NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = J.Vary Found 198 matches. Showing 1 to 100. [Next]2023PA25 Phys.Rev. C 108, 024001 (2023) S.Pal, S.Sarker, P.J.Fasano, P.Maris, J.P.Vary, M.A.Caprio, R.A.M.Basili Magnetic moments of A = 3 nuclei obtained from chiral effective field theory operators NUCLEAR STRUCTURE 3H, 3He; calculated ground-state energies, magnetic dipole moments. Ab initio no-core shell-model (NCSM) calculations with the LENPIC (Low Energy Nuclear Physics International Collaboration) interactions. Comparison with experimental values, and with other theoretical predictions.
doi: 10.1103/PhysRevC.108.024001
2022CH55 Phys.Rev. C 106, 064312 (2022) J.Chen, B.P.Kay, T.L.Tang, I.A.Tolstukhin, C.R.Hoffman, H.Li, P.Yin, X.Zhao, P.Maris, J.P.Vary, G.Li, J.L.Lou, M.L.Avila, Y.Ayyad, S.Bennett, D.Bazin, J.A.Clark, S.J.Freeman, H.Jayatissa, C.Muller-Gatermann, A.Munoz-Ramos, D.Santiago-Gonzalez, D.K.Sharp, A.H.Wuosmaa, C.X.Yuan Probing the quadrupole transition strength of 15C via deuteron inelastic scattering NUCLEAR REACTIONS 1H(15C, p), 2H(15C, d);E=7.1 MeV/nucleon; measured reaction products, Ep, Ip, deuteron spectrum; deduced elastic and inelastic scattering σ(θ). 15C; deduced B(E2), proton quadrupole matrix element, ratio of neutron and proton matrix elements, proton deformation length, core polarization parameters, neutron effective charge; calculated levels, J, π, B(E2), magnetic dipole moments. Comparison to data on 17O and other C isotopes. Ab initio no-core configuration interaction (NCCI) calculations with Daejeon16 interaction. HELIOS spectrometer at ATLAS in-flight facility (Argonne National Laboratory).
doi: 10.1103/PhysRevC.106.064312
2022DU14 Phys.Rev. C 106, 054608 (2022) W.Du, S.Pal, M.Sharaf, P.Yin, S.Sarker, A.M.Shirokov, J.P.Vary Calculations of the np → dγ reaction in chiral effective field theory NUCLEAR REACTIONS 1H(n, dγ), E(cm)=0.000000012625, 0.0000005, 0.0005, 0.005, 0.001, 0.01 MeV; calculated scattering phase shift, σ(E) via the M1 reaction channel. Chiral effective field theory calculations employing the LENPIC (Low Energy Nuclear Physics International Collaboration) nucleon-nucleon interaction up to the fifth order (N4LO). Bayesian analysis for the error estimation. Comparison to available experimental results and other theoretical predictions. Bayaesian analysis for the error estimation.
doi: 10.1103/PhysRevC.106.054608
2022FA05 Phys.Rev. C 105, 054301 (2022) P.J.Fasano, C.Constantinou, M.A.Caprio, P.Maris, J.P.Vary Natural orbitals for the ab initio no-core configuration interaction approach NUCLEAR STRUCTURE 3,6He; calculated ground-state energy, point-proton and point-neutron rms radii, radial wave functions. Improved accuracy of the ab initio no-core configuration interaction (NCCI) calculations by implementing the basis of natural orbitals in the NCCI framework. Comparison to experimental data.
doi: 10.1103/PhysRevC.105.054301
2022MA63 Phys.Rev. C 106, 064002 (2022) P.Maris, R.Roth, E.Epelbaum, R.J.Furnstahl, J.Golak, K.Hebeler, T.Huther, H.Kamada, H.Krebs, H.Le, Ulf-G.Meissner, J.A.Melendez, A.Nogga, P.Reinert, R.Skibinski, J.P.Vary, H.Witala, T.Wolfgruber Nuclear properties with semilocal momentum-space regularized chiral interactions beyond N2LO NUCLEAR STRUCTURE 14,16,18,20,22,24,26O, 40,48Ca; calculated ground-state energies, point-proton radii. 4,6,8He, 6Li, 10Be, 10,12B, 12C; calculated ground state energies. 10,12B, 12C; calculated low-lying levels, J, π. Chiral EFT calculations with semilocal momentum-space regularized NN potentials up to fourth leading order N4LO. NUCLEAR REACTIONS 2H(n, X), E=70, 135, 200 MeV; calculated σ(E), σ(θ), vector- and tensor analyzing power. Comparison to experimental data.
doi: 10.1103/PhysRevC.106.064002
2022MA64 Phys.Rev. C 106, 064320 (2022) I.A.Mazur, I.J.Shin, Y.Kim, A.I.Mazur, A.M.Shirokov, P.Maris, J.P.Vary SS-HORSE extension of the no-core shell model: Application to resonances in 7He NUCLEAR STRUCTURE 7He; calculated resonances width and energy, J, π, phase shifts in the n+6He and in n+6He* channels. SS-HORSE extension of the ab initio no-core shell model (NCSM) with the realistic Daejeon16 and JISP16 NN interactions. Comparison to other theoretical results and available experimental data.
doi: 10.1103/PhysRevC.106.064320
2022MA71 Phys.Atomic Nuclei 85, 823 (2022) I.A.Mazur, A.I.Mazur, V.A.Kulikov, A.M.Shirokov, I.J.Shin, Y.Kim, P.Maris, J.P.Vary Bound and Resonant States of the 9Li Nucleus with Daejeon16 Nucleon-Nucleon Interaction NUCLEAR STRUCTURE 9Li; calculated the energies of bound states, the respective asymptotic normalization coefficients, the energies and widths of its resonance states by the SS-HORSE method on the basis of ab initio calculations within no-core shell model with Daejeon16 nucleon-nucleon interaction.
doi: 10.1134/S1063778823010349
2022YI05 J.Phys.(London) G49, 125102 (2022) P.Yin, W.Du, W.Zuo, X.Zhao, J.P.Vary Sub Coulomb barrier d+208Pb scattering in the time-dependent basis function approach NUCLEAR REACTIONS 208Pb(d, d), E=3-7 MeV; calculated σ using the non-perturbative time-dependent basis function (tBF) approach; deduced the higher-order inelastic scattering effects are noticeable for sub barrier scatterings with the tBF method.
