NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.Viviani Found 143 matches. Showing 1 to 100. [Next]2024CO01 Phys.Rev. C 109, 014301 (2024) L.Coraggio, N.Itaco, G.De Gregorio, A.Gargano, Z.H.Cheng, Y.Z.Ma, F.R.Xu, M.Viviani The renormalization of the shell-model Gamow-Teller operator starting from effective field theory for nuclear systems
doi: 10.1103/PhysRevC.109.014301
2024GN01 Phys.Rev. C 109, 035502 (2024) A.Gnech, L.E.Marcucci, M.Viviani Bayesian analysis of muon capture on the deuteron in chiral effective field theory
doi: 10.1103/PhysRevC.109.035502
2024KI04 Phys.Rev. C 109, 034006 (2024) A.Kievsky, E.Garrido, M.Viviani, L.E.Marcucci, L.Serksnyte, R.Del Grande nnn and ppp correlation functions
doi: 10.1103/PhysRevC.109.034006
2024KI06 Few-Body Systems 65, 23 (2024) A.Kievsky, E.Garrido, M.Viviani, M.Gattobigio The ppp Correlation Function with a Screened Coulomb Potential
doi: 10.1007/s00601-024-01893-6
2023GI08 Phys.Rev. C 107, L061001 (2023) L.Girlanda, E.Filandri, A.Kievsky, L.E.Marcucci, M.Viviani Effect of the N3LO three-nucleon contact interaction on p-d scattering observables NUCLEAR REACTIONS 1H(d, d), 2H(p, p), E(cm)=2 MeV; calculated proton and deuteron analyzing power, tensor observables, σ(θ). Chiral effective field theory with AV18 2N potential. Expression of short-range component in terms of five combinations of low-energy constants (LECs) parameterizing the N3LO 2N contact Lagrangian. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.L061001
2023TU05 Commun. Phys. 6, 106 (2023) A.Tumino, G.G.Rapisarda, M.La Cognata, A.Oliva, A.Kievsky, C.A.Bertulani, G.D'Agata, M.Gattobigio, G.L.Guardo, L.Lamia, D.Lattuada, R.G.Pizzone, S.Romano, M.L.Sergi, R.Sparta, M.Viviani Coulomb-free 1So p - p scattering length from the quasi-freep p + d → p + p + n reaction and its relation to universality NUCLEAR REACTIONS 2H(p, 2p), E(cm)<1 MeV; analyzed available data; deduced p-p scattering σ, σ(θ), scattering length and effective range from a Bayesian approach analysis.
doi: 10.1038/s42005-023-01221-0
2023VI02 Phys.Rev.Lett. 130, 122501 (2023) M.Viviani, L.Girlanda, A.Kievsky, D.Logoteta, L.E.Marcucci Theoretical Study of the d(d, p)3H and d(d, n)3H Processes at Low Energies NUCLEAR REACTIONS 2H(d, p), (d, n), E(cm)<1 MeV; analyzed available data; deduced astrophysical S factor, the quintet suppression factor, single and double polarized observables, first estimate of the theoretical uncertainty for all these quantities.
doi: 10.1103/PhysRevLett.130.122501
2023VI05 Phys.Rev. C 108, 064002 (2023) M.Viviani, S.Konig, A.Kievsky, L.E.Marcucci, B.Singh, O.Vazquez Doce Role of three-body dynamics in nucleon-deuteron correlation functions
doi: 10.1103/PhysRevC.108.064002
2022GU20 Phys.Rev.Lett. 129, 242503 (2022) V.Guzey, M.Rinaldi, S.Scopetta, M.Strikman, M.Viviani Coherent J/γ Electroproduction on 4He and 3He at the Electron-Ion Collider: Probing Nuclear Shadowing One Nucleon at a Time
doi: 10.1103/PhysRevLett.129.242503
2022VI01 Phys.Rev. C 105, 014001 (2022) M.Viviani, E.Filandri, L.Girlanda, C.Gustavino, A.Kievsky, L.E.Marcucci, R.Schiavilla X17 boson and the3H(p, e+e-)4He and 3He(n, e+e-4He processes: A theoretical analysis NUCLEAR REACTIONS 3H(p, γ)4He, E(cm)<0.85 MeV; 3He(n, γ)4He, E(cm)<2 MeV; calculated astrophysical S factor, total σ(E) using Δ-less (N3LO500/N2LO500) and Δ-full (NVIa/3NIa) χEFT formalism, and compared with experimental data. 3H(p, e-e+)4He, E=0.90 MeV; calculated five-fold differential σ(E, θ) as function of the electron energy using N3LO500/N2LO500 interactions in the ATOMKI setup. 3H(p, e-e+)4He, E=0.40, 0.90 MeV; 3He(n, e-e+)4He, E=0.17, 0.35, 0.70, 2.0 MeV; calculated four-fold differential σ(E, θ) based on the N3LO500/N2LO500 interactions, including results obtained from the exchange of a scalar, pseudoscalar, vector, and axial X17 boson, and compared with differential σ data for 3H(p, e-e+)4He, E=0.51, 0.61.0.90 MeV reaction from ATOMKI (reported by 2021Kr08: Phys. Rev. C 104, 044003). 3H(p, p)(p, p'), E=0.9 MeV; calculated reduced matrix elements (RMEs) for channels with J≤2, dependences on the three-momentum transfer and proton incident energy of electromagnetic RMEs using N3LO500/N2LO500 or NVIa/3NIa chiral interactions. 3He(n, e-e+)4He, 3He(n, γ)4He, E=0.17, 0.35, 0.70, 1.00, 2.00, 3.50 MeV; calculated total σ(E) using the N3LO500/N2LO500 and NVIa/3NIa Hamiltonians; deduced X17 coupling constants from the fit of the 2019 ATOMKI angular distribution data for 3H(p, e+e-)4He, E=0.90 MeV. Relevance to possible future experiments probing e+ - e- pair production in a four-nucleon system such as 4He at a number of candidate facilities.
