NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = P.Ricci Found 21 matches. 2016FA09 Nat.Phys. 12, 411 (2016) A.Fasoli, S.Brunner, W.A.Cooper, J.P.Graves, P.Ricci, O.Sauter, L.Villard Computational challenges in magnetic-confinement fusion physics
doi: 10.1038/nphys3744
2015BE08 Nucl.Phys. A937, 17 (2015) V.B.Belyaev, P.Ricci, F.Simkovic, J.Adam, Jr., M.Tater, E.Truhlik Consequence of total lepton number violation in strongly magnetized iron white dwarfs
doi: 10.1016/j.nuclphysa.2015.02.002
2010RI02 Nucl.Phys. A837, 110 (2010) P.Ricci, E.Truhlik, B.Mosconi, J.Smejkal Muon capture in deuterium
doi: 10.1016/j.nuclphysa.2010.02.009
2007MO14 Phys.Rev. C 75, 044610 (2007) B.Mosconi, P.Ricci, E.Truhlik, P.Vogel Model dependence of the neutrino-deuteron disintegration cross sections at low energies NUCLEAR REACTIONS 2H(ν, ν'n), (ν, ep), E=2-20 MeV; calculated σ, reaction rates, model dependence.
doi: 10.1103/PhysRevC.75.044610
2006MO14 Nucl.Phys. A722, 81 (2006) Weak axial nuclear heavy meson exchange currents and interactions of solar neutrinos with deuterons NUCLEAR REACTIONS 2H(ν, X), E=2-20 MeV; calculated weak axial meson exchange currents, σ. Comparison of several models.
doi: 10.1016/j.nuclphysa.2006.03.011
2006MO28 Eur.Phys.J. A 27, Supplement 1, 67 (2006) Interactions of the solar neutrinos with the deuterons NUCLEAR REACTIONS 2H(ν, ν'n), (ν, e-p), (ν, e+n), E=2-20 MeV; calculated σ.
doi: 10.1140/epja/i2006-08-009-6
2005MO26 Eur.Phys.J. A 25, 283 (2005) The role of the pion pair term in the theory of the weak axial meson exchange currents
doi: 10.1140/epja/i2005-10111-6
1999MO11 Phys.Rev. C59, 2844 (1999) Parity Violating Target Asymmetry in Electron-Proton Scattering NUCLEAR REACTIONS 1H(polarized e, e), E not given; calculated σ(θ), analyzing power, parity violating target asymmetry; deduced sensitivity to weak form factors.
doi: 10.1103/PhysRevC.59.2844
1997MO14 Phys.Rev. C55, 3115 (1997) Deuteron Electroweak Disintegration NUCLEAR REACTIONS 2H(polarized e, e'p), (polarized e, e'n), E not given; calculated proton asymmetry vs θ, nucleon asymmetry associated parameters; deduced nucleon weak form factors related features. Coplanar geometry, electrodisintegration.
doi: 10.1103/PhysRevC.55.3115
1993MO08 Phys.Rev. C48, 332 (1993) B.Mosconi, J.Pauschenwein, P.Ricci Nucleon Polarization in Deuteron Electrodisintegration NUCLEAR REACTIONS 2H(polarized e, X), E not given; calculated vector, tensor target polarization transfer, tensor target-beam polarization transfer following target breakup; deduced neutron charge form factor role. Standard theory.
doi: 10.1103/PhysRevC.48.332
1990MO24 Nucl.Phys. A517, 483 (1990) Relativistic Corrections in Deuteron Electrodisintegration at the Quasi-Elastic Peak NUCLEAR REACTIONS 2H(polarized e, e'p), E not given; calculated longitudinal, longitudinal-transverse structure function. Relativistic corrections.
doi: 10.1016/0375-9474(90)90213-6
1990SC04 Phys.Rev. C41, 841 (1990) K.-M.Schmitt, P.Wilhelm, H.Arenhovel, A.Cambi, B.Mosconi, P.Ricci Gauge Dependence of Nonrelativistic Calculations of Deuteron Photodisintegration NUCLEAR REACTIONS 2H(γ, p), (γ, n), E=30-140 MeV; calculated photodisintegration σ(θ); deduced gauge dependence. Nonrelativistic model.
doi: 10.1103/PhysRevC.41.841
1989MO11 Few-Body Systems 6, 63 (1989); Erratum Few-Body Systems 8, 159 (1990) Deuteron A(q2) Structure Function in the Low and Medium q2 Range NUCLEAR STRUCTURE 2H; calculated structure function. Paris potential, relativistic corrections.
doi: 10.1007/BF01080551
1988MO34 Phys.Rev. C38, 2976 (1988) Reply to ' Comment on 'Center-of-Mass Motion and Siegert's Theorem' ' NUCLEAR STRUCTURE 2H; calculated breakup multipole reduced matrix elements.
doi: 10.1103/PhysRevC.38.2976
1987MO10 Phys.Rev. C36, 60 (1987) Center-of-Mass Motion and Siegert's Theorem NUCLEAR REACTIONS 2H(γ, n), E ≈ 0-120 MeV; calculated photodisintegration σ(E). Siegert's theorem, center-of-mass motion.
doi: 10.1103/PhysRevC.36.60
1986CA06 Czech.J.Phys. B36, 309 (1986) Relativistic Effects in Deuteron Electrodisintegration NUCLEAR REACTIONS 2H(e, e'p), E ≈ 500 MeV; calculated σ(E(e'), θ(e'), θp); deduced nucleonic, pionic relativistic corrections.
doi: 10.1007/BF01597165
1985CA24 J.Phys.(London) G11, 897 (1985) Relativistic Effects in Deuteron Photoabsorption Sum Rules NUCLEAR REACTIONS 2H(γ, X), E=0-140 MeV; calculated photoabsorption sum rule σ, E1 bremsstrahlung weighted σ; deduced relativistic effects role.
doi: 10.1088/0305-4616/11/8/007
1984CA01 J.Phys.(London) G10, L11 (1984) Relativistic Effects in the Forward Deuteron Photodisintegration Cross Section NUCLEAR REACTIONS 2H(γ, p), E=5-120 MeV; calculated σ(θ=0°); deduced one-, two-body relativistic effect coherent effect.
doi: 10.1088/0305-4616/10/1/008
1982CA02 Phys.Rev.Lett. 48, 462 (1982) Relativistic and Mesonic Corrections to the Forward Cross Section for d(γ, p)n NUCLEAR REACTIONS 2H(γ, p), E=5-130 MeV; calculated σ(θ=0°, E); deduced relativistic corrections. Soft-core potentials, Darwin-Foldy, spin-orbit terms, one-body charge density.
doi: 10.1103/PhysRevLett.48.462
1981CA04 Nucl.Phys. A356, 469 (1981) Two-Body Modifications of the Siegert Dipole Operator and Doubly Radiative n - p Capture NUCLEAR REACTIONS 1H(n, γ), E=thermal; calculated σ(two-photon). Siegert dipole operator, one pion exchange effects.
doi: 10.1016/0375-9474(81)90201-3
1980CA10 Phys.Rev. C21, 1921 (1980) Consistency between Pion Exchange Currents and N-N Potential in Double Radiative n-p Capture NUCLEAR REACTIONS 1H(n, γ), E=thermal; calculated two-photon production σ. Reid soft-core potential, meson exchange currents.
doi: 10.1103/PhysRevC.21.1921
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