NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = R.B.Wiringa Found 98 matches. 2023PI01 Phys.Rev. C 107, 014314 (2023) M.Piarulli, S.Pastore, R.B.Wiringa, S.Brusilow, R.Lim Densities and momentum distributions in A ≤ 12 nuclei from chiral effective field theory interactions NUCLEAR STRUCTURE 3H, 3,4,8He, 6,7Li, 9Be, 10B, 12C; calculated one-body neutron and proton densities, relative-distance np and pp pair densities, total number of spin-isospin pairs, total one-body neutron and proton momentum distributions, total np and pp momentum distributions, ratio of np and pp pairs as function of relative momentum. Variational Monte Carlo calculations with AV18+UX phenomenological three-nucleon interactions.
doi: 10.1103/PhysRevC.107.014314
2022AN04 Phys.Rev. C 105, 014002 (2022) L.Andreoli, J.Carlson, A.Lovato, S.Pastore, N.Rocco, R.B.Wiringa Electron scattering on A=3 nuclei from quantum Monte Carlo based approaches NUCLEAR REACTIONS 3H(e, e), (e, e'), at momentum transfer θ=300 MeV/c; calculated total longitudinal response density. 3H, 3He(e, e'), at momentum transfer θ=300, 500, 700 MeV/c; calculated longitudinal and transverse response functions, single proton momentum distribution of 3He. 3He(e, e), (e, e'), E=287.2, 319.1, 469.4, 499.9, 560.3, 667.3 MeV; 3H(e, e), (e, e'), E=367.7, 506.9, 557.9, 652.4, 790.2 MeV; calculated inclusive double-differential σ(E). Green's function Monte Carlo (GFMC) method with two approaches for the final hadronic state: the spectral-function (SF) formalism and the short-time approximation (STA). Comparison with experimental data.
doi: 10.1103/PhysRevC.105.014002
2022KU08 Phys.Rev. C 105, 034314 (2022) A.N.Kuchera, D.Bazin, T.Phan, J.A.Tostevin, M.Babo, T.Baumann, P.C.Bender, M.Bowry, J.Bradt, J.Brown, P.A.DeYoung, B.Elman, J.E.Finck, A.Gade, G.F.Grinyer, M.D.Jones, B.Longfellow, E.Lunderberg, T.H.Redpath, W.F.Rogers, K.Stiefel, M.Thoennessen, D.Votaw, D.Weisshaar, K.Whitmore, R.B.Wiringa Mirror nucleon removal reactions in p-shell nuclei NUCLEAR REACTIONS 9Be(7Li, 6He), (7Li, 6Li), (9Li, 8Li), (10Be, 9Li) E=80 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced partial σ to the individual final states of the daughter nuclei. Comparison to fully microscopic variational Monte Carlo (VMC) model calculations. Systematics of partial σ for nucleon removal reactions in mirror pairs. CAESAR array of 170 CsI(Te) scintillators. Secondaries beam produced in 9Be(16O, X), E=150 MeV/nucleon reaction and delivered to the target via A1900 fragment separator (NSCL-MSU).
doi: 10.1103/PhysRevC.105.034314
2022LO07 Phys.Rev. C 105, 055808 (2022) A.Lovato, I.Bombaci, D.Logoteta, M.Piarulli, R.B.Wiringa Benchmark calculations of infinite neutron matter with realistic two- and three-nucleon potentials
doi: 10.1103/PhysRevC.105.055808
2022PA12 Phys.Rev. C 105, 049802 (2022) S.Pastore, J.Carlson, R.Schiavilla, J.L.Barrow, S.Gandolfi, R.B.Wiringa Reply to "Comment on 'Quasielastic lepton scattering and back-to-back nucleons in the short-time approximation" NUCLEAR REACTIONS 4He(e, e'), q=300-800 MeV/c; calculated transverse scaling functions for 4He with one-body and one plus two-body currents. Short time approximation (STA). Pointed that enhanced scaling reflects quasielastic kinematics and the dominant role played by pion-exchange interactions and currents in the quasielastic regime.
doi: 10.1103/PhysRevC.105.049802
2022SC13 Phys.Rev. C 106, 054323 (2022) J.Schmitt, G.B.King, R.G.T.Zegers, Y.Ayyad, D.Bazin, B.A.Brown, A.Carls, J.Chen, A.Davis, M.DeNudt, J.Droste, B.Gao, C.Hultquist, H.Iwasaki, S.Noji, S.Pastore, J.Pereira, M.Piarulli, H.Sakai, A.Stolz, R.Titus, R.B.Wiringa, J.C.Zamora Probing spin-isospin excitations in proton-rich nuclei via the 11C(p, n)11N reaction NUCLEAR REACTIONS 1H(11C, n), E=95 MeV/nucleon; measured reaction products, time-of-flight, En, In, (particle)n-coin, angular distribution; deduced σ(θ), σ(θ, E), cumulative Gamow-Teller transition strengths, B(GT) values to the 1/2- state at 0.73 MeV and the 3/2- state at 2.86 MeV in 11N. Multipole decomposition analysis. Comparison to shell-model calculations with wbp interaction and to experimental data on the 11B(n, p), (d, 2He), (t, 3He) reactions. Ursinus liquid hydrogen target coupled to Low Energy Neutron Detector Array (LENDA) and S800 spectrograph. 11C beam produced from Be(16O, X) reaction and purified with A1900 fragment separator at Coupled Cyclotron Facility (CCF) at the NSCL.
doi: 10.1103/PhysRevC.106.054323
2022WE03 Phys.Rev. C 106, 054319 (2022) R.Weiss, A.Lovato, R.B.Wiringa Isospin-symmetry implications for nuclear two-body distributions and short-range correlations NUCLEAR STRUCTURE 6,7Li, 6,10Be; calculated two-body pp, nn and pn densities with spins equal 0 and 1. Ab initio variational Monte Carlo calculations with AV18 + UX potential. RADIOACTIVITY 10Be(2β-); calculated 0νββ Fermi transition densities.
doi: 10.1103/PhysRevC.106.054319
2022WE06 Phys.Rev. C 106, 065501 (2022) R.Weiss, P.Soriano, A.Lovato, J.Menendez, R.B.Wiringa Neutrinoless double-β decay: Combining quantum Monte Carlo and the nuclear shell model with the generalized contact formalism RADIOACTIVITY 12,10Be, 14C, 48Ca, 76Ge, 130Te, 136Xe(2β-); calculated Fermi, Gamow-Teller, and short-range transition densities, 0νββ-decay matrix elements. Calculation within framework based on the generalized contact formalism that combines the nuclear shell model and quantum Monte Carlo methods.