doi: 10.1103/PhysRevC.105.014001
2021GN01 Phys.Rev. C 104, 035501 (2021) A.Gnech, L.E.Marcucci, R.Schiavilla, M.Viviani Comparative study of 6He β-decay based on different similarity-renormalization-group evolved chiral interactions RADIOACTIVITY 3H, 6He(β-); calculated Gamow-Teller reduced matrix element (RMEs) using the similarity renormalization group (SRG) versions of momentum- and configuration-space two-nucleon interactions N2LO450 and NV2-Ia deduced from chiral effective field theory (χEFT), with and without the explicit inclusion of Δ isobars, contributions of two-body currents such as N3LO(OPE), transition densities; deduced that N3LO(OPE) contribution is opposite in sign for the SRG-evolved N2LO450 and NV2-Ia interactions. NUCLEAR STRUCTURE 6He, 6Li; calculated binding energies using the similarity renormalization group (SRG) versions of momentum- and configuration-space
doi: 10.1103/PhysRevC.104.035501
2021HI04 Phys.Rev. C 103, 024004 (2021) M.D.Higgins, C.H.Greene, A.Kievsky, M.Viviani Comprehensive study of the three- and four-neutron systems at low energies NUCLEAR STRUCTURE 3,4n; calculated adiabatic hyperspherical potential curves for Jπ=3/2- for the 3n system and Jπ=0+ for the 4n system, phase shifts and eigenshifts using explicitly correlated Gaussian (CGHS) and the hyperspherical harmonic (HH) bases, multichannel analysis of the three-and four-neutron scattering near the scattering continuum threshold; deduced no evidence of a 4n-resonance at low energy. Discussed experimental result of possible 4n resonance by 2016Ki01 in 4He(8He, 4n8Be) reaction.
doi: 10.1103/PhysRevC.103.024004
2021SC12 Phys.Rev. C 103, 054003 (2021) R.Schiavilla, L.Girlanda, A.Gnech, A.Kievsky, A.Lovato, L.E.Marcucci, M.Piarulli, M.Viviani Two- and three-nucleon contact interactions and ground-state energies of light- and medium-mass nuclei NUCLEAR STRUCTURE 3H, 3,4,6He, 6Li, 16O, 40,48Ca, 90Zr; calculated binding energies in the EFT formalism with the construction of 2N contact local interactions at LO, NLO, and N3LO in configuration space, with deuteron properties determined from analysis of np and pp scattering data. Comparison with experimental data. NUCLEAR REACTIONS 1H(n, n), (p, p), E=1-25 MeV; analyzed experimental scattering data; deduced scattering lengths, effective radii and phase shifts, deuteron S-wave radial functions at LO and deuteron S- and D-wave radial functions in the EFT formalism.
doi: 10.1103/PhysRevC.103.054003
2020DE41 Phys.Rev. C 102, 064001 (2020) A.Deltuva, M.Gattobigio, A.Kievsky, M.Viviani Gaussian characterization of the unitary window for N = 3: bound, scattering, and virtual states
doi: 10.1103/PhysRevC.102.064001
2020FU07 Phys.Rev. C 102, 065205 (2020) S.Fucini, S.Scopetta, M.Viviani Incoherent deeply virtual Compton scattering off 4He NUCLEAR REACTIONS 4He(e-, e-'p'γ), Q2<5 GeV2; calculated cross sections for the electromagnetic Bethe-Heitler (BH), and nuclear deeply virtual incoherent Compton scattering (DVCS) processes on the free proton and on a proton bound in 4He, beam-spin asymmetry (BSA) as function of azimuthal angle, azimuthal beam-spin asymmetry for the proton in 4He. Calculations based on impulse approximation (IA) analysis, based on state-of-the-art models for the proton and nuclear structure. Comparison with experimental data from CLAS collaboration at the Jefferson Laboratory.
doi: 10.1103/PhysRevC.102.065205
2020GI08 Phys.Rev. C 102, 064003 (2020) L.Girlanda, A.Kievsky, L.E.Marcucci, M.Viviani Unitary ambiguity of NN contact interactions and the 3N force
doi: 10.1103/PhysRevC.102.064003
2020GN01 Phys.Rev. C 101, 024004 (2020) Time-reversal violation in light nuclei NUCLEAR STRUCTURE 2,3H, 3He; calculated electric dipole moments (EDM) by deriving the time-reversal violation (TRV) nucleon-nucleon (NN) and three-nucleon (NNN) potential up to next-to-next leading order (N2LO) in a chiral effective field theory (χEFT) framework. Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.101.024004
2020GN02 Phys.Rev. C 102, 014001 (2020) A.Gnech, M.Viviani, L.E.Marcucci Calculation of the 6Li ground state within the hyperspherical harmonic basis NUCLEAR STRUCTURE 6Li; calculated ground state binding energy, charge radius, magnetic dipole moment, electric quadrupole moment, asymptotic normalization coefficients (ANCs), matrix elements relevant for direct dark matter search, mean values of the proton and neutron spin operators using the hyperspherical harmonic (HH) approach with two-body nuclear forces. Comparison with other theoretical predictions.
doi: 10.1103/PhysRevC.102.014001
2020HI09 Phys.Rev.Lett. 125, 052501 (2020) M.D.Higgins, C.H.Greene, A.Kievsky, M.Viviani Nonresonant Density of States Enhancement at Low Energies for Three or Four Neutrons NUCLEAR STRUCTURE 3,4NN; calculated hyperspherical potential curves, rescaled Wigner-Smith time delays, low energy enhancement of the density of states.
doi: 10.1103/PhysRevLett.125.052501
2020VI07 Phys.Rev. C 102, 034007 (2020) M.Viviani, L.Girlanda, A.Kievsky, L.E.Marcucci n + 3H, p + 3He, p + 3H and n + 3He scattering with the hyperspherical harmonic method NUCLEAR REACTIONS 3H(n, X), E<10 MeV; calculated total σ(E). 3He(p, p), E=2-6 MeV; calculated phase shifts. 3He(p, p), (polarized p, p), E=2.25, 4.05, 5.54 MeV; calculated differential σ(θ, E), analyzing powers Ay(θ, E), spin polarization coefficients. 3H(p, p), (p, n), E(cm)<3.5 MeV; calculated phase shifts as function of the center-of-mass kinetic energy, energies and widths of resonances. 3H(p, p), (polarized p, p), E=0.4, 0.6, 1.16, 2.0, 3.0, 4.17 MeV; 3H(n, n), (polarized n, n), E=1, 2, 3.5 MeV; 3H(p, n), (polarized p, n), E=2.5, 3.5, 4.15 MeV; calculated differential σ(θ, E), analyzing powers, and relevant model parameters. Hyperspherical harmonic (HH) method with nuclear Hamiltonians of two- and three-nucleon NN N3LO and 3N N2LO interactions. Comparison with experimental data. Application of HH method to the 4N scattering problem.
doi: 10.1103/PhysRevC.102.034007
2019GA25 Phys.Rev. C 100, 034004 (2019) M.Gattobigio, A.Kievsky, M.Viviani Embedding nuclear physics inside the unitary-limit window NUCLEAR STRUCTURE 6He, 6Li, 3H, 3,4He; calculated energies of ground- and excited states, Efimov plot for N=2, 3, 4 and 6 particles, s-wave scattering lengths, spectra of A=2, 3, 4, and 6 nuclei in the region between the unitary limit and the point where the scattering lengths get their physical values.Gaussian potential model with variable strength.
