NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = R.Wirth Found 13 matches. 2023ZA03 Eur.Phys.J. A 59, 95 (2023) A.Zare, R.Wirth, C.A.Haselby, H.Hergert, M.Iwen Modewise Johnson-Lindenstrauss embeddings for nuclear many-body theory
doi: 10.1140/epja/s10050-023-00999-5
2022YA19 Phys.Rev. C 106, 014315 (2022) J.M.Yao, I.Ginnett, A.Belley, T.Miyagi, R.Wirth, S.Bogner, J.Engel, H.Hergert, J.D.Holt, S.R.Stroberg Ab initio studies of the double-Gamow-Teller transition and its correlation with neutrinoless double-β decay RADIOACTIVITY 6,8He, 10Be, 14C, 18,22O, 22Ne, 26,28Mg, 30Si, 34S, 38Ar, 42,44,48,56Ca, 50Cr, 46,52Ti(2β-); A=6-76(2β-); calculated nuclear matrix elements (NMEs) for ground-state-to-ground-state double Gamow-Teller transitions (DGT) and Gamow Teller (GT) 0νββ decay, transition densities of parent nuclei, correlation between the transition densities and NMEs of DGT transitions. Ab initio many body methods by importance-truncated no-core shell model (IT-NCSM) with GXPF1A interaction, valence-space in-medium similarity renormalization group method (VSIMSRG) with EM1.8/2.0 interaction, and in-medium generator coordinate method (IM-GCM). 6He, 10Be, 14C, 18O, 22Ne, 26Mg, 30Si, 34S, 38Ar, 42,44Ca, 46Ti, 50Cr; 2β- decay mode forbidden for these nuclei due to negative Q values, however, on query, authors mentioned that these nuclei were included for NMEs for 0νββ decays as these involved the same decay operators that determine the allowed decay rates, thus helpful to benchmark many-body approaches for the nuclear matrix elements of neutrinoless double beta decay.
doi: 10.1103/PhysRevC.106.014315
2021WI16 Phys.Rev.Lett. 127, 242502 (2021) Ab Initio Calculation of the Contact Operator Contribution in the Standard Mechanism for Neutrinoless Double Beta Decay RADIOACTIVITY 6,8He, 48Ca(2β-); calculated the contribution of the leading-order contact transition operator to the nuclear matrix element(NME) of neutrinoless double-beta decay assuming a light Majorana neutrino-exchange mechanism.
doi: 10.1103/PhysRevLett.127.242502
2021YA03 Phys.Rev. C 103, 014315 (2021) J.M.Yao, A.Belley, R.Wirth, T.Miyagi, C.G.Payne, S.R.Stroberg, H.Hergert, J.D.Holt Ab initio benchmarks of neutrinoless double-β decay in light nuclei with a chiral Hamiltonian RADIOACTIVITY 6,8He, 10Be, 14C, 22O(2β-); calculated nuclear matrix elements (NMEs) for isospin-conserving and isospin-changing 0νββ decay modes. Valence-space in-medium similarity renormalization group (VS-IMSRG) and importance-truncated no-core shell model (IT-NCSM) calculations. Comparison with results of calculations using NCSM and coupled-cluster theory with singles and doubles plus leading-order triples excitations (CC-SDT1). NUCLEAR STRUCTURE 6,8He, 6,8,10Be, 10,14C, 14,22O, 22Ne; calculated energies per nucleon (E/A) using VS-IMSRG, in-medium generator coordinate (IM-GCM), and IT-NCSM calculations, and compared with those from the CC-SDT1 calculations.
doi: 10.1103/PhysRevC.103.014315
2021ZH55 Phys.Rev. C 104, 044002 (2021) Singular value decomposition and similarity renormalization group evolution of nuclear interactions NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated ground-state energies as function of flow parameter from in-medium similarity renormalization group (IMSRG) approach. 2H; calculated ground-state energy from singular value decompositions (SVD), similarity renormalization group (SRG) with Entem and Machleidt (EM) interaction. NUCLEAR REACTIONS 1H(p, X), (n, X); calculated singular value spectra in proton-proton and neutron-proton 1S0 partial waves for chiral N3LO two-nucleon, Entem and Machleidt (EM), and AV18 interactions, contours of momentum-space matrix elements of the EM interaction, neutron-proton phase shifts and mixing angles of the EM interaction. Singular value decompositions (SVD) method of nucleon-nucleon interactions in partial wave representation similarity renormalization group (SRG).