doi: 10.1103/PhysRevC.106.065501
2021AT02 Phys.Rev. C 104, 059802 (2021) M.C.Atkinson, W.H.Dickhoff, M.Piarulli, A.Rios, R.B.Wiringa Reply to "Comment on 'Reexamining the relation between the binding energy of finite nuclei and the equation of state of infinite nuclear matter'"
doi: 10.1103/PhysRevC.104.059802
2020AT02 Phys.Rev. C 102, 044333 (2020) M.C.Atkinson, W.H.Dickhoff, M.Piarulli, A.Rios, R.B.Wiringa Reexamining the relation between the binding energy of finite nuclei and the equation of state of infinite nuclear matter NUCLEAR STRUCTURE 12C, 40,48Ca, 208Pb; calculated binding energies, binding energy as a function of radius in 12C, energy densities using a dispersive optical model. Comparison with ab initio self-consistent Green's-function calculations, and with experimental data. 8Be; calculated total binding-energy density, the kinetic-energy density, the two-body potential-energy density, and the three-body potential-energy density using Green's-function Monte Carlo method, with the Argonne-Urbana two- and three-body interactions. 12C; calculated three-body potential-energy densities for different chiral interactions and the Urbana-X. NUCLEAR REACTIONS 12C(p, p), (n, n), (polarized p, p), (polarized n, n), (p, X), (n, X), E<200 MeV; calculated differential σ(θ, E) and analyzing powers Ay(θ, E) for elastic scattering, proton and neutron total reaction σ(E) generated from the dispersive optical model (DOM). Comparison with experimental data.
doi: 10.1103/PhysRevC.102.044333
2020KI13 Phys.Rev. C 102, 025501 (2020) G.B.King, L.Andreoli, S.Pastore, M.Piarulli, R.Schiavilla, R.B.Wiringa, J.Carlson, S.Gandolfi Chiral effective field theory calculations of weak transitions in light nuclei NUCLEAR STRUCTURE 3H, 4,6,8He, 6,7,8Li, 7,8Be, 8,10B, 10C; calculated energies of ground and excited states, point-proton radii using Green's function Monte Carlo (GFMC) calculations, and compared with experimental data. RADIOACTIVITY 6,8He, 8Li(β-); 7Be(EC); 8B, 10C(β+); calculated Gamow-Teller reduced matrix elements (RMEs), two-body transition densities and pair densities using chiral axial currents and GFMC (VMC) wave functions, with NV2+3-Ia and NV2+3-Ia* Hamiltonian models, and RMEs compared to experimental data.
doi: 10.1103/PhysRevC.102.025501
2020PA15 Phys.Rev. C 101, 044612 (2020) S.Pastore, J.Carlson, S.Gandolfi, R.Schiavilla, R.B.Wiringa Quasielastic lepton scattering and back-to-back nucleons in the short-time approximation NUCLEAR REACTIONS 4He(e, e'), q=300-800 MeV/c; calculated transverse response densities, longitudinal and transverse sum rules, contribution of response density in the back-to-back configurations due to scattering from pp and nn pairs. Short time approximation (STA), combined with quantum Monte Carlo computational methods. Comparison with experimental data, and with results from Green's function Monte Carlo (GFMC) method. Relevance to current and planned neutrino oscillation experiments.
doi: 10.1103/PhysRevC.101.044612
2020PI05 Phys.Rev. C 101, 045801 (2020) M.Piarulli, I.Bombaci, D.Logoteta, A.Lovato, R.B.Wiringa Benchmark calculations of pure neutron matter with realistic nucleon-nucleon interactions
doi: 10.1103/PhysRevC.101.045801
2019CH51 Phys.Rev. C 100, 064314 (2019) J.Chen, K.Auranen, M.L.Avila, B.B.Back, M.A.Caprio, C.R.Hoffman, D.Gorelov, B.P.Kay, S.A.Kuvin, Q.Liu, J.L.Lou, A.O.Macchiavelli, D.G.McNeel, T.L.Tang, D.Santiago-Gonzalez, R.Talwar, J.Wu, G.Wilson, R.B.Wiringa, Y.L.Ye, C.X.Yuan, H.L.Zang Experimental study of the low-lying negative-parity states in 11Be using the 12B (d, 3He) 11Be reaction NUCLEAR REACTIONS 2H(12B, 3He)11Be, (12B, 12B'), E=12 MeV/nucleon, [secondary 12Be beam from 2H(11B, 12B), E=13.5 MeV/nucleon primary reaction]; measured reaction products, E(3He), I(3He), (3He)(11Be)- and (3He)(10Be)-coin, σ(θ) using the HELical Orbit Spectrometer (HELIOS) at the ATLAS In-Flight facility at ANL. Deuterated polyethylene (CD2)n target. 11Be; deduced levels, l-transfers, configurations, spectroscopic factors. Distorted wave Born approximation (DWBA) analysis. Comparison with previous experimental data, and with results from variational Monte Carlo and no-core shell-model calculations. Comparison with 11B(d, 3He)10Be experimental data.
doi: 10.1103/PhysRevC.100.064314
2019CI06 Phys.Rev. C 100, 055504 (2019) V.Cirigliano, W.Dekens, J.de Vries, M.L.Graesser, E.Mereghetti, S.Pastore, M.Piarulli, U.van Kolck, R.B.Wiringa Renormalized approach to neutrinoless double-β decay RADIOACTIVITY 6He, 12Be(2β-); calculated Fermi (F), Gamow-Teller (GT), and tensor (T) densities, variational Monte Carlo (VMC) for the dimensionless matrix elements of the long-range and short-range neutrino-exchange potentials and short-range transition densities for 0νββ decay modes; deduced that a short-range operator is only needed in spin-singlet s-wave transitions, while leading-order transitions involving higher partial waves depend solely on long-range currents.Ab initio calculations of the matrix elements for 0νββ decay using pionless and chiral effective field theory, extended to include next-to-leading-order corrections.
doi: 10.1103/PhysRevC.100.055504
2019DI06 Phys.Rev. C 99, 034004 (2019) N.N.Dinur, O.J.Hernandez, S.Bacca, N.Barnea, C.Ji, S.Pastore, M.Piarulli, R.B.Wiringa Zemach moments and radii of 2, 3H and 3, 4He NUCLEAR STRUCTURE 2,3H, 3,4He; calculated Zemach electromagnetic moments, charge radii, ground-state wave-functions using various few-body methods, such as Numerov algorithm or the harmonic oscillator expansion method for A=2 nuclei, and Monte Carlo (VMC) and Green's function Monte Carlo (GFMC) methods, with hyperspherical harmonics (HH) expansions and momentum-space formulation (HH-p), and the effective interaction scheme in coordinate space (EIHH). Comparison with experimental values. Benchmarking of electromagnetic moments relevant to ongoing experimental efforts of muon-nucleus systems, and to muonic atom data measured by the CREMA collaboration at the Paul Scherrer Institute.
doi: 10.1103/PhysRevC.99.034004
2019MA33 Phys.Rev.Lett. 122, 182501 (2019) B.Maass, T.Huther, K.Konig, J.Kramer, J.Krause, A.Lovato, P.Muller, K.Pachucki, M.Puchalski, R.Roth, R.Sanchez, F.Sommer, R.B.Wiringa, W.Nortershauser Nuclear Charge Radii of 10, 11B NUCLEAR MOMENTS 10,11B; measured frequencies; deduced nuclear charge radii by combining high-accuracy ab initio mass-shift calculations and a high-accuracy measurement of the isotope shift.