doi: 10.1088/1361-6471/ac79c3
2021AB10 Phys.Rev. C 104, 054315 (2021) T.Abe, P.Maris, T.Otsuka, N.Shimizu, Y.Utsuno, J.P.Vary Ground-state properties of light 4n self-conjugate nuclei in ab initio no-core Monte Carlo shell model calculations with nonlocal NN interactions NUCLEAR STRUCTURE 4He, 8Be, 12C, 16O, 20Ne; calculated ground-state energies and point-proton rms radii using ab initio no-core Monte Carlo shell model (MCSM), with the JISP16 and Daejeon16 nonlocal nucleon-nucleon interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.104.054315
2021MA32 Phys.Rev. C 103, 054001 (2021) P.Maris, E.Epelbaum, R.J.Furnstahl, J.Golak, K.Hebeler, T.Huther, H.Kamada, H.Krebs, Ulf-G.Meissner, J.A.Melendez, A.Nogga, P.Reinert, R.Roth, R.Skibinski, V.Soloviov, K.Topolnicki, J.P.Vary, Yu.Volkotrub, H.Witala, T.Wolfgruber, for the LENPIC Collaboration Light nuclei with semilocal momentum-space regularized chiral interactions up to third order NUCLEAR STRUCTURE 3H, 3,4,6,8He, 6,7,8,9Li, 8,10Be, 10,11,12,13B, 12,13,14C, 14,15N, 16O; calculated energies of ground and excited states, S(2n) for 6He and 6Li, α+d breakup up for 6Li, and 3α breakup for 12C, energies, wave functions and radii for 3H, 3,4He. Semilocal momentum-space (SMS) regularized two- and three-nucleon forces up to third chiral order (N2LO), with the two low-energy constants entering the three-body force determined from the triton binding energy and the differential cross-section minimum in elastic nucleon-deuteron scattering. Comparison with experimental data. NUCLEAR REACTIONS 1H(polarized d, d), E=70, 140, 200, 270 MeV; 2H(p, d), (polarized p, d), E=65 MeV; calculated analyzing powers Ay(θ) and differential cross sections for elastic scattering using semilocal momentum-space (SMS) regularized two- and three-nucleon forces up to third chiral order (N2LO) three-nucleon force (3NF). Comparison with experimental data.
doi: 10.1103/PhysRevC.103.054001
2021PA26 J.Phys.(London) G48, 085105 (2021) P.Papakonstantinou, J.P.Vary, Y.Kim Daejeon 16 interaction with contact-term corrections for heavy nuclear systems NUCLEAR STRUCTURE 16,28O, 40,48,60Ca, 90Zr, 100,132Sn, 208Pb; calculated ground-state energy and point-proton rms radii, electric dipole polarizability in many-body approaches based on the mean-field approximation.
doi: 10.1088/1361-6471/ac0b30
2020BA33 Phys.Rev. C 102, 014302 (2020) R.A.M.Basili, J.M.Yao, J.Engel, H.Hergert, M.Lockner, P.Maris, J.P.Vary Benchmark neutrinoless double-β decay matrix elements in a light nucleus RADIOACTIVITY 6He(2β-); calculated nuclear radius, ground state binding energy, and neutrinoless double β-decay (0νββ) nuclear matrix elements (NMEs) using the no-core shell model (NCSM), and the multireference in-medium similarity renormalization group (MR-IMSRG).
doi: 10.1103/PhysRevC.102.014302
2020CA14 Eur.Phys.J. A 56, 120 (2020) M.A.Caprio, P.J.Fasano, P.Maris, A.E.McCoy, J.P.Vary Probing ab initio emergence of nuclear rotation
doi: 10.1140/epja/s10050-020-00112-0
2020DU04 Phys.Rev. C 101, 035202 (2020) W.Du, Y.Li, X.Zhao, G.A.Miller, J.P.Vary Basis light-front quantization for a chiral nucleon-pion Lagrangian
doi: 10.1103/PhysRevC.101.035202
2020QI02 Phys.Rev. C 102, 055207 (2020) Light mesons within the basis light-front quantization framework
doi: 10.1103/PhysRevC.102.055207
2020SA30 Phys.Rev. C 102, 024324 (2020) M.Sanchez Sanchez, N.A.Smirnova, A.M.Shirokov, P.Maris, J.P.Vary Improved description of light nuclei through chiral effective field theory at leading order NUCLEAR STRUCTURE 3H, 4,6He; calculated ground-state energies and point-proton rms radii using chiral effective field theory at leading order with LENPIC and modified LENPIC interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.102.024324
2019AD05 Phys.Rev. C 99, 035208 (2019) L.Adhikari, Y.Li, M.Li, J.P.Vary Form factors and generalized parton distributions of heavy quarkonia in basis light front quantization
doi: 10.1103/PhysRevC.99.035208
2019CH36 Phys.Rev. C 100, 025208 (2019) G.Chen, Y.Li, K.Tuchin, J.P.Vary Heavy quarkonia production at energies available at the CERN Large Hadron Collider and future electron-ion colliding facilities using basis light-front quantization wave functions
doi: 10.1103/PhysRevC.100.025208
2019EP01 Phys.Rev. C 99, 024313 (2019) E.Epelbaum, J.Golak, K.Hebeler, T.Huther, H.Kamada, H.Krebs, P.Maris, Ulf-G.Meissner, A.Nogga, R.Roth, R.Skibinski, K.Topolnicki, J.P.Vary, K.Vobig, H.Witala, for the LENPIC Collaboration Few- and many-nucleon systems with semilocal coordinate-space regularized chiral two- and three-body forces NUCLEAR REACTIONS 2H(n, n), E=14.1, 70, 108, 135, 250 MeV; analyzed differential σ(θ); deduced low energy coefficients; calculated differential σ(θ), neutron analyzing powers Ay(θ), and deuteron vector and tensor analyzing powers using chiral effective field theory with semilocal coordinate-space regularized two- and three-nucleon forces. Comparison with experimental data. NUCLEAR STRUCTURE 4,6,8He, 6,7,8,9Li, 8,9,10Be, 10,11,12B, 12C, 16O; calculated ground state binding energies, and excitation energies using chiral N2LO interactions.
doi: 10.1103/PhysRevC.99.024313
2019JI03 Phys.Rev. C 99, 035206 (2019) Basis light front quantization for the charged light mesons with color singlet Nambu--Jona-Lasinio interactions
doi: 10.1103/PhysRevC.99.035206
2019MA76 Physics of Part.and Nuclei 50, 537 (2019) I.A.Mazur, A.M.Shirokov, A.I.Mazur, I.J.Shin, Y.Kim, P.Maris, J.P.Vary Description of Continuum Spectrum States of Light Nuclei in the Shell Model
doi: 10.1134/s1063779619050186
2019NE03 Phys.Rev. C 99, 054308 (2019) G.A.Negoita, J.P.Vary, G.R.Luecke, P.Maris, A.M.Shirokov, I.Shin, Y.Kim, Es.G.Ng, C.Yang, M.Lockner, G.M.Prabhu Deep learning: Extrapolation tool for ab initio nuclear theory NUCLEAR STRUCTURE 6Li; calculated ground state energy, and ground state proton rms radius using ab initio no-core shell model (NCSM) results, and with artificial neural network (ANN) extrapolation method. Comparison with other extrapolation methods and experimental data.
