NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.I.Mazur Found 30 matches. 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
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
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
2017BL06 Phys.Atomic Nuclei 80, 226 (2017); Yad.Fiz. 80, 102 (2017) L.D.Blokhintsev, A.I.Mazur, I.A.Mazur, D.A.Savin, A.M.Shirokov SS-HORSE method for studying resonances
doi: 10.1134/S1063778817020077
2017BL11 Phys.Atomic Nuclei 80, 1093 (2017) L.D.Blokhintsev, A.I.MazurI.A.Mazur, D.A.Savin, A.M.Shirokov SS-HORSE Method for Analysis of Resonances: Charged-Particle Scattering
doi: 10.1134/S1063778817060072
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
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
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
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
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
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
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
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
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
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
2005VA32 Eur.Phys.J. A 25, Supplement 1, 475 (2005) J.P.Vary, O.V.Atramentov, B.R.Barrett, M.Hasan, A.C.Hayes, R.Lloyd, A.I.Mazur, P.Navratil, A.G.Negoita, A.Nogga, W.E.Ormand, S.Popescu, B.Shehadeh, A.M.Shirokov, J.R.Spence, I.Stetcu, S.Stoica, T.A.Weber, S.A.Zaytsev Ab initio No-Core Shell Model -- Recent results and future prospects NUCLEAR STRUCTURE 4He; calculated radius. 6Li, 16O, 48Ar, 48K, 48Ca, 48Sc, 48Ti, 48V, 48Cr, 48Mn; calculated ground-state energies. 16O, 47Ca; calculated excited states energies. No-core shell model.
doi: 10.1140/epjad/i2005-06-214-x
2004SH41 Phys.Rev. C 70, 044005 (2004) A.M.Shirokov, A.I.Mazur, S.A.Zaytsev, J.P.Vary, T.A.Weber Nucleon-nucleon interaction in the J-matrix inverse scattering approach and few-nucleon systems NUCLEAR REACTIONS 1H(n, n), E=0-350 MeV; calculated phase shifts. No-core shell model, J-matrix version of inverse scattering theory. NUCLEAR STRUCTURE 2,3H, 4He; calculated ground-state energies, radii. 4He calculated excited states energies. No-core shell model, J-matrix version of inverse scattering theory.
doi: 10.1103/PhysRevC.70.044005
2002SH36 Bull.Rus.Acad.Sci.Phys. 65, 1709 (2002) A.M.Shirokov, J.P.Vary, T.A.Weber, A.I.Mazur Realistic NN-Interaction in Shell Model NUCLEAR STRUCTURE 2H; calculated wave function. 3H, 4He; calculated ground-state energies vs model parameters. Phase-equivalent transformations.
1993KN04 Yad.Fiz. 56, No 10, 72 (1993); Phys.Atomic Nuclei 56, 1342 (1993) V.A.Knyr, A.I.Mazur, Yu.F.Smirnov Study of the Reaction 16O(π+, K+)16O(Lambda) with Inclusion of the Continuous Spectrum NUCLEAR REACTIONS 16O(π+, K+), E at 500 MeV/c; analyzed σ(θ, E(K+)); deduced Lambda particle continuum, hole excitation roles. Impulse approximation.
1991KN06 Yad.Fiz. 54, 1518 (1991); Sov.J.Nucl.Phys. 54, 927 (1991) V.A.Knyr, A.I.Mazur, Yu.F.Smirnov Cross Section for Production of the Hypernucleus 7Li(Lambda) with Allowance for the Continuum NUCLEAR REACTIONS 7Li(K-, π-), E not given; calculated σ(θ) vs excitation, hypernucleus decay width. Shell model, continuum effects, R-matrix.
1990KN07 Yad.Fiz. 52, 754 (1990); Sov.J.Nucl.Phys. 52, 483 (1990) V.A.Knyr, A.I.Mazur, Yu.E.Smirnov Calculation of the Cross Section for the 16O(K-, π-)16O(Lambda) Reaction in the Oscillator Representation of Scattering Theory NUCLEAR REACTIONS 16O(K-, π-), E not given; calculated σ(θ) vs hypernucleus excitation; deduced channel coupling effects role. Shell model in the continuum.
1987IS06 Ukr.Fiz.Zh. 32, 1141 (1987) V.Iskra, A.I.Mazur, V.G.Neudachin, Yu.I.Nechaev, Yu.F.Smirnov Interference of Different Partial Amplitudes in Mutual Scattering of the Lightest Clusters NUCLEAR REACTIONS 2H(d, d), E ≤ 250 MeV; calculated partial amplitudes. Resonating group method.
1987KN09 Ukr.Fiz.Zh. 32, 1129 (1987) V.A.Knyr, A.I.Mazur, Yu.F.Smirnov Energy Spectrum of the 7(Lambda)Li Hypernucleus in the Model of Shells NUCLEAR REACTIONS 7Li(K-, π-), E ≤ 25 MeV; calculated σ(θ); deduced hypernucleus decay features. Harmonic oscillator shell model.
Back to query form |