doi: 10.1103/PhysRevLett.122.182501
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
2018PA05 Phys.Rev. C 97, 014606 (2018) S.Pastore, J.Carlson, V.Cirigliano, W.Dekens, E.Mereghetti, R.B.Wiringa Neutrinoless double-β decay matrix elements in light nuclei RADIOACTIVITY 6,8,10He, 10,12Be, 48Ca, 76Ge, 136Xe(2β-); calculated dimensionless matrix elements for light Majorana-neutrino exchange in 0νββ decay using variational Monte Carlo (VMC) wave functions obtained from the Argonne ν18 two-nucleon potential and Illinois-7 three-nucleon interaction.
doi: 10.1103/PhysRevC.97.014606
2018PA08 Phys.Rev. C 97, 022501 (2018) S.Pastore, A.Baroni, J.Carlson, S.Gandolfi, StevenC.Pieper, R.Schiavilla, R.B.Wiringa Quantum Monte Carlo calculations of weak transitions in A = 6-10 nuclei RADIOACTIVITY 3H, 6He(β-); 10C(β+); 7Be(EC); calculated ab initio Gamow-Teller (GT) reduced matrix elements (RMEs) using variational and Green's function Monte Carlo wave functions (GFMC, VMC)from the Argonne v18 two-nucleon and Illinois-7 three-nucleon interactions, and axial many-body currents from either meson-exchange phenomenology or chiral effective field theory. Comparison with experimental data. Calculations for 3H decay in Supplemental Material (Ref, 32 in paper).
doi: 10.1103/PhysRevC.97.022501
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
2017LO11 Phys.Rev. C 96, 024326 (2017) D.Lonardoni, A.Lovato, S.C.Pieper, R.B.Wiringa Variational calculation of the ground state of closed-shell nuclei up to A=40 NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated cluster contributions to energies per nucleon, point radii, total energies, charge radii, point proton and two-nucleon densities, operator two-nucleon densities, proton momentum distributions, integrated strengths, longitudinal elastic form factors, Coulomb sum rules, central and radial correlation functions, and variational parameters. Variational Monte Carlo calculations using realistic phenomenological two- and three-nucleon potentials AV18 and AV18+UIX. Comparison with experimental data.
doi: 10.1103/PhysRevC.96.024326
2017WU03 Phys.Rev. C 95, 014310 (2017) A.H.Wuosmaa, S.Bedoor, K.W.Brown, W.W.Buhro, Z.Chajecki, R.J.Charity, W.G.Lynch, J.Manfredi, S.T.Marley, D.G.McNeel, A.S.Newton, D.V.Shetty, R.H.Showalter, L.G.Sobotka, M.B.Tsang, J.R.Winkelbauer, R.B.Wiringa Ground-state properties of 5H from the 6He (d, 3He) 5H reaction NUCLEAR REACTIONS 2H(6He, 3He), (6He, t), E=55 MeV/nucleon, [secondary 6He beam from 9Be(18O, X), E=120 MeV/nucleon and using A1900 fragment separator at NSCL-MSU facility]; measured particle identification (PID) spectra, kinetic-energy spectra of low-energy 3He and 3H particles using High Resolution Array (HiRA) of charged-particle-detector telescopes and CsI(Tl) scintillator crystals; deduced correlations between E(3He) and E(3H), and E(3H) and E(4He), Q-value dependence of cross sections from DWBA calculations, 3H recoil-energy distributions from the decay of 5H, beam-like recoils and two-neutron correlations. 5H, 5He; deduced energies and widths of resonances corresponding to the ground state. Comparison with previous experimental results, shell-model and ab initio nuclear-structure calculations. COMPILATION 5H; compiled theoretical and previous (1968-2005) experiments for identification, and results of resonance energy and width of ground-state resonance of 5H.
doi: 10.1103/PhysRevC.95.014310
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
2014GA06 Eur.Phys.J. A 50, 10 (2014) S.Gandolfi, J.Carlson, S.Reddy, A.W.Steiner, R.B.Wiringa The equation of state of neutron matter, symmetry energy and neutron star structure
doi: 10.1140/epja/i2014-14010-5
2014PA41 Phys.Rev. C 90, 024321 (2014) S.Pastore, R.B.Wiringa, S.C.Pieper, R.Schiavilla Quantum Monte Carlo calculations of electromagnetic transitions in 8Be with meson-exchange currents derived from chiral effective field theory NUCLEAR STRUCTURE 8Be; calculated Green's function Monte Carlo (GFMC) ground-state energies, levels, J, π, E2 and M1 transition matrix elements, isospin-mixed widths, one- and two-body M1 transition densities. Argonne ν18 two-nucleon and Illinois-7 three-nucleon potentials and chiral effective field theory. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.024321
2014WI01 Phys.Rev. C 89, 024305 (2014) R.B.Wiringa, R.Schiavilla, S.C.Pieper, J.Carlson Nucleon and nucleon-pair momentum distributions in A ≤ 12 nuclei NUCLEAR STRUCTURE 2H, 3,4,6,8He, 6,7,8,9Li, 8,9,10Be, 10B, 12C; calculated neutron and proton single-nucleon distributions, nucleon-pair, and nucleon-cluster momentum distributions distribution, spin-isospin densities and correlations. Variational Monte Carlo wave functions using realistic Argonne ν18 two-nucleon and Urbana X three-nucleon potentials.
doi: 10.1103/PhysRevC.89.024305
2013AL09 Phys.Lett. B 721, 224 (2013) H.Al Falou, R.Kanungo, C.Andreoiu, D.S.Cross, B.Davids, M.Djongolov, A.T.Gallant, N.Galinski, D.Howell, R.Kshetri, D.Niamir, J.N.Orce, A.C.Shotter, S.Sjue, I.Tanihata, I.J.Thompson, S.Triambak, M.Uchida, P.Walden, R.B.Wiringa Inelastic scattering of 9Li and excitation mechanism of its first excited state NUCLEAR REACTIONS C, 2H(9Li, 8Li), (9Li, X), (9Li, 9Li), E=5 MeV/nucleon; measured reaction products. 9Li; deduced σ(θ), quadrupole deformation parameter, B(E2). DWUCK4, FRESCO calculations, comparison with available data.
doi: 10.1016/j.physletb.2013.03.018
2013DA10 Phys.Rev.Lett. 111, 062502 (2013) V.M.Datar, D.R.Chakrabarty, S.Kumar, V.Nanal, S.Pastore, R.B.Wiringa, S.P.Behera, A.Chatterjee, D.Jenkins, C.J.Lister, E.T.Mirgule, A.Mitra, R.G.Pillay, K.Ramachandran, O.J.Roberts, P.C.Rout, A.Shrivastava, P.Sugathan Electromagnetic Transition from the 4+ to 2+ Resonance in 8Be Measured via the Radiative Capture in 4He+4He NUCLEAR REACTIONS 4He(α, γ), E=19-29 MeV; measured reaction products, Eγ, Iγ; deduced σ; calculated energy levels, proton radii, quadrupole moments, B(E2). Green Function Monte Carlo method, comparison with available data.