doi: 10.1103/PhysRevC.99.054308
2019SM04 Phys.Rev. C 100, 054329 (2019) N.A.Smirnova, B.R.Barrett, Y.Kim, I.J.Shin, A.M.Shirokov, E.Dikmen, P.Maris, J.P.Vary Effective interactions in the sd shell NUCLEAR STRUCTURE 18,19,21,23,25,26,27F, 21,22,23,24O, 22Na, 24Mg, 28,29Si, 32S, 39K; calculated levels, J, π, effective single-particle energies (ESPEs), B(E2) and Q(first 2+) for 24Mg, 28Si, 32S. 16,17,18,19,20,21,22,23,24,25,26,27,28O; calculated ground state energies relative to that of 16O, sub-shell gap and neutron spin-orbit splitting for even-A nuclei. No-core shell-model calculations with Okubo-Lee-Suzuki transformation, and microscopic effective shell-model interactions in the valence sd shell, obtained from chiral N3LO, JISP16, and Daejeon16 nucleon-nucleon potentials. Comparison with experimental data. Discussed possible role of the three-nucleon forces.
doi: 10.1103/PhysRevC.100.054329
2018BI08 Phys.Rev. C 98, 014002 (2018) S.Binder, A.Calci, E.Epelbaum, R.J.Furnstahl, J.Golak, K.Hebeler, T.Huther, H.Kamada, H.Krebs, P.Maris, Ulf-G.Meissner, A.Nogga, R.Roth, R.Skibinski, K.Topolnicki, J.P.Vary, K.Vobig, H.Witala, at the LENPIC Collaboration Few-nucleon and many-nucleon systems with semilocal coordinate-space regularized chiral nucleon-nucleon forces NUCLEAR REACTIONS 2H(n, n), E=5, 10, 14.1 MeV; 2H(n, 2np), E=13, 65 MeV; calculated differential σ(θ), Ay analyzing powers, nucleon and deuteron vector analyzing powers, phase shifts, polarization-transfer coefficient, breakup cross sections, and pd analyzing powers. NUCLEAR STRUCTURE 3H, 3,4He, 6Li; calculated binding energies, ground-state energies of 4He and 6Li, proton rms radii. 3H, 4,6,8He, 6,7,8,9Li, 8,9Be, 10B, 16,24O, 40,48Ca; calculated ground state energies. 3H, 3He, 6,7,8,9Li, 7,9Be, 8,9,10B, 9C; calculated magnetic dipole moments. 16,24O, 40,48Ca; calculated charge radii. Faddeev-Yakubovsky equations, with no-core configuration interaction approach, coupled-cluster (CC) theory, and in-medium similarity renormalization group (IM-SRG)methods with SCS chiral nucleon-nucleon (NN) potentials. Comparison with experimental values, and with other theoretical predictions.
doi: 10.1103/PhysRevC.98.014002
2018DU05 Phys.Rev. C 97, 064620 (2018) W.Du, P.Yin, Y.Li, G.Chen, W.Zuo, X.Zhao, J.P.Vary Coulomb excitation of the deuteron in peripheral collisions with a heavy ion NUCLEAR REACTIONS U(d, d'), E=4.7, 19.4, 85.5 MeV/nucleon; calculated low and intermediate energy Coulomb excitations of uranium, internal charge distributions of 2H target before, during and after scattering, rms charge radii, rms momentum and rms orbital angular momentum, intrinsic energy of 2H during scattering using ab-initio nonperturbative, time-dependent basis function (tBF) method with JISP16 nucleon-nucleon interaction. Discussed excitation mechanism and dynamics.
doi: 10.1103/PhysRevC.97.064620
2018SH33 Phys.Rev. C 98, 044624 (2018) A.M.Shirokov, A.I.Mazur, I.A.Mazur, E.A.Mazur, I.J.Shin, Y.Kim, L.D.Blokhintsev, J.P.Vary Nucleon-α scattering and resonances in 5He and 5Li with JISP16 and Daejeon16 NN interactions NUCLEAR REACTIONS 4He(p, X)5Li, E*=0-15 MeV; 4He(n, X)5He, E*=0-17 MeV; calculated eigenenergies, widths, and phase shifts of resonances in pα and nα scattering in non-resonant and resonant 3/2- and 1/2- states using extension of the ab initio no-core shell model single state harmonic oscillator representation of scattering equations (NCSM-SS-HORSE) with JISP16 and Daejeon16 nucleon-nucleon interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.98.044624
2018SK01 Phys.Rev. C 97, 014002 (2018) R.Skibinski, J.Golak, K.Topolnicki, H.Witala, Yu.Volkotrub, H.Kamada, A.M.Shirokov, R.Okamoto, K.Suzuki, J.P.Vary Nucleon-deuteron scattering with the JISP16 potential NUCLEAR REACTIONS 2H(polarized p, p), (polarized n, n), (n, p), (polarized p, 2p), 1H(polarized d, d), E=5, 13, 65, 135 MeV; calculated differential elastic σ(θ), deuteron vector and tensor analyzing powers iT11, T22, differential cross section for deuteron breakup process. Nucleon-nucleon J-matrix inverse scattering potential JISP16 for elastic nucleon-deuteron scattering and the deuteron breakup process using the formalism of Faddeev equations. Comparison with experimental data, and with theoretical calculations using CD Bonn, Argonne AV18, and the chiral forces. NUCLEAR STRUCTURE 2H; calculated ground state energies, 3S1 and 3D1 state probabilities for deuteron, potential and kinetic energies for various NN interactions. 3H; calculated binding energy, potential and kinetic energies for various NN interactions.
doi: 10.1103/PhysRevC.97.014002
2018VA18 Phys.Rev. C 98, 065502 (2018) J.P.Vary, R.Basili, W.Du, M.Lockner, P.Maris, S.Pal, S.Sarker Effective operators in two-nucleon systems
doi: 10.1103/PhysRevC.98.065502
2017HE02 Phys.Rev. C 95, 014306 (2017) Ab initio no-core properties of 7Li and 7Be with the JISP16 and chiral NNLOopt interactions NUCLEAR STRUCTURE 7Li, 7Be; calculated energies of the ground states, and four lowest excited states of negative parity, point proton rms radius, magnetic dipole and electric quadrupole moment of the ground state, B(E2), B(M1), spin decompositions and total magnetic moments. The ab initio no-core full configuration (NCFC) approach with JISP16 and chiral NNLOopt nucleon-nucleon interactions. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.014306
2017MA50 Physics of Part.and Nuclei 48, 84 (2017) I.A.Mazur, A.M.Shirokov, A.I.Mazur, J.P.Vary Description of resonant states in the shell model NUCLEAR STRUCTURE 5He, 5Li; calculated (3/2)-, (1/2)-, (1/2)+ resonance states energy, width using ab initio NCSM (No-Core Shell Model). NUCLEAR REACTIONS 4He(n, n'), E=0-42 MeV; calculated phase shift, the lowest eigenenergy in 5He using NCSM, SS HORSE (Single-State Harmonic Oscillator Representation of Scattering Equations) formalism. Compared to data.
doi: 10.1134/S1063779617010142
2017SH14 J.Phys.(London) G44, 075103 (2017) I.J.Shin, Y.Kim, P.Maris, J.P.Vary, C.Forssen, J.Rotureau, N.Michel Ab initio no-core solutions for 6Li NUCLEAR STRUCTURE 6Li; calculated energy levels, rms radii, quadrupole moments, ground state energy, magnetic dipole moment, B(E2), B(M1), Gamow-Teller matrix elements. Ab initio NCFC approach, comparison with experimental values.