doi: 10.1103/PhysRevC.100.034004
2019GI08 Phys.Rev. C 99, 054003 (2019) L.Girlanda, A.Kievsky, M.Viviani, L.E.Marcucci Short-range three-nucleon interaction from A = 3 data and its hierarchical structure NUCLEAR REACTIONS 2H(p, p), E=0.647, 1.0, 2.0, 2.5, 3.0 MeV; analyzed experimental data for differential σ(θ, E), Ay(θ, E), iT11(θ, E), T20(θ, E) and T21(θ, E) polarization observables using a hybrid phenomenological approach; deduced accurate models of the three-nucleon (3N) interaction by fitting the low-energy constants (LECs) to the triton binding energy, n-d scattering lengths, cross sections, and polarization observables of p-d scattering.
doi: 10.1103/PhysRevC.99.054003
2019MA22 Phys.Rev. C 99, 034003 (2019) L.E.Marcucci, F.Sammarruca, M.Viviani, R.Machleidt Momentum distributions and short-range correlations in the deuteron and 3He with modern chiral potentials NUCLEAR STRUCTURE 2H, 3He; calculated single neutron and proton, neutron-proton, and proton-proton momentum distributions, short-range correlation probabilities using two-nucleon (2N) and 2N+3N chiral potentials (LO, NLO, N2LO, N3LO, N4LO) with and without leading chiral three-nucleon force; deduced model dependence of one- and two-body momentum distributions and the impact of three body forces. Comparison with previous theoretical predictions.
doi: 10.1103/PhysRevC.99.034003
2019SC07 Phys.Rev. C 99, 034005 (2019) R.Schiavilla, A.Baroni, S.Pastore, M.Piarulli, L.Girlanda, A.Kievsky, A.Lovato, L.E.Marcucci, StevenC.Pieper, M.Viviani, R.B.Wiringa Local chiral interactions and magnetic structure of few-nucleon systems NUCLEAR STRUCTURE 2,3H, 3He; calculated magnetic form factors, and contributions to the isoscalar and isovector combinations of the trinucleon magnetic moments using chiral interactions. Comparison with experimental data. NUCLEAR REACTIONS 2H(γ, n), E=2-29 MeV; 2H(e, n), E=0-3 MeV; calculated deuteron photodisintegration cross sections, deuteron threshold electrodisintegration cross sections at backward angles using chiral two-, and three-nucleon interactions including Δ intermediate states for LO, NLO, N2LO, and N3LO models. Comparison with experimental data.
doi: 10.1103/PhysRevC.99.034005
2018BA37 Phys.Rev. C 98, 044003 (2018) A.Baroni, R.Schiavilla, L.E.Marcucci, L.Girlanda, A.Kievsky, A.Lovato, S.Pastore, M.Piarulli, S.Pieper, M.Viviani, R.B.Wiringa Local chiral interactions, the tritium Gamow-Teller matrix element, and the three-nucleon contact term RADIOACTIVITY 3H(β-); calculated Gamow-Teller matrix element, and low energy constants in the contact three-nucleon interaction within the chiral two- and three nucleon interactions including Δ intermediate states, contributions due to loop corrections in the axial current at next-to-next-to-next-to-next-to-leading order (N4LO). Comparison with experimental values.
doi: 10.1103/PhysRevC.98.044003
2018FU12 Phys.Rev. C 98, 015203 (2018) S.Fucini, S.Scopetta, M.Viviani Coherent deeply virtual Compton scattering off 4He NUCLEAR REACTIONS 4He(e, e'γ), Q2=1-2.5 GeV2; calculated generalized parton distribution, azimuthal beam-spin asymmetry, real and imaginary parts of the Compton form factors of coherent deeply virtual Compton scattering using impulse approximation with Argonne 18 nucleon-nucleon interaction; derived convolution formula for the nuclear generalized parton distribution (GPD). Comparison with experimental data from EG6 experiment at Jefferson Laboratory (Jlab).
doi: 10.1103/PhysRevC.98.015203
2018KI09 Phys.Rev.Lett. 121, 072701 (2018) A.Kievsky, M.Viviani, D.Logoteta, I.Bombaci, L.Girlanda Correlations imposed by the unitary limit between few-nucleon systems, nuclear matter, and neutron stars
doi: 10.1103/PhysRevLett.121.072701
2018PI01 Phys.Rev.Lett. 120, 052503 (2018) M.Piarulli, A.Baroni, L.Girlanda, A.Kievsky, A.Lovato, E.Lusk, L.E.Marcucci, S.C.Pieper, R.Schiavilla, M.Viviani, R.B.Wiringa Light-Nuclei Spectra from Chiral Dynamics
doi: 10.1103/PhysRevLett.120.052503
2018VI01 Few-Body Systems 59, 73 (2018) M.Viviani, L.Girlanda, A.Kievsky, L.E.Marcucci, J.Dohet-Eraly Three-nucleon force effects in A=4 scattering NUCLEAR REACTIONS 3H(p, X)4He, E<3 MeV; calculated phase shift, σ(θ). Comparison with available data.
doi: 10.1007/s00601-018-1379-6
2017KI01 Phys.Rev. C 95, 024001 (2017) A.Kievsky, M.Viviani, M.Gattobigio, L.Girlanda Implications of Efimov physics for the description of three and four nucleons in chiral effective field theory NUCLEAR STRUCTURE 3H, 4He; calculated binding energies as function of regulator β for different values of the potential range, and compared with results form SU(4) symmetry. Chiral effective field theory with the leading order (LO) nucleon-nucleon potential, and the one-pion-exchange potential (OPEP).
doi: 10.1103/PhysRevC.95.024001
2017VI03 Phys.Rev. C 95, 034003 (2017) M.Viviani, A.Deltuva, R.Lazauskas, A.C.Fonseca, A.Kievsky, L.E.Marcucci Benchmark calculation of p - 3H and n-3He scattering NUCLEAR REACTIONS 3H(polarized n, n), E=1.0, 2.0, 3.5 MeV; 3H(polarized p, p), 3H(polarized p, n)3He, E=2.5, 3.5, 4.15 MeV; calculated differential σ(E), neutron, proton and 3He analyzing powers, spin-correlation coefficient using N3LO500 potential. Calculations used three techniques for elastic and charge-exchange processes: Alt, Grassberger, Sandhas (AGS), hyperspherical harmonics (HH), and Faddeev-Yakubovsky (FY). Comparison with experimental data.