doi: 10.1103/PhysRevLett.111.062502
2013PA10 Phys.Rev. C 87, 035503 (2013) S.Pastore, S.C.Pieper, R.Schiavilla, R.B.Wiringa Quantum Monte Carlo calculations of electromagnetic moments and transitions in A≤9 nuclei with meson-exchange currents derived from chiral effective field theory NUCLEAR STRUCTURE 2,3H, 3He, 6,7,8,9Li, 7,9Be, 8,9B, 9C; calculated levels, J, π, isospin, nucleon radii, magnetic dipole moments, electric quadrupole moments, magnetic density, M1 and E2 transition widths and matrix elements. Greens function Monte Carlo (GFMC) calculations using realistic Argonne ν18 two-nucleon and Illinois-7 three-nucleon potentials, with inclusion of two-body meson-exchange current (MEC) operators for magnetic moments and M1 transitions. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.035503
2013WI08 Phys.Rev. C 88, 044333 (2013) R.B.Wiringa, S.Pastore, S.C.Pieper, G.A.Miller Charge-symmetry breaking forces and isospin mixing in 8Be NUCLEAR STRUCTURE 8Be; calculated levels, J, π, isospin-mixing (IM) matrix elements, isovector energy differences of mirror nuclei 8Be and 8Li; evaluated charge-symmetry breaking (CSB) components of the AV18 potential, contribution from one-photon, one-pion, one-ρ, and ρ-ω mixing. Green's function Monte Carlo (GFMC) calculations with realistic Argonne ν18 (AV18) two-nucleon and Illinois-7 three-nucleon potentials. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.044333
2012GR13 Phys.Rev. C 86, 024315 (2012) G.F.Grinyer, D.Bazin, A.Gade, J.A.Tostevin, P.Adrich, M.D.Bowen, B.A.Brown, C.M.Campbell, J.M.Cook, T.Glasmacher, S.McDaniel, A.Obertelli, K.Siwek, J.R.Terry, D.Weisshaar, R.B.Wiringa Systematic study of p-shell nuclei via single-nucleon knockout reactions NUCLEAR REACTIONS 9Be(7Li, p), (9Li, n), (10Be, p), (10Be, n), E=80 MeV/nucleon; 9Be(7Li, n), (10C, n), (10Be, n), E=120 MeV/nucleon; 9Be(9C, p), E=100 MeV/nucleon; C(9Li, n), E=80 MeV/nucleon; C(10C, n), E=120 MeV/nucleon; measured energy loss, time of flight, longitudinal-momentum distribution, nondispersive and dispersive angular plots, inclusive σ in single-nucleon knockout reactions at NSCL facility. Secondary beams of 9Be, 9Li, 10Be, 9,10C from 9Be(16O, X), E=150 MeV primary reaction. Comparison with shell-model calculations with Hartree-Fock structure inputs, and with variational Monte Carlo (VMC) calculations.
doi: 10.1103/PhysRevC.86.024315
2012KA33 Phys.Rev. C 86, 044601 (2012) Polarized proton+4, 6, 8He elastic scattering with breakup effects in the eikonal approximation NUCLEAR REACTIONS 4,6,8He(polarized p, p), E=71, 300, 500 MeV; calculated rms radii, density distribution, optical potential, σ(θ), analyzing powers. Glauber model. Pauli-blocking effect. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.044601
2012MC03 Phys.Rev. C 86, 014312 (2012) E.A.McCutchan, C.J.Lister, StevenC.Pieper, R.B.Wiringa, D.Seweryniak, J.P.Greene, P.F.Bertone, M.P.Carpenter, C.J.Chiara, G.Gurdal, C.R.Hoffman, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, S.Zhu Lifetime of the 21+ state in 10C NUCLEAR REACTIONS 1H(10B, n)10C, E=95 MeV; measured Eγ, Iγ, (10C)γ-coin, energy loss versus total energy plot, DSA, half-life of first 2+ state using Gammasphere array and FMA at ANL facility; deduced B(E2). Comparison with B(E2) value for 10Be, and with calculations using VMC and GFMC methods. NUCLEAR STRUCTURE 10Be, 10B, 10C; calculated energies of ground states and first two 2+ states, ground-state charge radii, quadrupole moments, B(E2) values. VMC and GFMC methods with AV18+IL7 interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.014312
2011BR14 Phys.Rev. C 84, 024319 (2011) I.Brida, S.C.Pieper, R.B.Wiringa Quantum Monte Carlo calculations of spectroscopic overlaps in A≤7 nuclei NUCLEAR STRUCTURE 3H, 4,6He, 7Li; calculated imaginary time evolution of spectroscopic factors. 2,3H, 3,4,6,7He, 6,7Li, 7Be; calculated binding energies, core-valence separation energies, spectroscopic factors and shell overlaps, asymptotic normalization coefficients (ANCs). Vibrational Monte Carlo (VMC), Green's function Monte Carlo (GFMC) methods. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.024319
2011EN03 Phys.Rev. C 83, 034317 (2011) J.Engel, J.Carlson, R.B.Wiringa Jastrow functions in double-β decay RADIOACTIVITY 82Se(2β-); analyzed applicability of Jastrow functions with two-body cluster approximation in calculating matrix elements for neutrinoless double β decay; comparison with unitary correlation operator method (UCOM) and Brueckner methods. Short-range correlation effects in double β decay.
doi: 10.1103/PhysRevC.83.034317
2011GR08 Phys.Rev.Lett. 106, 162502 (2011) G.F.Grinyer, D.Bazin, A.Gade, J.A.Tostevin, P.Adrich, M.D.Bowen, B.A.Brown, C.M.Campbell, J.M.Cook, T.Glasmacher, S.McDaniel, P.Navratil, A.Obertelli, S.Quaglioni, K.Siwek, J.R.Terry, D.Weisshaar, R.B.Wiringa Knockout Reactions from p-Shell Nuclei: Tests of Ab Initio Structure Models NUCLEAR REACTIONS Be(10Be, n)9Be, Be(10C, n)9C, C(10C, n)9C, E=80, 120 MeV/nucleon; measured reaction products. 10Be, 10C; deduced σ, three-body forces. Variational Monte Carlo, no core shell model ab initio calculations.
doi: 10.1103/PhysRevLett.106.162502
2011NO03 Phys.Rev. C 83, 041001 (2011) Asymptotic normalization coefficients from ab initio calculations NUCLEAR STRUCTURE 3H, 3,4He, 7,8,9Li, 7,9Be, 8B, 9C; calculated asymptotic normalization coefficients for one-nucleon removal using Monte Carlo solutions to the many-body Schrodinger equation. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.041001
2010LI49 Bull.Am.Phys.Soc. 55, MG5 (2010) C.J.Lister, E.A.McCutchan, R.B.Wiringa, S.C.Pieper, D.Seweryniak, J.P.Greene, P.F.Bertone, M.P.Carpenter, C.R.Hoffman, G.Henning, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, S.Shu, G.Gurdal, C.J.Chiara A precise determination of the 10C excited state lifetime NUCLEAR REACTIONS 1H(10B, n)10C, E=95 MeV; measured reaction products, Eγ, Iγ; deduced excited state lifetime, B(E2). Doppler Shift Attenuation Method (DSAM).