doi: 10.1103/PhysRevC.104.044002
2020BR12 Phys. Rev. Res. 2, 022035 (2020) B.A.Brown, K.Minamisono, J.Piekarewicz, H.Hergert, D.Garand, A.Klose, K.Konig, J.D.Lantis, Y.Liu, B.Maass, A.J.Miller, W.Nortershauser, S.V.Pineda, R.C.Powel, D.M.Rossi, F.Sommer, C.Sumithrarachchi, A.Teigelhofer, J.Watkins, R.Wirth Implications of the 36Ca-36S and 38Ca-38Ar difference in mirror charge radii on the neutron matter equation of state NUCLEAR STRUCTURE 36Ca, 36S, 38Ca, 38Ar; analyzed available data; deduced differences in charge radii between mirror nuclei, the slope of the symmetry energy L at the nuclear saturation density. Comparison with theoretical calculations of charge radii, differences and symmetry energy.
doi: 10.1103/PhysRevResearch.2.022035
2020TI05 Eur.Phys.J. A 56, 272 (2020) A.Tichai, R.Wirth, J.Ripoche, T.Duguet Symmetry reduction of tensor networks in many-body theory
doi: 10.1140/epja/s10050-020-00233-6
2020YA16 Phys.Rev.Lett. 124, 232501 (2020) J.M.Yao, B.Bally, J.Engel, R.Wirth, T.R.Rodriguez, H.Hergert Ab Initio Treatment of Collective Correlations and the Neutrinoless Double Beta Decay of 48Ca RADIOACTIVITY 48Ca(2β-); calculated particle-number projected potential energy surfaces. 48Ti; deduced nuclear matrix elements correlations with B(E2).
doi: 10.1103/PhysRevLett.124.232501
2019WI10 Phys.Rev. C 100, 044313 (2019) Similarity renormalization group evolution of hypernuclear Hamiltonians NUCLEAR STRUCTURE 7Li, 9Be, 11B, 13C; calculated low-lying levels, J, π, extrapolated ground-state energies for the hypernuclei. 4,5,6,7H, 5,6,7,8,9,10He; calculated extrapolated absolute energies of low-lying natural-parity states for hypernuclei. 6Li, 8Be, 10B, 12C; calculated low-lying levels, J, π, extrapolated ground-state energies for the core nuclei of corresponding hypernuclei. 3,4,5,6H, 4,5,6,7,8,9He; calculated extrapolated absolute energies of low-lying natural-parity states for the core nuclei of corresponding hypernuclei. Similarity renormalization group (SRG) calculations in a basis spanned by antisymmetric harmonic-oscillator states with respect to three-body Jacobi coordinates and N4LOEMN+N2LONL, N3LOEM+N2LOL and N3LOEM+N2LONLnucleonic Hamiltonians. Comparison with available experimental data.
doi: 10.1103/PhysRevC.100.044313
2018WI03 Phys.Rev. C 97, 064315 (2018) R.Wirth, D.Gazda, P.Navratil, R.Roth Hypernuclear no-core shell model NUCLEAR STRUCTURE 4,5,6,7He; calculated ground state energies, excitation energies of low-lying states in 4,5,6,7He hypernuclei and 4,5,6He core nuclei using Jacobi-coordinate (J-NCSM) and Slater-determinant formulations of no-core shell model (NCSM) for the ab initio description of single-Λ hypernuclei. Comparison with available experimental values.
doi: 10.1103/PhysRevC.97.064315
2016WI07 Phys.Rev.Lett. 117, 182501 (2016) Induced Hyperon-Nucleon-Nucleon Interactions and the Hyperon Puzzle NUCLEAR STRUCTURE 6,7Li, 8,9Be, 12,13C; calculated hypernuclei separation and binding energies, energy levels, J, π.
doi: 10.1103/PhysRevLett.117.182501
2014GA25 Few-Body Systems 55, 857 (2014) D.Gazda, J.Mares, P.Navratil, R.Roth, R.Wirth No-Core Shell Model for Nuclear Systems with Strangeness NUCLEAR STRUCTURE 3,4H, 4He; calculated hypernuclei ground state, and separation energies. ab initio approach, comparison with available data.
doi: 10.1007/s00601-014-0848-9
2014WI05 Phys.Rev.Lett. 113, 192502 (2014) R.Wirth, D.Gazda, P.Navratil, A.Calci, J.Langhammer, R.Roth AbĀInitio Description of p-Shell Hypernuclei NUCLEAR STRUCTURE 7Li, 9Be, 13C; calculated ground-state energy of s-shell hypernuclei, absolute and excitation energies.
doi: 10.1103/PhysRevLett.113.192502
Back to query form Note: The following list of authors and aliases matches the search parameter R.Wirth: , R.K.WIRTH |