doi: 10.1103/PhysRevC.95.034003
2017VI04 Few-Body Systems 58, 110 (2017) M.Viviani, L.Girlanda, A.Kievsky, L.E.Marcucci Three-Nucleon Force Effects in p-3H and n-3He Scattering NUCLEAR REACTIONS 3H(p, p), 3He(n, n), E<5 MeV; analyzed available data; calculated σ(θ) using N3LO500 model.
doi: 10.1007/s00601-017-1264-8
2016BA06 Phys.Rev. C 93, 015501 (2016); Erratum Phys.Rev. C 95, 059901 (2017) A.Baroni, L.Girlanda, S.Pastore, R.Schiavilla, M.Viviani Nuclear axial currents in chiral effective field theory
doi: 10.1103/PhysRevC.93.015501
2016BA40 Phys.Rev. C 94, 024003 (2016); Erratum Phys.Rev. C 95, 059902 (2017) A.Baroni, L.Girlanda, A.Kievsky, L.E.Marcucci, R.Schiavilla, M.Viviani Tritium β decay in chiral effective field theory RADIOACTIVITY 3H(β-); calculated Fermi and Gamow-Teller (GT) matrix elements by including in the charge-changing weak current corrections up to one in nuclear chiral effective field theory (χEFT), low-energy constants (LECs), one pion exchange (OPE) contributions.
doi: 10.1103/PhysRevC.94.024003
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
2016MA14 Phys.Rev.Lett. 116, 102501 (2016) L.E.Marcucci, G.Mangano, A.Kievsky, M.Viviani Implication of the Proton-Deuteron Radiative Capture for Big Bang Nucleosynthesis NUCLEAR REACTIONS 2H(p, γ), E<1 MeV; calculated S-factor using ab initio approach. Comparison with available data.
doi: 10.1103/PhysRevLett.116.102501
2016PI15 Phys.Rev. C 94, 054007 (2016) M.Piarulli, L.Girlanda, R.Schiavilla, A.Kievsky, A.Lovato, L.E.Marcucci, StevenC.Pieper, M.Viviani, R.B.Wiringa Local chiral potentials with Δ-intermediate states and the structure of light nuclei NUCLEAR STRUCTURE 3H, 3,4,6He, 6Li; calculated ground- and excited-state energies, and proton rms radii using nonlocal nucleon-nucleon potentials in hyperspherical harmonics (HH), variational Monte Carlo (VMC), Green's function Monte Carlo (GFMC) approaches. NUCLEAR REACTIONS 1H(p, p), (n, n), E=0-125, 0-200 MeV; analyzed Granada-2013 database of pp and np observables order by order in the chiral expansion up to N3LO and fitted to the deuteron binding energy and nn singlet scattering length; deduced nucleon-nucleon potentials, long-range included one- and two-pion exchange contributions without and with Δ isobars in the intermediate states up to order Q3 in the chiral expansion, while the short range consisted of contact interactions up to order Q4.
doi: 10.1103/PhysRevC.94.054007
2014GA15 Phys.Rev. C 90, 014607 (2014) E.Garrido, A.Kievsky, M.Viviani Breakup of three particles within the adiabatic expansion method
doi: 10.1103/PhysRevC.90.014607
2014SA57 Few-Body Systems 55, 693 (2014) G.Salme, T.Frederico, M.Viviani Solutions of the Bethe-Salpeter Equation in Minkowski Space: A Comparative Study
doi: 10.1007/s00601-014-0838-y
2014VI02 Phys.Rev. C 89, 064004 (2014) M.Viviani, A.Baroni, L.Girlanda, A.Kievsky, L.E.Marcucci, R.Schiavilla Chiral effective field theory analysis of hadronic parity violation in few-nucleon systems NUCLEAR REACTIONS 1H(polarized p, X), 1,2H(polarized n, X), 3He(polarized n, p)3H; analyzed parity-violating (PV) nucleon-nucleon potential up to next-to-next-to-leading (N2LO) order within a chiral effective field theory (χEFT) framework. Predictions for other PV observables. Discussed relevant ongoing and planned experiments at SNS facility of Oak Ridge National Laboratory.
doi: 10.1103/PhysRevC.89.064004
2013MA37 Phys.Rev.Lett. 110, 192503 (2013) L.E.Marcucci, R.Schiavilla, M.Viviani Proton-Proton Weak Capture in Chiral Effective Field Theory
doi: 10.1103/PhysRevLett.110.192503
2013PI01 Phys.Rev. C 87, 014006 (2013) M.Piarulli, L.Girlanda, L.E.Marcucci, S.Pastore, R.Schiavilla, M.Viviani Electromagnetic structure of A=2 and 3 nuclei in chiral effective field theory NUCLEAR STRUCTURE 2H, 3H, 3He; calculated structure function, tensor polarization, charge, isoscalar and isovector magnetic and quadrupole form factors, low-energy constants (LEC). Chiral-effective-field-theory. Chiral or conventional two- and three-nucleon potentials and Monte Carlo methods.
doi: 10.1103/PhysRevC.87.014006
2013VI05 Phys.Rev.Lett. 111, 172302 (2013) M.Viviani, L.Girlanda, A.Kievsky, L.E.Marcucci Effect of Three-Nucleon Interactions in p-3He Elastic Scattering NUCLEAR REACTIONS 3He(p, p), E<6 MeV; calculated σ(θ), polarization. Three-nucleon interaction, comparison with experimental data.
doi: 10.1103/PhysRevLett.111.172302
2012KI02 Phys.Rev. C 85, 014001 (2012) A.Kievsky, M.Viviani, L.E.Marcucci Theoretical description of three- and four-nucleon scattering states using bound-state-like wave functions NUCLEAR REACTIONS 2H(n, n'), E=1, 2, 3 MeV; 3He(p, p'), E=3.13, 4.05, 5.54 MeV; calculated scattering matrix eigenvalues, state occupation probabilities, phase shifts, mixing parameters. Coupled-channel form of the integral relations derived from the Kohn variational principle. Comparison with other theoretical calculations.
doi: 10.1103/PhysRevC.85.014001
2012MA01 Phys.Rev.Lett. 108, 052502 (2012) L.E.Marcucci, A.Kievsky, S.Rosati, R.Schiavilla, M.Viviani Chiral Effective Field Theory Predictions for Muon Capture on Deuteron and 3He NUCLEAR REACTIONS 2H, 3He(μ-, ν), E not given; calculated muon capture rates; deduced a value of induced pseudoscalar form factor. Comparison with measurements and chiral perturbation theory.