2009FL01 Phys.Rev. C 79, 034302 (2009) Enhanced effect of quark mass variation in 229Th and limits from Oklo data NUCLEAR STRUCTURE 229Th, 150Sm; calculated enhancement of effects of variation of quark mass and strong interaction parameter on the 7.6-eV transition from the first excited state in 229Th and on the 0.1 eV resonance in 150Sm from extrapolations of calculations for light nuclei. 2,3H, 3,4,5,6,7He, 6,7Li, 7,8,9Be; calculated variations of nuclear binding energies, spin-orbit intervals, nuclear radius, shifts of nuclear resonances and weakly-bound energy levels. Comparisons with data from Oklo natural reactor and estimates from Walecka model.
doi: 10.1103/PhysRevC.79.034302
2009MC02 Phys.Rev.Lett. 103, 192501 (2009) E.A.McCutchan, C.J.Lister, R.B.Wiringa, Steven C.Pieper, D.Seweryniak, J.P.Greene, M.P.Carpenter, C.J.Chiara, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, I.Stefanescu, S.Zhu Precise Electromagnetic Tests of Ab Initio Calculations of Light Nuclei: States in 10Be NUCLEAR REACTIONS 7Li(7Li, α)10Be, E=8, 10 MeV; measured Eγ, Iγ; deduced lifetime, B(E2) values for 10Be. DSAM technique, comparison with ab initio calculations.
doi: 10.1103/PhysRevLett.103.192501
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
2008KA04 Phys.Lett. B 660, 26 (2008) R.Kanungo, A.N.Andreyev, L.Buchmann, B.Davids, G.Hackman, D.Howell, P.Khalili, B.Mills, E.Padilla-Rodal, Steven C.Pieper, J.Pearson, C.Ruiz, G.Ruprecht, A.Shotter, I.Tanihata, C.Vockenhuber, P.Walden, R.B.Wiringa Spectroscopic factors for the 9Li ground state and N = 6 shell closure NUCLEAR REACTIONS 2H(9Li, t), (9Li, d), E=1.68 MeV/nucleon; measured σ(θ); deduced spectroscopic factors.
doi: 10.1016/j.physletb.2007.12.024
2008MA50 Phys.Rev. C 78, 065501 (2008) L.E.Marcucci, M.Pervin, Steven C.Pieper, R.Schiavilla, R.B.Wiringa Quantum Monte Carlo calculations of magnetic moments and M1 transitions in A ≤ 7 nuclei including meson-exchange currents NUCLEAR STRUCTURE 2H, 3H, 3He, 6Li, 7Li, 7Be; calculated magnetic moments, transition widths. Monte Carlo method.
doi: 10.1103/PhysRevC.78.065501
2008WI08 Phys.Rev. C 78, 021001 (2008) R.B.Wiringa, R.Schiavilla, Steven C.Pieper, J.Carlson Dependence of two-nucleon momentum densities on total pair momentum NUCLEAR STRUCTURE 3,4He; calculated dependence of two-nucleon momentum distributions for ground states on total pair momentum using variational Monte Carlo wave functions.
doi: 10.1103/PhysRevC.78.021001
2008WU05 Phys.Rev. C 78, 041302 (2008) A.H.Wuosmaa, J.P.Schiffer, K.E.Rehm, J.P.Greene, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, J.C.Lighthall, S.T.Marley, E.F.Moore, R.C.Pardo, N.Patel, M.Paul, D.Peterson, S.C.Pieper, G.Savard, R.E.Segel, R.H.Siemssen, X.D.Tang, R.B.Wiringa Structure of 7He by proton removal from 8Li with the (d, 3He) reaction NUCLEAR REACTIONS 2H(8Li, 3He), E=76 MeV; 2H(7Li, t), (7Li, 3He), E=81 MeV; measured charged particle spectra, (particle)(particle)-coin, angular distributions, σ, σ(θ), spectroscopic factors. 7He; deduced levels, J, π. Comparisons with data from 2H(6He, p) experiment. Comparisons with nuclear structure models and variational quantum Monte Carlo calculations.
doi: 10.1103/PhysRevC.78.041302
2007FL02 Phys.Rev. C 76, 054002 (2007) Dependence of nuclear binding on hadronic mass variation NUCLEAR STRUCTURE 2,3H, 3,4,5He, 6,7Li, 7,8Be; calculated ground-state energies, multi-nucleon energies using various Hamiltonians.
doi: 10.1103/PhysRevC.76.054002
2007NO10 Phys.Rev.Lett. 99, 022502 (2007) K.M.Nollett, S.C.Pieper, R.B.Wiringa, J.Carlson, G.M.Hale Quantum Monte Carlo Calculations of Neutron-α Scattering
doi: 10.1103/PhysRevLett.99.022502
2007PE34 Phys.Rev. C 76, 064319 (2007) M.Pervin, Steven C.Pieper, R.B.Wiringa Quantum Monte Carlo calculations of electroweak transition matrix elements in A = 6, 7 nuclei RADIOACTIVITY 6He, 7Be (β-); calculated B(GT), log(ft) values. 6,7Li, 6,7Be; calculated electromagneitc transition rates B(M1) and B(E2), transition widths. Used Greens' function Monte Carlo model.
doi: 10.1103/PhysRevC.76.064319
2007SC06 Phys.Rev.Lett. 98, 132501 (2007) R.Schiavilla, R.B.Wiringa, S.C.Pieper, J.Carlson Tensor Forces and the Ground-State Structure of Nuclei NUCLEAR STRUCTURE 3,4He, 6Li, 8Be; calculated two-nucleon momentum distributions; deduced effect of tensor forces. Variational Monte Carlo wave functions.
doi: 10.1103/PhysRevLett.98.132501
2007WU05 Eur.Phys.J. Special Topics 150, 79 (2007) A.H.Wuosmaa, K.E.Rehm, J.P.Greene, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, J.C.Lighthall, S.T.Marley, E.F.Moore, R.C.Pardo, N.Patel, M.Paul, D.Peterson, S.C.Pieper, G.Savard, J.P.Schiffer, R.E.Segal, R.H.Siemssen, S.Sinha, X.Tang, R.B.Wiringa Nucleon transfer reactions with exotic beams at ATLAS
doi: 10.1140/epjst/e2007-00271-y
2006MA94 Nucl.Phys. A777, 111 (2006) L.E.Marcucci, K.M.Nollett, R.Schiavilla, R.B.Wiringa Modern theories of low-energy astrophysical reactions NUCLEAR REACTIONS 1H(n, γ), E=1-1000 keV; calculated σ(E). 1H(n, γ), E=thermal; calculated σ. 2H(p, γ), E(cm)=0-50 keV; 3He(p, e+ν), E=low; 2H(α, γ), E(cm)=0.05-10 MeV; 3He(α, γ), E(cm)=0-2.5 MeV; 3H(α, γ), E(cm)=0-1.5 MeV; calculated astrophysical S-factor. Direct integration, correlated hyperspherical harmonics and variational Monte Carlo models with realistic two- and three-nucleon interactions. Comparison with data. RADIOACTIVITY 7Be(EC);3H(β-); calculated T1/2 and Gamow-Teller matrix elements. Comparison with data. NUCLEAR STRUCTURE 3H, 3,4He, 6,7Li, 7Be; calculated binding energies. Correlated hyperspherical harmonics, variational Monte Carlo and Green's function Monte Carlo models. Comparison with data.
