NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = O.Pisanti Found 7 matches. 2017GR16 Phys.Rev. C 96, 045807 (2017) A.Grassi, G.Mangano, L.E.Marcucci, O.Pisanti α + d → 6Li + γ astrophysical S factor and its implications for Big Bang nucleosynthesis NUCLEAR REACTIONS 2H(α, 6Li), E(cm)<7 MeV; calculated phase shifts for every partial wave, partial astrophysical S(E) factors, total astrophysical S(E) factors for five potential models. Comparison with available experimental data. NUCLEAR STRUCTURE 6Li; calculated binding energy, s-state ANC, magnetic dipole moment, electric quadrupole moment using five different potential models, and compared with available experimental data. 6Li; deduced effect of S-factor prediction on the primordial abundance of 6Li using the code PArthENoPE. Two-body framework for α+d radiative capture, with the α particle and the deuteron treated as structureless constituent of 6Li.
doi: 10.1103/PhysRevC.96.045807
2000ES02 Nucl.Phys. B568, 421 (2000) S.Esposito, G.Mangano, G.Miele, O.Pisanti Big Bang Nucleosynthesis: An accurate determination of light element yields
doi: 10.1016/S0550-3213(99)00725-7
2000ES05 Nucl.Phys. B(Proc.Supp.) S81, 59 (2000) S.Esposito, G.Mangano, G.Miele, O.Pisanti Primordial Nucleosynthesis: Accurate predictions
doi: 10.1016/S0920-5632(99)00859-2
1999ES02 Nucl.Phys. B540, 3 (1999) S.Esposito, G.Mangano, G.Miele, O.Pisanti Precision Rates for Nucleon Weak Interactions in Primordial Nucleosynthesis and 4He Abundance NUCLEAR REACTIONS 1n(ν, e), (e+, ν), 1H(e, ν), (ν, e+), E not given; calculated radiative corrections, thermal effects, weak interactions related features; deduced correction to primordial 4He mass fraction.
doi: 10.1016/S0550-3213(98)00757-3
1998BO25 Prog.Theor.Phys.(Kyoto) 99, 1017 (1998) C.Bourrely, F.Buccella, O.Pisanti, P.Santorelli, J.Soffer Polarized Quarks, Gluons and Sea in Nucleon Structure Functions NUCLEAR REACTIONS 1H(e, e'X), E not given; analyzed data; deduced structure function parameters, relative merits of spin crisis solutions.
doi: 10.1143/PTP.99.1017
1996BU28 Nuovo Cim. 109A, 159 (1996) F.Buccella, O.Pisanti, P.Santorelli, J.Soffer Does One Need the Anomaly to Describe the Polarized Structure Functions ( Question ) NUCLEAR STRUCTURE 1n, 2,1H; calculated polarized structure functions.
doi: 10.1007/BF02730943
1995AC03 Nuovo Cim. 108A, 375 (1995) F.Acampora, G.Amelino-Camelia, F.Buccella, O.Pisanti, L.Rosa, T.Tuzi Proton Decay and Neutrino Masses in SO(10)
doi: 10.1007/BF02787063
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