doi: 10.1103/PhysRevLett.108.052502
2011GA05 Phys.Rev. C 83, 024001 (2011) M.Gattobigio, A.Kievsky, M.Viviani Nonsymmetrized hyperspherical harmonic basis for an A-body system
doi: 10.1103/PhysRevC.83.024001
2011GI01 Few-Body Systems 49, 51 (2011) Relativistic Covariance of the 2-Nucleon Contact Interactions
doi: 10.1007/s00601-010-0185-6
2011GI04 Phys.Rev. C 84, 014001 (2011); Erratum Phys.Rev. C 102, 019903 (2020) L.Girlanda, A.Kievsky, M.Viviani Subleading contributions to the three-nucleon contact interaction
doi: 10.1103/PhysRevC.84.014001
2011MA05 Phys.Rev. C 83, 014002 (2011) L.E.Marcucci, M.Piarulli, M.Viviani, L.Girlanda, A.Kievsky, S.Rosati, R.Schiavilla Muon capture on deuteron and 3He NUCLEAR REACTIONS 2H(μ-, ν)2n, 3He(μ-, ν)3H; calculated binding energies of deuteron, triton and 3H, scattering lengths, magnetic moments, total and differential rates for muon capture using chiral effective field theory (EFT) with the two- and three-nucleon potentials AV18/UIX and N3LO/N2LO. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.014002
2011PA22 Phys.Rev. C 84, 024001 (2011) S.Pastore, L.Girlanda, R.Schiavilla, M.Viviani Two-nucleon electromagnetic charge operator in chiral effective field theory (χEFT) up to one loop
doi: 10.1103/PhysRevC.84.024001
2011RO58 J.Phys.:Conf.Ser. 312, 082036 (2011) C.Romero-Redondo, E.Garrido, A.Kievsky, P.Barletta, M.Viviani Multichannel reactions using the adiabatic expansion method
doi: 10.1088/1742-6596/312/4/082036
2011TO06 Phys.Lett. B 702, 121 (2011) W.Tornow, H.J.Karwowski, J.H.Kelley, R.Raut, G.Rusev, S.C.Stave, A.P.Tonchev, A.Deltuva, A.C.Fonseca, L.E.Marcucci, M.Viviani, A.Kievsky, J.Golak, R.Skibinski, H.Witala, R.Schiavilla Two-body photodisintegration of 3He between 7 and 16 MeV NUCLEAR REACTIONS 3He(γ, p), E=7-16 MeV; measured reaction products, Ep, Ip; deduced σ. Comparison with theoretical calculations and experimental data.
doi: 10.1016/j.physletb.2011.06.080
2011VI06 Phys.Rev. C 84, 054010 (2011) M.Viviani, A.Deltuva, R.Lazauskas, J.Carbonell, A.C.Fonseca, A.Kievsky, L.E.Marcucci, S.Rosati Benchmark calculation of n-3H and p-3He scattering NUCLEAR REACTIONS 3He(p, p), E=2.25, 4.05, 5.54 MeV; 3H(n, n), E=1.0, 2.0, 3.5, 6.0 MeV; analyzed phase shifts, mixing parameters, total cross sections, differential σ(θ), neutron and triton analyzing powers using AGS, HS, and FY methods with I-N3LO, Argonne v18, CD Bonn interactions for four-nucleon problem.
doi: 10.1103/PhysRevC.84.054010
2010GI01 Phys.Rev. C 81, 034005 (2010) L.Girlanda, S.Pastore, R.Schiavilla, M.Viviani Relativity constraints on the two-nucleon contact interaction
doi: 10.1103/PhysRevC.81.034005
2010GI10 Phys.Rev.Lett. 105, 232502 (2010) L.Girlanda, A.Kievsky, L.E.Marcucci, S.Pastore, R.Schiavilla, M.Viviani Thermal Neutron Captures on d and 3He NUCLEAR REACTIONS 2H, 3He(n, γ), E=thermal; calculated wave functions, σ. Comparison with experimental data.
doi: 10.1103/PhysRevLett.105.232502
2010KI04 Phys.Rev. C 81, 034002 (2010) A.Kievsky, M.Viviani, P.Barletta, C.Romero-Redondo, E.Garrido Variational description of continuum states in terms of integral relations NUCLEAR STRUCTURE 3H, 3He; calculated n-d, p-d doublet and quartet scattering lengths, convergence of bound states as a function of the number of Laguerre polynomials and effective range functions in the formalism of Kohn Variational Principle (KVP).
doi: 10.1103/PhysRevC.81.034002
2010KI05 Phys.Rev. C 81, 044003 (2010) A.Kievsky, M.Viviani, L.Girlanda, L.E.Marcucci Comparative study of three-nucleon force models in A=3, 4 systems NUCLEAR STRUCTURE 3H, 4He; calculated binding energies, n-d doublet scattering length, and triton kinetic energy using AV18+TM', AV18+URIX, and AV18+N2LOL potentials. Three nucleon-force models. NUCLEAR REACTIONS 2H(polarized p, p), E=3 MeV; calculated σ(θ), A(y)(θ), iT11(θ), T20(θ), T21(θ), and T22(θ) using the AV18+TM', AV18+URIX, and AV18+N2LOL models. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.044003
2010RO25 Nucl.Phys. A834, 799c (2010) C.Romero-Redondo, E.Garrido, P.Barletta, A.Kievsky, M.Viviani Accurate calculation of phase shifts for three-body reactions with the adiabatic expansion method
doi: 10.1016/j.nuclphysa.2010.01.150
2010VI06 Phys.Rev. C 82, 044001 (2010) M.Viviani, R.Schiavilla, L.Girlanda, A.Kievsky, L.E.Marcucci Parity-violating asymmetry in the 3He(n(pol), p)3H reaction NUCLEAR REACTIONS 3He(polarized n, p)3H, E AP 0; calculated parity-violating R-and T-matrix elements using the meson-exchange DDH or pionless effective-field-theory (EFT) model for the weak-interaction potential.
doi: 10.1103/PhysRevC.82.044001
2009MA53 Phys.Rev. C 80, 034003 (2009) L.E.Marcucci, A.Kievsky, L.Girlanda, S.Rosati, M.Viviani N-d elastic scattering using the hyperspherical harmonics approach with realistic local and nonlocal interactions NUCLEAR REACTIONS 2H(n, n), (p, p), (polarized n, n), (polarized p, p), E(cm)=0.266-2.0 MeV; calculated scattering lengths, differential σ, σ(θ), vector and tensor analyzing powers using hyperspherical harmonic (HH) approach and two- and three-nucleon interactions (Argonne v18, N3LO-Idaho, Vlow-k, Urbana IX, N2LO). Comparisons with experimental data.