doi: 10.1016/j.nuclphysa.2004.09.008
2006WI07 Phys.Rev. C 73, 034317 (2006) Pair counting, pion-exchange forces and the structure of light nuclei NUCLEAR STRUCTURE 2,3H, 4,5,6,7,8,9,10He, 6,7,8,9,10Li, 7,8,9,10Be, 7,8,10B, 8,12C; calculated levels, pair structure, one-pion-exchange forces.
doi: 10.1103/PhysRevC.73.034317
2005WU03 Phys.Rev.Lett. 94, 082502 (2005) A.H.Wuosmaa, K.E.Rehm, J.P.Greene, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, E.F.Moore, R.C.Pardo, M.Paul, D.Peterson, S.C.Pieper, G.Savard, J.P.Schiffer, R.E.Segel, S.Sinha, X.Tang, R.B.Wiringa Neutron Spectroscopic Factors in 9Li from 2H(8Li, p)9Li NUCLEAR REACTIONS 2H(8Li, p), E ≈ 76 MeV; measured Ep, excitation energy spectra, σ(θ). 9Li deduced levels, J, π, spectroscopic factors. Comparison with model predictions.
doi: 10.1103/PhysRevLett.94.082502
2005WU08 Phys.Rev. C 72, 061301 (2005) A.H.Wuosmaa, K.E.Rehm, J.P.Greene, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, E.F.Moore, R.C.Pardo, M.Paul, D.Peterson, Steven C.Pieper, G.Savard, J.P.Schiffer, R.E.Segel, S.Sinha, X.Tang, R.B.Wiringa Search for excited states in 7He with the (d, p) reaction NUCLEAR REACTIONS 2H(6He, p), E=69 MeV; 2H(7Li, p), E=81 MeV; measured particle spectra, σ(θ). 7He deduced ground-state J, π, excited state energy, width.
doi: 10.1103/PhysRevC.72.061301
2004CH65 Nucl.Phys. A746, 215c (2004) S.-Y.Chang, J.Morales, Jr., V.R.Pandharipande, D.G.Ravenhall, J.Carlson, S.C.Pieper, R.B.Wiringa, K.E.Schmidt Neutron matter: a superfluid gas
doi: 10.1016/j.nuclphysa.2004.09.119
2004PI09 Phys.Rev. C 70, 054325 (2004) S.C.Pieper, R.B.Wiringa, J.Carlson Quantum Monte Carlo calculations of excited states in A = 6-8 nuclei NUCLEAR STRUCTURE 4,6,7,8He, 6,7,8Li, 8Be; calculated ground and excited states energies. Green's function Monte Carlo approach, comparison with data.
doi: 10.1103/PhysRevC.70.054325
2003WI13 Phys.Rev. C 68, 054006 (2003) R.B.Wiringa, A.Arriaga, V.R.Pandharipande Quadratic momentum dependence in the nucleon-nucleon interaction NUCLEAR STRUCTURE 2H; calculated binding energy, radius, μ, quadrupole moment. 3H, 3,4He; calculated binding energies, role of quadratic momentum-dependent terms.
doi: 10.1103/PhysRevC.68.054006
2002PI19 Phys.Rev. C66, 044310 (2002) S.C.Pieper, K.Varga, R.B.Wiringa Quantum Monte Carlo calculations of A = 9, 10 nuclei NUCLEAR STRUCTURE 9Li, 9,10Be, 10B; calculated ground and excited states energies, radii, μ. Quantum Monte Carlo approach, comparison with data.
doi: 10.1103/PhysRevC.66.044310
2002SC18 Phys.Rev. C65, 054302 (2002) Weak Transitions in A = 6 and 7 Nuclei RADIOACTIVITY 6He(β-); 7Be(EC); calculated decay matrix elements, T1/2, branching ratios. Variational Monte Carlo wave functions, comparison with data. NUCLEAR STRUCTURE 6He, 6,7Li, 7Be; calculated binding energies, radii. Variational Monte Carlo wave functions, comparison with other models and data.
doi: 10.1103/PhysRevC.65.054302
2002VA17 Phys.Rev. C66, 034611 (2002) K.Varga, S.C.Pieper, Y.Suzuki, R.B.Wiringa Monte Carlo Integration in Glauber Model Analysis of Reactions of Halo Nuclei NUCLEAR REACTIONS 4,6He, 6Li, 12C(p, X), 4He(α, X), 12C(6He, X), (6Li, X), (12C, X), E ≈ 0.7 GeV/nucleon; calculated reaction σ. 4He(α, α), E at 5.07 GeV/c; 4,6He, 6Li(p, p), E=0.7 GeV; 12C(p, p), (α, α), (6He, 6He), (12C, 12C), E=0.8 GeV/nucleon; calculated σ(θ). Glauber model, Monte Carlo integration, comparisons with data.
doi: 10.1103/PhysRevC.66.034611
2002WI14 Phys.Rev.Lett. 89, 182501 (2002) Evolution of Nuclear Spectra with Nuclear Forces NUCLEAR STRUCTURE 4,5,6,8He, 6,7Li, 8Be, 10B; calculated levels, J, π. Comparison of several nuclear force models.
doi: 10.1103/PhysRevLett.89.182501
2002WI19 Prog.Theor.Phys.(Kyoto), Suppl. 146, 403 (2002) Quantum Monte Carlo Calculations of Light Nuclei NUCLEAR STRUCTURE 4,6,8He, 6,7,8,9Li, 8,9,10Be, 10B; calculated ground and excited states energies, J, π, configurations. Green's function Monte Carlo approach, comparison with data.
doi: 10.1143/PTPS.146.403
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
2001LE01 Phys.Rev. C63, 014006 (2001) Quantum Monte Carlo Calculations of Pion Scattering from Li NUCLEAR STRUCTURE 6,7Li; calculated transitions B(E2), transition densities. Quantum Monte-Carlo approach. NUCLEAR REACTIONS 6Li(π-, π-), (π-, π-'), E=100-240 MeV; 7Li(π+, π+'), (π-, π-'), E=164 MeV; calculated σ(θ). Quantum Monte-Carlo approach, comparisons with data.
doi: 10.1103/PhysRevC.63.014006
2001NO01 Phys.Rev. C63, 024003 (2001) K.M.Nollett, R.B.Wiringa, R.Schiavilla Six-Body Calculation of the α-Deuteron Radiative Capture Cross Section NUCLEAR REACTIONS 2H(α, γ), E < 3 MeV; calculated σ, S-factors, multipole contributions. Six-body wavefunction, variational Monte Carlo method. Astrophysical implications discussed.