doi: 10.1088/1361-6471/aa6cb7
2016AD25 Phys.Rev. C 93, 055202 (2016) L.Adhikari, Y.Li, X.Zhao, P.Maris, J.P.Vary, A.Abd El-Hady Form factors and generalized parton distributions in basis light-front quantization
doi: 10.1103/PhysRevC.93.055202
2016BI06 Phys.Rev. C 93, 044002 (2016) S.Binder, A.Calci, E.Epelbaum, R.J.Furnstahl, J.Golak, K.Hebeler, H.Kamada, H.Krebs, J.Langhammer, S.Liebig, P.Maris, Ulf-G.Meissner, D.Minossi, A.Nogga, H.Potter, R.Roth, R.Skibinski, K.Topolnicki, J.P.Vary, H.Witala, for the LENPIC Collaboration Few-nucleon systems with state-of-the-art chiral nucleon-nucleon forces NUCLEAR STRUCTURE 3H, 4He, 6Li; calculated energies of ground-state and lowest two states, point-proton radius using improved NN chiral potentials LO, NLO, N2LO, N3LO and N4LO. Comparison with experimental data. NUCLEAR REACTIONS 3H, 4He, 6Li(d, X), (polarized d, d), E=10, 70, 135, 200 MeV; total σ(E), differential cross section and tensor analyzing powers for elastic scattering based on NN chiral potentials LO, NLO, N2LO, N3LO and N4LO. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.044002
2016HU11 Phys.Rev. C 94, 014303 (2016) B.S.Hu, F.R.Xu, Z.H.Sun, J.P.Vary, T.Li Ab initio nuclear many-body perturbation calculations in the Hartree-Fock basis NUCLEAR STRUCTURE 4He, 16O; calculated binding energies and point-proton rms radii using ab initio many-body perturbation theory (MBPT), with realistic nuclear forces, chiral N3LO and JISP16. Comparison with experimental data.
doi: 10.1103/PhysRevC.94.014303
2016SH35 Phys.Rev.Lett. 117, 182502 (2016) A.M.Shirokov, G.Papadimitriou, A.I.Mazur, I.A.Mazur, R.Roth, J.P.Vary Prediction for a Four-Neutron Resonance NUCLEAR REACTIONS 4He(8He, 8Be), E<30 MeV; calculated scattering phase shifts, tetraneutron ground state energy, resonance parameters. ab initio approach using the JISP16 realistic NN interaction.
doi: 10.1103/PhysRevLett.117.182502
2016SH44 Phys.Rev. C 94, 064320 (2016); Erratum Phys.Rev. C 98, 039901 (2018) A.M.Shirokov, A.I.Mazur, I.A.Mazur, J.P.Vary Shell model states in the continuum NUCLEAR STRUCTURE 5He; calculated resonance energies and widths for the first 3/2- and 1/2- states using no-core shell model (NCSM). NUCLEAR REACTIONS 4He(n, n'), E(cm)=0-20 MeV; calculated phase shifts and S-matrix poles for 3/2-, 1/2- and 1/2+ scattering using single state harmonic oscillator representation of scattering equations (SS-HORSE) approach.
doi: 10.1103/PhysRevC.94.064320
2015CA08 Rom.J.Phys. 60, 738 (2015) M.A.Caprio, P.Maris, J.P.Vary, R.Smith Emergence of Rotational Collectivity in Ab Initio no-Core Configuration Interaction Calculations NUCLEAR STRUCTURE 7,8,9,10,11,12Be; calculated band energy parameters. ab initio no-core configuration interaction (NCCI).
2015CA22 Int.J.Mod.Phys. E24, 1541002 (2015) M.A.Caprio, P.Maris, J.P.Vary, R.Smith Collective rotation from ab initio theory NUCLEAR STRUCTURE 7,8,9Be; calculated electric quadrupole transition strengths, level energies, quadrupole and dipole matrix element observables, natural parity yrast, band energy parameters. Comparison with available data.
doi: 10.1142/S0218301315410025
2015DI05 Phys.Rev. C 91, 064301 (2015) E.Dikmen, A.F.Lisetskiy, B.R.Barrett, P.Maris, A.M.Shirokov, J.P.Vary Ab initio effective interactions for sd-shell valence nucleons NUCLEAR STRUCTURE 18,19F; calculated ground-state energies and energy levels, J, π using a double Okubo-Lee-Suzuki transformation within the ab initio no core shell model approach to generate microscopically the input for standard shell model calculations in the sd-shell, e.g. core and single-particle energies and two-body effective shell-model interactions. Comparison with exact no core shell model results yields good agreement.
doi: 10.1103/PhysRevC.91.064301
2015DY01 Phys.Rev. C 91, 024326 (2015) T.Dytrych, A.C.Hayes, K.D.Launey, J.P.Draayer, P.Maris, J.P.Vary, D.Langr, T.Oberhuber Electron-scattering form factors for 6Li in the ab initio symmetry-guided framework NUCLEAR REACTIONS 6Li(e, e'), E not given; calculated longitudinal C0 form factors using ab initio symmetry-adapted no-core shell-model description (SA-NCSM) for the bare JISP16 and NNLOopt NN interactions, and for several SU(3)-selected spaces. Comparison with available experimental data.
doi: 10.1103/PhysRevC.91.024326
2015MA03 Phys.Rev. C 91, 014310 (2015); Erratum Phys.Rev. C 99, 029902 (2019) Emergence of rotational bands in ab initio no-core configuration interaction calculations of the Be isotopes NUCLEAR STRUCTURE 7,8,9,10,11,12Be; calculated levels, J, π, rotational bands, magnetic dipole and electric quadrupole moments, B(M1), B(E2), natural and unnatural parity yrast bands, rotational band parameters. The ab initio no-core configuration interaction (NCCI) calculation with realistic interactions. Comparison with available experimental results.
doi: 10.1103/PhysRevC.91.014310
2015NA20 Phys.Rev. C 92, 064003 (2015) R.Navarro-Perez, J.E.Amaro, E.Ruiz Arriola, P.Maris, J.P.Vary Statistical error propagation in ab initio no-core full configuration calculations of light nuclei NUCLEAR STRUCTURE 3H, 4He; calculated binding energies using ab initio no-core full configuration (NCFC) model with Gauss-one-pion exchange (OPE) potential, and by using realistic statistical uncertainty from experimental NN scattering data extracted by Monte Carlo techniques.
doi: 10.1103/PhysRevC.92.064003
2015PA08 Phys.Rev. C 91, 021001 (2015) Nucleon-nucleon scattering with the complex scaling method and realistic interactions
doi: 10.1103/PhysRevC.91.021001
2014CA30 Phys.Rev. C 90, 034305 (2014) Halo nuclei 6He and 8He with the Coulomb-Sturmian basis NUCLEAR STRUCTURE 4,6,8He; calculated ground-state energies, proton and matter rms radii for neutron halo nuclei 6,8He and the baseline 4He nucleus. Harmonic oscillator and Coulomb-Sturmian radial functions for ab initio no-core configuration interaction (NCCI) calculations with JISP16 nucleon-nucleon interaction. Comparison with available experimental results.