doi: 10.1103/PhysRevC.80.034003
2009PA34 Phys.Rev. C 80, 034004 (2009) S.Pastore, L.Girlanda, R.Schiavilla, M.Viviani, R.B.Wiringa Electromagnetic currents and magnetic moments in chiral effective field theory χEFT)
doi: 10.1103/PhysRevC.80.034004
2008KI08 J.Phys.(London) G35, 063101 (2008) A.Kievsky, S.Rosati, M.Viviani, L.E.Marcucci, L.Girlanda A high-precision variational approach to three- and four-nucleon bound and zero-energy scattering states
doi: 10.1088/0954-3899/35/6/063101
2008SC14 Phys.Rev. C 78, 014002 (2008); Erratum Phys.Rev. C 83, 029902 (2011) R.Schiavilla, M.Viviani, L.Girlanda, A.Kievsky, L.E.Marcucci Neutron spin rotation in n(pol)-d scattering
doi: 10.1103/PhysRevC.78.014002
2007GI15 Phys.Rev. C 76, 044002 (2007) L.Girlanda, M.Viviani, W.H.Klink Bakamjian-Thomas mass operator for few-nucleon systems from chiral dynamics
doi: 10.1103/PhysRevC.76.044002
2007RI02 Nucl.Phys. A784, 25 (2007) A.S.Rinat, M.F.Taragin, M.Viviani Inclusive scattering data on light nuclei as a tool for the extraction of GnM NUCLEAR REACTIONS 2H, 4He(e, e'X), E=0.9-21 GeV; analyzed σ(E, θ), related data. 1n deduced magnetic form factor.
doi: 10.1016/j.nuclphysa.2006.10.086
2007RI05 Eur.Phys.J. A 31, 415 (2007) A.S.Rinat, M.F.Taragin, M.Viviani Extraction of GnM from inclusive electron scattering on D, 4He NUCLEAR REACTIONS 2H, 4He(e, e'X), E=high; analyzed σ(E, θ), related data. 1n deduced magnetic form factor.
doi: 10.1140/epja/i2006-10293-3
2007VI04 Eur.Phys.J. A 31, 429 (2007) Few- and many-body methods in nuclear physics
doi: 10.1140/epja/i2006-10263-9
2007VI12 Nucl.Phys. A790, 46c (2007) M.Viviani, L.Girlanda, A.Kievsky, L.E.Marcucci, S.Rosati Bound and scattering states with non-local potentials NUCLEAR STRUCTURE 3H, 4He; calculated binding energies, radii, related features. Hyperspherical harmonic approach.
doi: 10.1016/j.nuclphysa.2007.03.054
2007VI13 Phys.Rev.Lett. 99, 112002 (2007) M.Viviani, R.Schiavilla, B.Kubis, R.Lewis, L.Girlanda, A.Kievsky, L.E.Marcucci, S.Rosati Isospin Mixing in the Nucleon and 4He and the Nucleon Strange Electric Form Factor NUCLEAR STRUCTURE 4He; calculated isospin breaking corrections needed to isolate the contribution of nucleon strange electric form factor to the parity violating assymetry measured in polarized electron scattering.
doi: 10.1103/PhysRevLett.99.112002
2006FI06 Phys.Rev. C 74, 034001 (2006) B.M.Fisher, C.R.Brune, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, T.C.Black, M.Viviani, A.Kievsky, S.Rosati Proton-3He elastic scattering at low energies NUCLEAR REACTIONS 3He(p, p), (polarized p, p), E=0.99, 1.59, 2.24, 3.11, 4.02 MeV; measured σ(θ), Ay(θ). Four-body variational calculations with realistic two- and three-body interactions.
doi: 10.1103/PhysRevC.74.034001
2006KI05 Few-Body Systems 38, 63 (2006) A.Kievsky, M.Viviani, L.E.Marcucci, S.Rosati Variational Description of Bound States in Three- and Four-Nucleon Systems NUCLEAR STRUCTURE A=3-4; calculated binding energies, configurations. Hyperspherical harmonic basis.
doi: 10.1007/s00601-005-0132-0
2006VI05 Few-Body Systems 39, 159 (2006) M.Viviani, L.E.Marcucci, S.Rosati, A.Kievsky, L.Girlanda Variational Calculation on A = 3 and 4 Nuclei with Non-Local Potentials NUCLEAR STRUCTURE 3H, 3,4He; calculated binding energies, radii, related features. Hyperspherical harmonic approach, non-local two-body potentials.
doi: 10.1007/s00601-006-0158-y
2006WI09 Phys.Rev. C 73, 044004 (2006) H.Witala, J.Golak, R.Skibinski, W.Glockle, A.Nogga, E.Epelbaum, H.Kamada, A.Kievsky, M.Viviani Testing nuclear forces by polarization transfer coefficients in d(p(pol), p(pol))d and d(p(pol), d(pol))p reactions at Elabp = 22.7 MeV NUCLEAR REACTIONS 2H(polarized p, p), (polarized p, d), E=22.7 MeV; measured spin transfer coefficients. Comparison with model predictions using various potentials.
doi: 10.1103/PhysRevC.73.044004
2005DE21 Phys.Rev. C 71, 064003 (2005) A.Deltuva, A.C.Fonseca, A.Kievsky, S.Rosati, P.U.Sauer, M.Viviani Benchmark calculation for proton-deuteron elastic scattering observables including the Coulomb interaction NUCLEAR REACTIONS 2H(p, p), E=3-65 MeV; calculated σ(θ), proton and deuteron analyzing powers, tensor analyzing powers, spin transfer coefficients.
doi: 10.1103/PhysRevC.71.064003
2005LA06 Phys.Rev. C 71, 034004 (2005) R.Lazauskas, J.Carbonell, A.C.Fonseca, M.Viviani, A.Kievsky, S.Rosati Low energy n-3H scattering: A novel testground for nuclear interactions NUCLEAR REACTIONS 3H(n, n), E(cm)=0.1-5 MeV; calculated phase shifts, total σ. Three methods compared.
doi: 10.1103/PhysRevC.71.034004
2005MA18 Eur.Phys.J. A 24, Supplement 1, 95 (2005) L.E.Marcucci, M.Viviani, R.Schiavilla, A.Kievsky, S.Rosati Electrodisintegration of 3He below and above deuteron breakup threshold NUCLEAR REACTIONS 2H(p, γ), E(cm)=2 MeV; calculated σ(θ), analyzing powers. 3He(e, e'), E not given; calculated longitudinal and transverse response functions. 3He(e, e'd), E=370, 576 MeV; calculated σ(E, θ). Pair-correlated hyperspherical harmonics method, comparison with data.
