π+), (polarized p, π+), E=578, 800 MeV; 2H(π+, π+), E=140, 256 MeV; analyzed σ(θ), polarization data. Nonrelativistic quark model, nucleon-Δ potential.
doi: 10.1103/PhysRevC.49.1799
1993CO14 Phys.Rev. C48, 2559 (1993) Momentum and Coordinate Space Three-Nucleon Potentials NUCLEAR STRUCTURE 3H; calculated three-body force contributions to binding energy. Potentials with ρ, π exchange, momentum, coordinate space.
doi: 10.1103/PhysRevC.48.2559
1992PE03 Phys.Rev. C45, 1487 (1992) M.T.Pena, H.Garcilazo, U.Oelfke, P.U.Sauer Effect of the NΔ Interaction on Observables of the πNN and γNN Systems NUCLEAR REACTIONS 1H(polarized p, π), E=578, 800 MeV; calculated analyzing power, iT11, other polarization observables vs θ. 2H(γ, π0), E=300 MeV; calculated σ(θ), asymmetry, polarization observables vs θ; deduced NΔ-interaction role.
doi: 10.1103/PhysRevC.45.1487
1990PE07 Phys.Rev. C42, 855 (1990) M.T.Pena, H.Henning, P.U.Sauer Effect of the Nucleon-Delta Interaction on Properties of the Three-Nucleon Ground State NUCLEAR STRUCTURE 3He; calculated charge monopole, magnetic dipole form factors; deduced nucleon-Δ interaction role.
doi: 10.1103/PhysRevC.42.855
1988FO07 Nucl.Phys. A487, 92 (1988) Faddeev-Born-Oppenheimer Equations for Molecular Three-Body Systems: Adiabatic calculation of 9Be NUCLEAR STRUCTURE 9Be; calculated levels. Molecular three-body system, Faddeev-Born-Oppenheimer equations.
doi: 10.1016/0375-9474(88)90131-5
1984CO18 Phys.Rev. C30, 1366 (1984) Three-Nucleon Forces and the Triton Binding Energy NUCLEAR STRUCTURE 3H; calculated binding energy. Faddeev equations, s-wave potentials, three-nucleon forces.
doi: 10.1103/PhysRevC.30.1366
Back to query form |