doi: 10.1103/PhysRevC.90.034305
2014GO30 Eur.Phys.J. A 50, 177 (2014) J.Golak, R.Skibinski, K.Topolnicki, H.Witala, E.Epelbaum, H.Krebs, H.Kamada, Ulf-G.Meissner, V.Bernard, P.Maris, J.Vary, S.Binder, A.Calci, K.Hebeler, J.Langhammer, R.Roth, A.Nogga, S.Liebig, D.Minossi Low-energy neutron-deuteron reactions with N3LO chiral forces NUCLEAR REACTIONS 2H(n, n), E=6.5, 10 MeV; calculated analyzing power. 2H(n, x), E=13.0 MeV; calculated σ(θ). Three-nucleon Faddeev equations with different N3LO chiral forces. Compared to data.
doi: 10.1140/epja/i2014-14177-7
2014KI07 Int.J.Mod.Phys. E23, 1461004 (2014) Y.Kim, I.J.Shin, P.Maris, J.P.Vary, C.Forssen, J.Rotureau Ab initio no core full configuration approach for light nuclei
doi: 10.1142/S0218301314610047
2014MA47 Phys.Rev. C 90, 014314 (2014) P.Maris, J.P.Vary, A.Calci, J.Langhammer, S.Binder, R.Roth 12C properties with evolved chiral three-nucleon interactions NUCLEAR STRUCTURE 12C; calculated levels, J, π, point-proton rms radii, quadrupole moments, B(E2), B(M1) using ab initio no-core shell model (NCSM), important truncated no-core shell model (IT-NCSM) methods with similarity renormalization group (SRG) involved chiral NN + 3N Hamiltonians. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.014314
2014SH22 Phys.Rev. C 90, 024324 (2014) A.M.Shirokov, A.G.Negoita, J.P.Vary, S.K.Bogner, A.I.Mazur, E.A.Mazur, D.Gogny Properties of nuclear matter within the JISP16 NN interaction
doi: 10.1103/PhysRevC.90.024324
2013BA02 Prog.Part.Nucl.Phys. 69, 131 (2013) B.R.Barrett, P.Navratil, J.P.Vary Ab initio no core shell model
doi: 10.1016/j.ppnp.2012.10.003
2013BO19 Comput.Phys.Commun. 184, 085101 (2013) S.Bogner, A.Bulgac, J.Carlson, J.Engel, G.Fann, R.J.Furnstahl, S.Gandolfi, G.Hagen, M.Horoi, C.Johnson, M.Kortelainen, E.Lusk, P.Maris, H.Nam, P.Navratil, W.Nazarewicz, E.Ng, G.P.A.Nobre, E.Ormand, T.Papenbrock, J.Pei, S.C.Pieper, S.Quaglioni, K.J.Roche, J.Sarich, N.Schunck, M.Sosonkina, J.Terasaki, I.Thompson, J.P.Vary, S.M.Wild Computational nuclear quantum many-body problem: The UNEDF project NUCLEAR REACTIONS 3He(d, p), 7Be(p, γ), E<1MeV; 172Yb, 188Os, 238U(γ, X), E<24 MeV; calculated σ. Comparison with experimental data. NUCLEAR STRUCTURE 100Zr; calculated quadrupole deformation parameter, radii, neutron separation energy.
doi: 10.1016/j.cpc.2013.05.020
2013DY04 Phys.Rev.Lett. 111, 252501 (2013) ` T.Dytrych, K.D.Launey, J.P.Draayer, P.Maris, J.P.Vary, E.Saule, U.Catalyurek, M.Sosonkina, D.Langr, M.A.Caprio Collective Modes in Light Nuclei from First Principles NUCLEAR STRUCTURE 6Li, 6He, 8Be; calculated B(E2), magnetic dipole moments, rms matter radii. ab initio analyses, comparison with available data.
doi: 10.1103/PhysRevLett.111.252501
2013JU01 Phys.Rev. C 87, 054312 (2013) E.D.Jurgenson, P.Maris, R.J.Furnstahl, P.Navratil, W.E.Ormand, J.P.Vary Structure of p-shell nuclei using three-nucleon interactions evolved with the similarity renormalization group NUCLEAR STRUCTURE 3H, 4He, 7Li, 8Be, 10B, 12C; calculated ground-state and low-lying levels, J, π. 7Li, 7Be, 10B; calculated magnetic dipole moments of ground states and low-lying states. No-core full configuration (NCFC) and similarity renormalization group (SRG) ab initio calculations for p-shell nuclei. Assessment of convergence properties, extrapolation techniques, and dependence of energies, including four-body contributions. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.054312
2013MA05 Phys.Rev. C 87, 014327 (2013) Structure of A=7-8 nuclei with two- plus three-nucleon interactions from chiral effective field theory NUCLEAR STRUCTURE 7,8Li, 7,8Be, 8B; calculated ground-state energies, levels, J, π, point-proton rms radii, electric quadrupole and magnetic dipole moments, B(M1), B(E2) using the ab initio no-core shell model (NCSM), with chiral effective field theory (EFT) for two- and three-nucleon interactions. Okubo-Lee-Suzuki renormalization. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.014327
2013MA38 Phys.Rev. C 87, 054318 (2013) P.Maris, J.P.Vary, S.Gandolfi, J.Carlson, S.C.Pieper Properties of trapped neutrons interacting with realistic nuclear Hamiltonians
doi: 10.1103/PhysRevC.87.054318
2013MA60 Int.J.Mod.Phys. E22, 1330016 (2013) ab initio nuclear structure calculations of p-shell nuclei with JISP16 NUCLEAR STRUCTURE 6,8He, 6,7,8,9Li, 7,8,9,11,12Be, 8,9,10,11,12,13B, 9,11,12,13,14C, 12,13,14,15N, 13,15,16O; calculated binding energies, excitation energies, J, π, magnetic moments, proton and neutron rms radii, quadrupole moments. ab initio No-Core Full Configuration (NCFC) approach, comparison with available data.
doi: 10.1142/S0218301313300166
2012AB14 Phys.Rev. C 86, 054301 (2012) T.Abe, P.Maris, T.Otsuka, N.Shimizu, Y.Utsuno, J.P.Vary Benchmarks of the full configuration interaction, Monte Carlo shell model, and no-core full configuration methods NUCLEAR STRUCTURE 4,6He, 6,7Li, 8Be, 10B, 12C, 16O; calculated levels, point-particle rms radii, electromagnetic moments using the full configuration interaction (FCI), Monte Carlo shell model (MCSM), and no core full configuration (NCFC) approaches using realistic JISP16 nucleon-nucleon interaction.
doi: 10.1103/PhysRevC.86.054301
2012CA29 Phys.Rev. C 86, 034312 (2012) Coulomb-Sturmian basis for the nuclear many-body problem NUCLEAR STRUCTURE 6Li; calculated levels, J, π, RMS radius using the no-core configuration interaction (NCCI) model and Coulomb-Sturmian basis functions. Comparison with calculations using harmonic-oscillator basis.