doi: 10.1140/epjad/s2005-05-017-7
2005MA54 Phys.Rev. C 72, 014001 (2005) L.E.Marcucci, M.Viviani, R.Schiavilla, A.Kievsky, S.Rosati Electromagnetic structure of A = 2 and 3 nuclei and the nuclear current operator NUCLEAR REACTIONS 2H(p, p), E(cm)=6.66 MeV; 2H(p, γ), E(cm)=2-18.66calculated σ(θ), analyzing powers. 1,2H(n, γ), E=thermal; calculated σ. 2H(n, γ), E(cm)=6, 7.2 MeV; calculated σ(θ). Comparisons with data. NUCLEAR STRUCTURE 3H, 3He; calculated μ, form factors.
doi: 10.1103/PhysRevC.72.014001
2005RI09 Phys.Rev. C 72, 015211 (2005) A.S.Rinat, M.F.Taragin, M.Viviani Simple qualitative description of EMC ratios μA for 0.2 ≤ x ≤ 1.5 and some sample calculations NUCLEAR STRUCTURE 4He, C, Fe, Au; calculated structure function ratios. Comparison with data.
doi: 10.1103/PhysRevC.72.015211
2005SC02 Phys.Rev.Lett. 94, 072303 (2005) R.Schiavilla, O.Benhar, A.Kievsky, L.E.Marcucci, M.Viviani Polarization Transfer in 4He(e(pol), e'p(pol))3H: Is the Ratio GEp/GMp Modified in the Nuclear Medium? NUCLEAR REACTIONS 4He(polarized e, e'p), E=high; analyzed polarization transfer, induced polarization; deduced no medium modification.
doi: 10.1103/PhysRevLett.94.072303
2005SC30 Phys.Rev. C 72, 064003 (2005) R.Schiavilla, O.Benhar, A.Kievsky, L.E.Marcucci, M.Viviani Two-body electrodisintegration of 3He at high momentum transfer NUCLEAR REACTIONS 3He(e, e'p), E=high; calculated σ vs missing momentum, longitudinal-transverse asymmetry. Comparison with data.
doi: 10.1103/PhysRevC.72.064003
2005VI02 Phys.Rev. C 71, 024006 (2005) M.Viviani, A.Kievsky, S.Rosati Calculation of the α-particle ground state within the hyperspherical harmonic basis NUCLEAR STRUCTURE 4H; calculated binding energy, radius, wave function, asymptotic normalization constants. Hyperspherical harmonic basis.
doi: 10.1103/PhysRevC.71.024006
2005VI05 Nucl.Phys. A751, 226c (2005) M.Viviani, A.Kievsky, L.E.Marcucci, S.Rosati New developments in the study of few-nucleon systems
doi: 10.1016/j.nuclphysa.2005.02.007
2004KI03 Phys.Rev. C 69, 014002 (2004) A.Kievsky, M.Viviani, L.E.Marcucci N-d scattering including electromagnetic forces NUCLEAR REACTIONS 2H(n, n), E=1.2, 1.9, 6.5 MeV; calculated Ay(θ). 2H(p, p), E=1, 3, 5, 10 MeV; 1H(d, d), E=20 MeV; calculated Ay(θ), iT11(θ). 2H(p, p), E=65 MeV; calculated σ(θ), analyzing powers. Coulomb plus magnetic moment interactions. Comparison with data.
doi: 10.1103/PhysRevC.69.014002
2004KI11 Nucl.Phys. A737, 61 (2004) A.Kievsky, M.Viviani, L.E.Marcucci, S.Rosati Recent Developments in Few-Nucleon Systems NUCLEAR REACTIONS 2H(n, n), E=1.2, 1.9 MeV; 2H(p, p), E=1, 3 MeV; calculated analyzing powers, contribution from magnetic moment interaction.
doi: 10.1016/j.nuclphysa.2004.03.044
2004RI13 Phys.Rev. C 70, 014003 (2004) A.S.Rinat, M.F.Taragin, M.Viviani Neutron magnetic form factor GnM(Q2) from quasielastic inclusive scattering data on D and 4He NUCLEAR REACTIONS 2H(e, e'X), E=4 GeV; 4He(e, e'X), E=2-3.6 GeV; analyzed quasielastic σ(E, θ), related data. 1n deduced magnetic form factor.
doi: 10.1103/PhysRevC.70.014003
2004VI06 Nucl.Phys. A737, 205 (2004) M.Viviani, A.Kievsky, S.Rosati Convergence of the Hyperspherical Harmonic Expansion for Four Body Scattering Problems
doi: 10.1016/j.nuclphysa.2004.03.065
2003NO01 Phys.Rev. C 67, 034004 (2003) A.Nogga, A.Kievsky, H.Kamada, W.Glockle, L.E.Marcucci, S.Rosati, M.Viviani Three-nucleon bound states using realistic potential models NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, mass difference, wave functions. Three-nucleon potential, Fadeev and hyperspherical harmonics calculations.
doi: 10.1103/PhysRevC.67.034004
2003PA19 Phys.Rev. C 67, 055206 (2003) T.-S.Park, L.E.Marcucci, R.Schiavilla, M.Viviani, A.Kievsky, S.Rosati, K.Kubodera, D.-P.Min, M.Rho Parameter-free effective field theory calculation for the solar proton-fusion and hep processes NUCLEAR REACTIONS 1H, 3He(p, e+ν), E=low; calculated threshold astrophysical S-factors, dependence on cutoff parameters. Effective field theory.
doi: 10.1103/PhysRevC.67.055206
2003VI01 Phys.Rev. C 67, 034003 (2003) M.Viviani, A.Kievsky, A.S.Rinat Gersch-Rodriquez-Smith computation of deep inelastic electron scattering on 4He NUCLEAR REACTIONS 4He(e, e'X), E=3.6 GeV; calculated σ(E, θ). Comparison with data.
doi: 10.1103/PhysRevC.67.034003
2003VI06 Eur.Phys.J. A 17, 483 (2003) M.Viviani, L.E.Marcucci, A.Kievsky, S.Rosati, R.Schiavilla Electromagnetic and weak transitions in light nuclei NUCLEAR REACTIONS 2H(p, γ), E(cm)=2, 3.33 MeV; calculated σ(θ), analyzing powers. 3He(μ-, ν), E not given; calculated capture rate, angular correlation parameters.