doi: 10.1103/PhysRevC.63.024003
2001PI07 Phys.Rev. C64, 014001 (2001) S.C.Pieper, V.R.Pandharipande, R.B.Wiringa, J.Carlson Realistic Models of Pion-Exchange Three-Nucleon Interactions NUCLEAR STRUCTURE 7,8n, 3H, 3,4,6,7,8He, 6,7,8Li, 8Be; calculated levels, J, π, radii, μ, quadrupole moments. Pion-exchange three-nucleon interactions.
doi: 10.1103/PhysRevC.64.014001
2001PI16 Ann.Rev.Nucl.Part.Sci. 51, 53 (2001) Quantum Monte Carlo Calculations of Light Nuclei
doi: 10.1146/annurev.nucl.51.101701.132506
2000LA17 Nucl.Phys. A663-664, 377c (2000) L.Lapikas, J.Wesseling, R.B.Wiringa Correlations in the Ground-State Wave Function of 7Li NUCLEAR REACTIONS 7Li, 32S(e, e'p), E not given; measured excitation energy spectra, momentum distributions; deduced structure effects. Comparison with variational Monte Carlo and mean-field calculations.
doi: 10.1016/S0375-9474(99)00621-1
2000WI09 Phys.Rev. C62, 014001 (2000) R.B.Wiringa, S.C.Pieper, J.Carlson, V.R.Pandharipande Quantum Monte Carlo Calculations of A = 8 Nuclei NUCLEAR STRUCTURE 4,6,7,8He, 6,7,8Li, 8Be; calculated levels, J, π, density distributions. 8He, 8Li, 8Be, 8B, 8C; calculated radii, μ, quadrupole moments. Quantum Monte Carlo approach, constrained path algorithm. Comparisons with data.
doi: 10.1103/PhysRevC.62.014001
1999LA13 Phys.Rev.Lett. 82, 4404 (1999) L.Lapikas, J.Wesseling, R.B.Wiringa Nuclear Structure Studies with the 7Li(e, e'p) Reaction NUCLEAR REACTIONS 7Li(e, e'p), E=329.7, 454.7 MeV; measured σ(E, θ); deduced momentum distributions. 6He levels deduced spectroscopic factors, radii. Comparison with variational Monte Carlo calculation predictions.
doi: 10.1103/PhysRevLett.82.4404
1998SC31 Phys.Rev. C58, 1263 (1998) R.Schiavilla, V.G.J.Stoks, W.Glockle, H.Kamada, A.Nogga, J.Carlson, R.Machleidt, V.R.Pandharipande, R.B.Wiringa, A.Kievsky, S.Rosati, M.Viviani Weak Capture of Protons by Protons NUCLEAR REACTIONS 1H(p, e+ν), E not given; calculated weak capture σ, axial matrix elements.
doi: 10.1103/PhysRevC.58.1263
1998WI10 Nucl.Phys. A631, 70c (1998) Quantum Monte Carlo Calculations for Light Nuclei NUCLEAR STRUCTURE 6,7,8He, 6,7,8Li, 8Be; calculated ground, excited states properties. 2,3H, 3,4,6,8He, 6,7,8Li, 6,7,8Be, 8B, 8C; calculated proton radii. Quantum Monte Carlo methods. Comparisons with data. NUCLEAR REACTIONS 6Li(e, e), (e, e'), E not given; calculated form factors. Quantum Monte Carlo methods. Comparison with data.
doi: 10.1016/S0375-9474(98)00016-5
1998WI28 Phys.Rev.Lett. 81, 4317 (1998) Microscopic Calculation of 6Li Elastic and Transition Form Factors NUCLEAR STRUCTURE 6Li; calculated elastic, transition form factors. Variational Monte Carlo functions. Comparison with data.
doi: 10.1103/PhysRevLett.81.4317
1997PU03 Phys.Rev. C56, 1720 (1997) B.S.Pudliner, V.R.Pandharipande, J.Carlson, S.C.Pieper, R.B.Wiringa Quantum Monte Carlo Calculations of Nuclei with A ≤ 7 NUCLEAR STRUCTURE 2,3H, 4,6,7He, 6,7Li; calculated ground-state, excited level properties, charge radii, binding energies, neutron, proton densities, two-nucleon densities for some nuclei. Quantum Monte Carlo methods, two-, three-nucleon potentials.
doi: 10.1103/PhysRevC.56.1720
1996FO04 Phys.Rev. C54, 646 (1996) J.L.Forest, V.R.Pandharipande, S.C.Pieper, R.B.Wiringa, R.Schiavilla, A.Arriaga Femtometer Toroidal Structures in Nuclei NUCLEAR STRUCTURE 2H, 3,4He, 6,7Li, 16O; calculated two-nucleon density distribution; deduced shape features.
doi: 10.1103/PhysRevC.54.646
1995AR22 Phys.Rev. C52, 2362 (1995) A.Arriaga, V.R.Pandharipande, R.B.Wiringa Three-Body Correlations in Few-Body Nuclei NUCLEAR STRUCTURE 4He, 3H; calculated binding energy; deduced three-body correlations role. Variational procedure, comparison with Faddeev approach.
doi: 10.1103/PhysRevC.52.2362
1995PU05 Phys.Rev.Lett. 74, 4396 (1995) B.S.Pudliner, V.R.Pandharipande, J.Carlson, R.B.Wiringa Quantum Monte Carlo Calculations of A ≤ 6 Nuclei NUCLEAR STRUCTURE 2,3H, 6,5,3,4He, 6Li, 6Be; calculated spectra, neutron, proton radii. Quantum Monte Carlo techniques.
doi: 10.1103/PhysRevLett.74.4396
1995WI02 Phys.Rev. C51, 38 (1995) R.B.Wiringa, V.G.J.Stoks, R.Schiavilla Accurate Nucleon-Nucleon Potential with Charge-Independence Breaking NUCLEAR STRUCTURE 2H; calculated binding energy, D-state probability, μ, quadrupole moment, asymptotic properties, structure functions, tensor polarization. Nonrelativistic NN-potential, np, nn, pp scattering data analyzed.
doi: 10.1103/PhysRevC.51.38
1994PA03 Phys.Rev. C49, 789 (1994) V.R.Pandharipande, J.Carlson, S.C.Pieper, R.B.Wiringa, R.Schiavilla Isovector Spin-Longitudinal and -Transverse Response of Nuclei NUCLEAR STRUCTURE 2H, 4He, 16O; calculated two-body density, sum, energy-weighted sum of isovector spin-longitudinal, -transverse responses. Realistic interactions.
doi: 10.1103/PhysRevC.49.789
1993SC17 Phys.Rev.Lett. 70, 3856 (1993) R.Schiavilla, R.B.Wiringa, J.Carlson Coulomb Sum and Proton-Proton Correlations in Few-Body Nuclei NUCLEAR STRUCTURE 3,4He, 3H; calculated longitudinal-longitudinal distribution function.