doi: 10.1103/PhysRevC.86.034312
2012CO18 Phys.Rev. C 86, 034325 (2012) Lithium isotopes within the ab initio no-core full configuration approach NUCLEAR STRUCTURE 6,7,8Li; calculated levels, J, π, RMS point-proton radius, angle-averaged densities, density contours, B(E2), B(M1), magnetic dipole and electric quadrupole moments using no-core full configuration calculations with JISP16 interaction.
doi: 10.1103/PhysRevC.86.034325
2012CO20 Phys.Rev. C 86, 054002 (2012) S.A.Coon, M.I.Avetian, M.K.G.Kruse, U.van Kolck, P.Maris, J.P.Vary Convergence properties of ab initio calculations of light nuclei in a harmonic oscillator basis NUCLEAR STRUCTURE 2,3H, 4,6He; calculated ground-state energy of light nuclei as function of momentum using shell model with the bare and soft NN interactions Idaho N3LO and JISP16.
doi: 10.1103/PhysRevC.86.054002
2012SH09 Phys.Rev. C 85, 034004 (2012) A.M.Shirokov, V.A.Kulikov, A.I.Mazur, J.P.Vary, P.Maris Deuteron-equivalent and phase-equivalent interactions within light nuclei NUCLEAR STRUCTURE 3H, 4He; calculated binding energies, Tjon line. No-core shell model (NCSM), no-core full configuration (NCFC) approach. Comparison with experimental data. NUCLEAR REACTIONS 1H(n, n), E=10 MeV; calculated scattering wave functions. Deuteron-equivalent phase-equivalent transformations (DET-PET). JISP16-NN interaction.
doi: 10.1103/PhysRevC.85.034004
2012SH16 Bull.Rus.Acad.Sci.Phys. 76, 496 (2012); Izv.Akad.Nauk RAS, Ser.Fiz 76, 554 (2012) A.M.Shirokov, V.A.Kulikov, A.I.Mazur, J.P.Vary, P.Maris Phase-equivalent transformation which does not affect bound state properties and its manifestation in many-body systems NUCLEAR STRUCTURE 3H, 4He; calculated correlation of binding energies, Tjon lines, scattering wave functions. DET-PET transformations, comparison with available data.
doi: 10.3103/S1062873812040326
2011BA53 J.Phys.:Conf.Ser. 312, 092016 (2011) B.Barrett, M.Kruse, A.Lisetskiy, P.Navratil, I.Stetcu, J.Vary Ab initio shell model with a core: Extending the No Core Shell Model to heavier nuclei NUCLEAR STRUCTURE 7Li; calculated ground state energy. 8,9,10He; calculated levels, J, π. 6Li; calculated quadrupole moment. SSM (standard shell model), NCSM (No Core Shell Model).
doi: 10.1088/1742-6596/312/9/092016
2011BO22 Phys.Rev. C 84, 044306 (2011) S.K.Bogner, R.J.Furnstahl, H.Hergert, M.Kortelainen, P.Maris, M.Stoitsov, J.P.Vary Testing the density matrix expansion against ab initio calculations of trapped neutron drops
doi: 10.1103/PhysRevC.84.044306
2011MA35 Phys.Rev.Lett. 106, 202502 (2011) P.Maris, J.P.Vary, P.Navratil, W.E.Ormand, H.Nam, D.J.Dean Origin of the Anomalous Long Lifetime of 14C NUCLEAR STRUCTURE 14C, 14N; calculated rms radii, quadrupole moment, dipole moment, B(M1), β-decay matrix elements. deduced long lifetime for 14C. Ab initio no-core shell model calculations.
doi: 10.1103/PhysRevLett.106.202502
2011PI09 Phys.Rev. C 84, 015201 (2011) Boundary between hadron and quark-gluon structure of nuclei
doi: 10.1103/PhysRevC.84.015201
2011SH21 Bull.Rus.Acad.Sci.Phys. 75, 463 (2011); Izv.Akad.Nauk RAS, Ser.Fiz 75, 499 (2011) A.M.Shirokov, J.P.Vary, V.A.Kulikov, P.Maris, A.I.Mazur, E.A.Mazur Light nuclei in ab initio approach with realistic inverse scattering NN-interaction NUCLEAR STRUCTURE 3H, 3,4,8He, 6Li, 10,14B, 12,14C, 14N, 13,16O, 14F; calculated ground state energies, binding energies. No-core shell model calculations.
doi: 10.3103/S106287381104040X
2011VA04 Acta Phys.Pol. B42, 397 (2011) Ab Initio Nuclear Theory - Progress and Prospects from Quarks to the Cosmos
doi: 10.5506/APhysPolB.42.397
2010LU10 Phys.Rev. C 82, 034003 (2010) T.Luu, M.J.Savage, A.Schwenk, J.P.Vary Nucleon-nucleon scattering in a harmonic potential
doi: 10.1103/PhysRevC.82.034003
2010MA06 Phys.Rev. C 81, 021301 (2010) P.Maris, A.M.Shirokov, J.P.Vary Ab initio nuclear structure simulations: The speculative 14F nucleus NUCLEAR STRUCTURE 6Li, 13O, 14B, 14F; calculated energies of ground states and excited levels using no-core shell model (NCSM) with LSO(2) interaction, and no-core full configuration (NCFC) approach. Comparisons with experimental data.
doi: 10.1103/PhysRevC.81.021301
2010NE02 J.Phys.(London) G37, 055109 (2010) A.G.Negoita, J.P.Vary, S.Stoica No-core shell model for A = 47 and A = 49 NUCLEAR STRUCTURE 47K, 47,48,49Ca, 49Sc; calculated single-particle ground and excitation energy levels, correlation matrix elements. GXPF1 interaction.
doi: 10.1088/0954-3899/37/5/055109
2010VA01 Phys.Rev. C 81, 035205 (2010) J.P.Vary, H.Honkanen, J.Li, P.Maris, S.J.Brodsky, A.Harindranath, G.F.de Teramond, P.Sternberg, E.G.Ng, C.Yang Hamiltonian light-front field theory in a basis function approach
doi: 10.1103/PhysRevC.81.035205
2010VA10 Pramana 75, 39 (2010) J.P.Vary, H.Honkanen, J.Li, P.Maris, A.M.Shirokov, S.J.Brodsky, A.Harindranath, G.F.De Teramond, E.G.Ng, C.Yang, M.Sosonkina Ab-initio Hamiltonian approach to light nuclei and to quantum field theory NUCLEAR STRUCTURE 6Li, 12C; calculated eigenstates, J, π.