doi: 10.1140/epja/i2002-10199-0
2003XU02 Phys.Rev. C 67, 012201 (2003) W.Xu, B.Anderson, L.Auberbach, T.Averett, W.Bertozzi, T.Black, J.Calarco, L.Cardman, G.D.Cates, Z.W.Chai, J.P.Chen, S.Choi, E.Chudakov, S.Churchwell, G.S.Corrado, C.Crawford, D.Dale, A.Deur, P.Djawotho, T.W.Donnelly, D.Dutta, J.M.Finn, H.Gao, R.Gilman, A.V.Glamazdin, C.Glashausser, W.Glockle, J.Golak, J.Gomez, V.G.Gorbenko, J.-O.Hansen, F.W.Hersman, D.W.Higinbotham, R.Holmes, C.R.Howell, E.Hughes, B.Humensky, S.Incerti, C.W.de Jager, J.S.Jensen, X.Jiang, C.E.Jones, M.Jones, R.Kahl, H.Kamada, A.Kievsky, I.Kominis, W.Korsch, K.Kramer, G.Kumbartzki, M.Kuss, E.Lakuriqi, M.Liang, N.Liyanage, J.LeRose, S.Malov, D.J.Margaziotis, J.W.Martin, K.McCormick, R.D.McKeown, K.McIlhany, Z.-E.Meziani, R.Michaels, G.W.Miller, J.Mitchell, S.Nanda, E.Pace, T.Pavlin, G.G.Petratos, R.I.Pomatsalyuk, D.Pripstein, D.Prout, R.D.Ransome, Y.Roblin, M.Rvachev, A.Saha, G.Salme, M.Schnee, T.Shin, K.Slifer, P.A.Souder, S.Strauch, R.Suleiman, M.Sutter, B.Tipton, L.Todor, M.Viviani, B.Vlahovic, J.Watson, C.F.Williamson, H.Witala, B.Wojtsekhowski, F.Xiong, J.Yeh, P.Zolnierczuk Plane-wave impulse approximation extraction of the neutron magnetic form factor from quasielastic 3He(pol)(e(pol), e') at Q2 = 0.3 to 0.6 (GeV/c)2 NUCLEAR REACTIONS 3He(polarized e, e'), E=0.778, 1.727 GeV; measured transverse spin-dependent asymmetry. 1n deduced magnetic form factor. Polarized target.
doi: 10.1103/PhysRevC.67.012201
2002MA66 Phys.Rev. C 66, 054003 (2002) L.E.Marcucci, R.Schiavilla, S.Rosati, A.Kievsky, M.Viviani Theoretical study of 3He(μ-, νμ)3H capture NUCLEAR REACTIONS 3He(μ-, ν), E not given; calculated capture rate, angular correlation parameters. Correlated hyperspherical harmonics wave function, several NN interactions compared. NUCLEAR STRUCTURE 3H, 3He; calculated binding energies.
doi: 10.1103/PhysRevC.66.054003
2002WO05 Phys.Rev. C65, 034002 (2002) M.H.Wood, C.R.Brune, B.M.Fisher, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, A.Kievsky, S.Rosati, M.Viviani Low-Energy p-d Scattering: High-Precision data, comparisons with theory, and phase-shift analyses NUCLEAR REACTIONS 2H(polarized p, p), 1H(polarized d, d), E(cm)=667 keV; measured σ(θ), Ay(θ), other analyzing powers; deduced phase shift parameters. Comparison with NN and 3N model predictions.
doi: 10.1103/PhysRevC.65.034002
2001BR12 Phys.Rev. C63, 044013 (2001) C.R.Brune, W.H.Geist, H.J.Karwowski, E.J.Ludwig, K.D.Veal, M.H.Wood, A.Kievsky, S.Rosati, M.Viviani Proton-Deuteron Elastic Scattering at Low Energies NUCLEAR REACTIONS 2H(polarized p, p), E=431.3-2000 keV; measured σ(θ), analyzing power vector and tensor components. Comparison with calculations using hyperspherical harmonic basis and different nuclear potentials.
doi: 10.1103/PhysRevC.63.044013
2001KA47 Phys.Rev. C64, 044001 (2001) H.Kamada, A.Nogga, W.Glockle, E.Hiyama, M.Kamimura, K.Varga, Y.Suzuki, M.Viviani, A.Kievsky, S.Rosati, J.Carlson, S.C.Pieper, R.B.Wiringa, P.Navratil, B.R.Barrett, N.Barnea, W.Leidemann, G.Orlandini Benchmark Test Calculation of a Four-Nucleon Bound State NUCLEAR STRUCTURE A=4; calculated four-nucleon bound state energy, radius, related features. Several approaches compared.
doi: 10.1103/PhysRevC.64.044001
2001KI03 Phys.Rev. C63, 024005 (2001) A.Kievsky, M.H.Wood, C.R.Brune, B.M.Fisher, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, S.Rosati, M.Viviani Evidence for Three Nucleon Force Effects in p-d Elastic Scattering NUCLEAR REACTIONS 2H(p, p), E=1 MeV; measured σ(θ); deduced contribution from three-nucleon force. Comparisons with model predictions.
doi: 10.1103/PhysRevC.63.024005
2001KI11 Phys.Rev. C63, 064004 (2001) A.Kievsky, J.L.Friar, G.L.Payne, S.Rosati, M.Viviani Phase Shifts and Mixing Parameters for Low-Energy Proton-Deuteron Scattering NUCLEAR REACTIONS 2H(p, p), E=1, 2, 3 MeV; calculated phase shifts, mixing parameters. AV14 two-body potential.
doi: 10.1103/PhysRevC.63.064004
2001KI22 Nucl.Phys. A689, 349c (2001) A.Kievsky, M.H.Wood, C.R.Brune, B.M.Fisher, H.J.Karwowski, D.S.Leonard, E.J.Ludwig, S.Rosati, M.Viviani χ2 Analysis of p-d Differential Cross Sections at Low Energies NUCLEAR REACTIONS 1H(d, d), E=1 MeV; measured σ(θ); deduced model parameters.
doi: 10.1016/S0375-9474(01)00852-1
2001KI24 Phys.Rev. C64, 024002 (2001) A.Kievsky, M.Viviani, S.Rosati Polarization Observables in p-d Scattering below 30 MeV NUCLEAR REACTIONS 2H(p, np), E=4-30 MeV; calculated breakup σ. 2H(polarized p, X), (polarized n, X), E=1-28 MeV; calculated σ(θ), vector and tensor analyzing powers. Argonne AV18 interaction, Urbana three-nucleon potential. Comparisons with data.
doi: 10.1103/PhysRevC.64.024002
2001KI30 Phys.Rev. C64, 041001 (2001) A.Kievsky, S.Rosati, M.Viviani Coulomb Effects in Nucleon-Deuteron Polarization-Transfer Coefficients NUCLEAR REACTIONS 2H(polarized n, n), (polarized p, p), E=10, 19, 22.7 MeV; calculated polarization transfer coefficients; deduced Coulomb and three-nucleon interaction effects. Comparison with data.
doi: 10.1103/PhysRevC.64.041001
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