doi: 10.1103/PhysRevLett.70.3856
1992PI17 Phys.Rev. C46, 1741 (1992) S.C.Pieper, R.B.Wiringa, V.R.Pandharipande Variational Calculation of the Ground State of 16O NUCLEAR STRUCTURE 16O; calculated binding energy, nucleon density, momentum distributions, charge form factor, longitudinal structure function. Variational calculations, Monte Carlo methods.
doi: 10.1103/PhysRevC.46.1741
1992SC12 Phys.Rev. C45, 2628 (1992) R.Schiavilla, R.B.Wiringa, V.R.Pandharipande, J.Carlson Effects of Δ-Isobar Degrees of Freedom on Low-Energy Electroweak Transitions in Few-Body Nuclei NUCLEAR STRUCTURE 3H(β-); calculated different contributions to Gamow-Teller matrix element. Variational wave functions with Δ-isobar components. NUCLEAR REACTIONS 3He(n, γ), E=thermal; calculated different contributions to the radiative capture reaction. 3He(p, e+ν), E not given; calculated weak capture reaction matrix element. Variational wave functions with Δ-isobar components.
doi: 10.1103/PhysRevC.45.2628
1992WI07 Nucl.Phys. A543, 199c (1992) Monte Carlo Calculations of Few-Body and Light Nuclei NUCLEAR STRUCTURE 3H, 4,5He, 6Li; compiled binding, breakup energy results. 16O, 40Ca; calculated binding energy. Variational Monte Carlo techniques.
doi: 10.1016/0375-9474(92)90419-K
1991CA16 Phys.Rev. C44, 619 (1991) J.Carlson, D.O.Riska, R.Schiavilla, R.B.Wiringa Weak Proton Capture Reactions on 1H and 3He and Tritium β Decay NUCLEAR REACTIONS 3He, 1H(p, e+ν), E=low; calculated weak capture σ; deduced exchange contribution role. Realistic wave function.
doi: 10.1103/PhysRevC.44.619
1991WI05 Phys.Rev. C43, 1585 (1991) Variational Calculations of Few-Body Nuclei NUCLEAR STRUCTURE 3H, 4,3He; calculated binding energies, form factors, magnetic moments. Variational Monte Carlo.
doi: 10.1103/PhysRevC.43.1585
1990CA28 Phys.Rev. C42, 830 (1990) J.Carlson, D.O.Riska, R.Schiavilla, R.B.Wiringa Radiative Neutron Capture on 3He NUCLEAR REACTIONS 3He(n, γ), E=thermal; calculated σ; deduced scattering length dependence. Monte Carlo variational methods.
doi: 10.1103/PhysRevC.42.830
1990PI02 Phys.Rev.Lett. 64, 364 (1990) S.C.Pieper, R.B.Wiringa, V.R.Pandharipande Ground State of 16O NUCLEAR STRUCTURE 16O; calculated charge density distribution, longitudinal structure function. Variational method.
doi: 10.1103/PhysRevLett.64.364
1987SC25 Nucl.Phys. A473, 267 (1987) R.Schiavilla, D.S.Lewart, V.R.Pandharipande, S.C.Pieper, R.B.Wiringa, S.Fantoni Structure Functions and Correlations in Nuclei NUCLEAR STRUCTURE 3H, 4,3He; calculated static longitudinal, structure functions. Faddeev, variational calculations.
doi: 10.1016/0375-9474(87)90145-X
1986KE07 Phys.Lett. 173B, 5 (1986) Implications of Dirac Nucleon Dynamics for the Binding of Light Nuclei NUCLEAR STRUCTURE 3H, 4He; calculated binding energy. Dirac nucleon dynamical model.
doi: 10.1016/0370-2693(86)91219-0
1986SC03 Nucl.Phys. A449, 219 (1986) R.Schiavilla, V.R.Pandharipande, R.B.Wiringa Momentum Distributions in A = 3 and 4 Nuclei NUCLEAR STRUCTURE 2,3H, 3,4He; calculated binding energy, nucleon rms radii, charge radius. 3He; calculated d+p amplitudes. 4He; calculated t+p, d+d amplitudes, nucleon momentum distributions. 3He deduced number. 4He deduced deuteron, triton number. Monte Carlo method.
doi: 10.1016/0375-9474(86)90003-5
1984CA20 Nucl.Phys. A424, 47 (1984) J.Carlson, V.R.Pandharipande, R.B.Wiringa Variational Calculations of Resonant States in 4He NUCLEAR STRUCTURE 4He; calculated resonances widths, variational calculations, realistic two-, three-nucleon interactions. NUCLEAR REACTIONS 3H(p, p), E=low; calculated 0-, 2- phase shifts. Variational calculations, realistic two-, three-nucleon interactions, modified R-matrix.
doi: 10.1016/0375-9474(84)90127-1
1984WI05 Phys.Rev. C29, 1207 (1984) R.B.Wiringa, R.A.Smith, T.L.Ainsworth Nucleon-Nucleon Potentials with and without Δ(1232) Degrees of Freedom NUCLEAR REACTIONS 1n, 1H(p, p), E ≈ 25-400 MeV; calculated phase shifts vs E. Nucleon-nucleon potentials with, without isobar degrees of freedom. NUCLEAR STRUCTURE 2H; calculated wave function, binding energy, quadrupole, magnetic moments, D-state probability. Nucleon-nucleon potentials with, without isobar degrees of freedom.
doi: 10.1103/PhysRevC.29.1207
1984WI12 Phys.Lett. 143B, 273 (1984) R.B.Wiringa, J.L.Friar, B.F.Gibson, G.L.Payne, C.R.Chen Faddeev Monte-Carlo Calculations of Trinucleon Binding Energy with Three-Body Potentials NUCLEAR STRUCTURE 3H, 3He; calculated binding energy, charge rms radii. Configuration space Faddeev wave functions, Monte Carlo integrations.
doi: 10.1016/0370-2693(84)91464-3
1983CA10 Nucl.Phys. A401, 59 (1983) J.Carlson, V.R.Pandharipande, R.B.Wiringa Three-Nucleon Interaction in 3-, 4- and Infinite-Body Systems NUCLEAR STRUCTURE 3H, 3,4He; calculated proton, neutron density distribution, charge form factors. 3H, 3He; calculated μ. Variational calculation, three-nucleon interaction.
doi: 10.1016/0375-9474(83)90336-6
1983FR20 Phys.Rev.Lett. 51, 763 (1983) B.L.Friman, V.R.Pandharipande, R.B.Wiringa Calculations of Pion Excess in Nuclei NUCLEAR STRUCTURE 2H, 3,4He, 27Al, 56Fe, 208Pb; calculated pion excess, isobar fraction. Static potential approximation, realistic Hamiltonian, variational wave functions.
doi: 10.1103/PhysRevLett.51.763
1983WI05 Nucl.Phys. A401, 86 (1983) Interplay between Two- and Three-Body Interaction in Light Nuclei and Nuclear Matter NUCLEAR STRUCTURE 3H, 3,4He; calculated rms charge radii, Coulomb energies. 3He; calculated charge form factor. New two-body potential.
doi: 10.1016/0375-9474(83)90337-8
Back to query form |