doi: 10.1007/s12043-010-0063-2
2009HY01 Phys.Lett. B 678, 459 (2009) S.Hyldegaard, C.Forssen, C.Aa.Diget, M.Alcorta, F.C.Barker, B.Bastin, M.J.G.Borge, R.Boutami, S.Brandenburg, J.Buscher, P.Dendooven, P.Van Duppen, T.Eronen, S.Fox, B.R.Fulton, H.O.U.Fynbo, J.Huikari, M.Huyse, H.B.Jeppesen, A.Jokinen, B.Jonson, K.Jungmann, A.Kankainen, O.Kirsebom, M.Madurga, I.Moore, P.Navratil, T.Nilsson, G.Nyman, G.J.G.Onderwater, H.Penttila, K.Perajarvi, R.Raabe, K.Riisager, S.Rinta-Antila, A.Rogachevskiy, A.Saastamoinen, M.Sohani, O.Tengblad, E.Traykov, J.P.Vary, Y.Wang, K.Wilhelmsen, H.W.Wilschut, J.Aysto Precise branching ratios to unbound 12C states from 12N and 12B β-decays NUCLEAR REACTIONS 1H(12C, n), 2H(11B, p), 12C(p, n), 11B(d, p), E not given; measured Eγ, Iγ, Eα, Iα, γα-coin, αα-coin, decay spectra; deduced branching ratio, log ft, B(GT) to various 12C states. Comparison with no-core shell model calculations. RADIOACTIVITY 12B(β-), 12N(β+); deduced branching ratio, log ft, B(GT) to various 12C states. Comparison with no-core shell model calculations.
doi: 10.1016/j.physletb.2009.06.064
2009LI31 Phys.Rev. C 80, 024315 (2009) A.F.Lisetskiy, M.K.G.Kruse, B.R.Barrett, P.Navratil, I.Stetcu, J.P.Vary Effective operators from exact many-body renormalization NUCLEAR STRUCTURE 6Li; calculated levels, J, π, reduced two-body matrix elements, E2 reduced matrix elements and quadrupole moments using ab initio no-core shell model (NCSM) approach. 7,9Li; calculated absolute quadrupole moments and E2 transition matrix elements. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.024315
2009MA02 Phys.Rev. C 79, 014308 (2009) P.Maris, J.P.Vary, A.M.Shirokov Ab initio no-core full configuration calculations of light nuclei NUCLEAR STRUCTURE 2,3,4H, 3,4,6,8He, 6Li, 12C, 16O; calculated ground-state energies, binding energies. 12C, 16O; calculated energies of first excited 0+ states. No-core full configuration space calculations using realistic nucleon-nucleon interaction JISP16. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.014308
2009MA36 Bull.Rus.Acad.Sci.Phys. 73, 745 (2009); Izv.Akad.Nauk RAS, Ser.Fiz 73, 792 (2009) A.I.Mazur, A.M.Shirokov, E.A.Mazur, J.P.Vary Resonant Parameters of 5He and 5Li States and Nucleon-α Scattering NUCLEAR STRUCTURE 5He, 5Li; calculated resonance energies and widths of low-lying states. J-matrix phase shifts, no-core shell model calculations.
doi: 10.3103/S1062873809060124
2009SH02 Phys.Rev. C 79, 014610 (2009) A.M.Shirokov, A.I.Mazur, J.P.Vary, E.A.Mazur Inverse scattering J-matrix approach to nucleon-nucleus scattering and the shell model NUCLEAR REACTIONS 1n(α, γ), E not given; 1H(α, γ), E=not given;calculated resonance energies, widths. J-matrix inverse scattering approach. Comparison with no-core shell model calculations.
doi: 10.1103/PhysRevC.79.014610
2009VA09 J.Phys.(London) G36, 085103 (2009) J.P.Vary, S.Popescu, S.Stoica, P.Navratil A no-core shell model for 48Ca, 48Sc and 48Ti NUCLEAR STRUCTURE 48Ca, 48Sc, 48Ti; calculated binding, excitation energies, J, π. NCSM model, comparison with experiment.
doi: 10.1088/0954-3899/36/8/085103
2008BO07 Nucl.Phys. A801, 21 (2008) S.K.Bogner, R.J.Furnstahl, P.Maris, R.J.Perry, A.Schwenk, J.P.Vary Convergence in the no-core shell model with low-momentum two-nucleon interactions NUCLEAR STRUCTURE 2,3H, 4,6He, 6,7Li; calculated ground/excited state energies with no core shell model using similarity renormalization group interactions.
doi: 10.1016/j.nuclphysa.2007.12.008
2008DR06 Int.J.Mod.Phys. E17, Supplement 1, 133 (2008) J.P.Draayer, T.Dytrych, K.D.Sviratcheva, C.Bahri, J.P.Vary Symplectic no-core shell model NUCLEAR STRUCTURE 12C, 16O; calculated lowest excited states, J, π. Sympletic no-core shell model (Sp-NCSM).
doi: 10.1142/S0218301308011811
2008DY01 J.Phys.(London) G35, 095101 (2008) T.Dytrych, K.D.Sviratcheva, C.Bahri, J.P.Draayer, J.P.Vary Highly deformed modes in the ab initio symplectic no-core shell model NUCLEAR STRUCTURE 12C, 16O; calculated wavefunction of ground state rotational band; symplectic basis; deformed many-particle many-hole configurations; no-core shell model.
doi: 10.1088/0954-3899/35/9/095101
2008FO02 Phys.Rev. C 77, 024301 (2008) C.Forssen, J.P.Vary, E.Caurier, P.Navratil Converging sequences in the ab initio no-core shell model NUCLEAR STRUCTURE 6Li, 9Be; calculated binding energies, level energies. CDB2k Hamiltonian.
doi: 10.1103/PhysRevC.77.024301
2008LI44 Phys.Rev. C 78, 044302 (2008) A.F.Lisetskiy, B.R.Barrett, M.K.G.Kruse, P.Navratil, I.Stetcu, J.P.Vary Ab-initio shell model with a core NUCLEAR STRUCTURE 6,7Li, 8,9,10He; calculated excitation energies, J, π. Ab-initio no-core shell model calculations.
doi: 10.1103/PhysRevC.78.044302
2008MA33 Bull.Rus.Acad.Sci.Phys. 72, 806 (2008) A.I.Mazur, A.M.Shirokov, J.P.Vary, T.A.Weber, E.A.Mazur Charge-dependent NN interaction in the J-matrix inverse scattering approach
doi: 10.3103/S1062873808060208
2008SH16 Phys.Atomic Nuclei 71, 1232 (2008); Yad.Fiz. 71, 1260 (2008) A.M.Shirokov, J.P.Vary, A.I.Mazur, T.A.Weber Spectroscopy of light nuclei with realistic NN interaction JISP NUCLEAR STRUCTURE 3H, 3,4,6He, 6,7Li, 7,8,9,10Be, 9,10,11,12,13B, 10,11,12,13,14C, 12,13,14,15N, 13,14,15,16O; calculated binding energies using bare and effective interaction; 6Li, 10B; calculated rms radii, ground state quadrupole moments, ground and excited state energies; 10B; calculated B(E2) and B(GT) transition strengths; microscopic no-core shell model; realistic NN interaction.
doi: 10.1134/S1063778808070168
2008VA13 Int.J.Mod.Phys. E17, Supplement 1, 109 (2008) AB initio no core methods: applications to light nuclei NUCLEAR STRUCTURE 4He, 12C, 14F; calculated ground state energies; No-core full configuration (NCFC) approach.
doi: 10.1142/S0218301308011793
2007DY01 Phys.Rev.Lett. 98, 162503 (2007) T.Dytrych, Kristina D.Sviratcheva, C.Bahri, J.P.Draayer, J.P.Vary Evidence for Symplectic Symmetry in Ab Initio No-Core Shell Model Results for Light Nuclei NUCLEAR STRUCTURE 12C, 16O; calculated ground-state configurations; deduced symplectic symmetry. No-core shell model.
doi: 10.1103/PhysRevLett.98.162503
2007DY02 Phys.Rev. C 76, 014315 (2007) T.Dytrych, K.D.Sviratcheva, C.Bahri, J.P.Draayer, J.P.Vary Dominant role of symplectic symmetry in ab initio no-core shell model results for light nuclei NUCLEAR STRUCTURE 12C, 16O; calculated B(E2) within the framework of no-core shell model.
doi: 10.1103/PhysRevC.76.014315
2007MA49 Bull.Rus.Acad.Sci.Phys. 71, 754 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 781 (2007) A.I.Mazur, A.M.Shirokov, J.P.Vary, T.A.Weber, S.A.Zaitsev, E.A.Mazur Nonlocal nucleon-nucleon interaction JISP
doi: 10.3103/S1062873807060020
2007NA16 Phys.Rev.Lett. 99, 042501 (2007) P.Navratil, V.G.Gueorguiev, J.P.Vary, W.E.Ormand, A.Nogga Structure of A=10-13 Nuclei with Two- Plus Three-Nucleon Interactions from Chiral Effective Field Theory NUCLEAR STRUCTURE 4He, 6Li, 10,11B, 12,13C; calculated level energies, B(E2), B(M1), B(GT) using effective field theory.
doi: 10.1103/PhysRevLett.99.042501
2007SH27 Bull.Rus.Acad.Sci.Phys. 71, 764 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 791 (2007) A.M.Shirokov, J.P.Vary, A.I.Mazur, T.A.Weber Nonlocal inverse-scattering nucleon-nucleon interaction and spectra of s- and p-shell nuclei NUCLEAR STRUCTURE H, He, Li, Be, B, C, N, O; calculated binding energies using no-core shell-model.
doi: 10.3103/S1062873807060032
2007SH52 Phys.Lett. B 644, 33 (2007) A.M.Shirokov, J.P.Vary, A.I.Mazur, T.A.Weber Realistic nuclear Hamiltonian: Ab exitu approach NUCLEAR STRUCTURE 3H, 3,4He, 6He, 6,7Li, 7,8,9,10Be, 9,10,11,12B, 10,11,12,13,14C, 12,13,14,15N, 13,14,15,16O; calculated binding energies with bare JISP16 and effective interaction generated by JISP16, ground and excitation energies. Fully-microscopic no-core shell model (NCSM).
doi: 10.1016/j.physletb.2006.10.066
2007SV01 Nucl.Phys. A786, 31 (2007) K.D.Sviratcheva, J.P.Draayer, J.P.Vary Global properties of fp-shell interactions in many-nucleon systems NUCLEAR STRUCTURE 58Ni, 58Cu; calculated levels, J, π. Effective interactions compared using spectral distribution theory.
doi: 10.1016/j.nuclphysa.2007.01.087
2006NE06 Phys.Rev.Lett. 97, 062502 (2006) A.Negret, T.Adachi, B.R.Barrett, C.Baumer, A.M.van den Berg, G.P.A.Berg, P.von Brentano, D.Frekers, D.De Frenne, H.Fujita, K.Fujita, Y.Fujita, E.-W.Grewe, P.Haefner, M.N.Harakeh, K.Hatanaka, K.Heyde, M.Hunyadi, E.Jacobs, Y.Kalmykov, A.Korff, K.Nakanishi, P.Navratil, P.von Neumann-Cosel, L.Popescu, S.Rakers, A.Richter, N.Ryezayeva, Y.Sakemi, A.Shevchenko, Y.Shimbara, Y.Shimizu, Y.Tameshige, A.Tamii, M.Uchida, J.Vary, H.J.Wortche, M.Yosoi, L.Zamick Gamow-Teller Strengths in the A = 14 Multiplet: A Challenge to the Shell Model NUCLEAR REACTIONS 14N(d, 2p), E=175 MeV; 14N(3He, t), E=420 MeV; measured excitation energy spectra, σ(E, θ); deduced Gamow-Teller strength distributions. Comparison with no-core shell model predictions.
doi: 10.1103/PhysRevLett.97.062502
2006NO04 Phys.Rev. C 73, 064002 (2006) A.Nogga, P.Navratil, B.R.Barrett, J.P.Vary Spectra and binding energy predictions of chiral interactions for 7Li NUCLEAR STRUCTURE 7Li; calculated ground and excited states energies; deduced sensitivity to chiral interactions, three-nucleon force. No-core shell model approach.
doi: 10.1103/PhysRevC.73.064002
2006ST06 Phys.Rev. C 73, 037307 (2006) I.Stetcu, B.R.Barrett, P.Navratil, J.P.Vary Long- and short-range correlations in the ab-initio no-core shell model NUCLEAR STRUCTURE 4He, 12C; calculated longitudinal-longitudinal distribution functions, effective operators. No-core shell model, two-body cluster approximation.
doi: 10.1103/PhysRevC.73.037307
2006SV02 Phys.Rev. C 73, 034324 (2006) K.D.Sviratcheva, J.P.Draayer, J.P.Vary Underlying symmetries of realistic interactions and the nuclear many-body problem NUCLEAR STRUCTURE 42Ca, 42Sc, 42Ti, 54Co, 54Fe; calculated levels, J, π, configurations, collective features from realistic interactions. Spectral distribution theory.
doi: 10.1103/PhysRevC.73.034324
2005SH31 Phys.Lett. B 621, 96 (2005) A.M.Shirokov, J.P.Vary, A.I.Mazur, S.A.Zaytsev, T.A.Weber Novel NN interaction and the spectroscopy of light nuclei NUCLEAR STRUCTURE 2H; calculated binding energy, radius, quadrupole moment. 3H, 3,4,6He, 6Li; calculated binding energies. 6He, 6Li; calculated excited states energies, radii, quadrupole moments. Inverse scattering potential.
doi: 10.1016/j.physletb.2005.06.043
2005SH33 J.Phys.(London) G31, S1283 (2005) A.M.Shirokov, J.P.Vary, A.I.Mazur, S.A.Zaytsev, T.A.Weber NN potentials from the J-matrix inverse scattering approach NUCLEAR STRUCTURE 2,3H, 3,4,6He, 6Li; calculated binding energies. 2H calculated radius, D-state probability. 6He, 6Li; calculated excited states energies, radii, quadrupole moments.
doi: 10.1088/0954-3899/31/8/006
2005ST14 Phys.Rev. C 71, 044325 (2005) I.Stetcu, B.R.Barrett, P.Navratil, J.P.Vary Effective operators within the ab initio no-core shell model NUCLEAR STRUCTURE 4He, 6Li, 12C; calculated wave functions, transitions B(M1), B(E2). Effective operator formalism, no-core shell model.
doi: 10.1103/PhysRevC.71.044325
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