NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.E.Sobczyk Found 11 matches. 2024SO05 Phys.Rev. C 109, 025502 (2024) J.E.Sobczyk, B.Acharya, S.Bacca, G.Hagen 40Ca transverse response function from coupled-cluster theory
doi: 10.1103/PhysRevC.109.025502
2023AN15 J.Phys.(London) G50, 120501 (2023) A.M.Ankowski, A.Ashkenazi, S.Bacca, J.L.Barrow, M.Betancourt, A.Bodek, M.E.Christy, L.Doria, S.Dytman, A.Friedland, O.Hen, C.J.Horowitz, N.Jachowicz, W.Ketchum, T.Lux, K.Mahn, C.Mariani, J.Newby, V.Pandey, A.Papadopoulou, E.Radicioni, F.Sanchez, C.Sfienti, J.M.Udias, L.Weinstein, L.Alvarez-Ruso, J.E.Amaro, C.A.Arguelles, A.B.Balantekin, S.Bolognesi, V.Brdar, P.Butti, S.Carey, Z.Djurcic, O.Dvornikov, S.Edayath, S.Gardiner, J.Isaacson, W.Jay, A.Klustova, K.S.McFarland, A.Nikolakopoulos, A.Norrick, S.Pastore, G.Paz, M.H.Reno, I.Ruiz Simo, J.E.Sobczyk, A.Sousa, N.Toro, Y.-D.Tsai, M.Wagman, J.G.Walsh, G.Yang Electron scattering and neutrino physics
doi: 10.1088/1361-6471/acef42
2023MI19 Eur.Phys.J. A 59, 225 (2023) M.Mihovilovic, P.Achenbach, C.Ayerbe Gayoso, M.Bajec, T.Beranek, J.Bericic, J.C.Bernauer, R.Bohm, D.Bosnar, M.Cardinali, L.Correa, L.Debenjak, A.Denig, M.O.Distler, A.Esser, M.I.Ferretti-Bondy, H.Fonvieille, J.M.Friedrich, I.Friscic, K.Griffioen, M.Hoek, S.Kegel, Y.Stottinger, H.Merkel, D.G.Middleton, U.Muller, L.Nungesser, J.Pochodzalla, M.Rohrbeck, S.Sanchez Majos, B.S.Schlimme, M.Schoth, F.Schulz, C.Sfienti, S.Sirca, J.E.Sobczyk, S.Stajner, M.Thiel, A.Tyukin, M.Vanderhaeghen, A.B.Weber, M.Weinriefer Non-forward radiative corrections to electron-carbon scattering
doi: 10.1140/epja/s10050-023-01128-y
2022SO15 Phys.Rev. C 106, 034310 (2022) J.E.Sobczyk, S.Bacca, G.Hagen, T.Papenbrock Spectral function for 4He using the Chebyshev expansion in coupled-cluster theory NUCLEAR REACTIONS 4He(e, e'), at momentum transfers q ≈ 270-670 MeV; calculated intrinsic momentum distribution, and compared with that in laboratory system, spectral functions, differential σ(momentum transfer) using coupled-cluster singles-and-doubles (CCSD) approximation, with an expansion of integral transforms into Chebyshev polynomials.
doi: 10.1103/PhysRevC.106.034310
2021SO24 Phys.Rev.Lett. 127, 072501 (2021) J.E.Sobczyk, B.Acharya, S.Bacca, G.Hagen Ab Initio Computation of the Longitudinal Response Function in 40Ca NUCLEAR STRUCTURE 40Ca; calculated longitudinal response function using the coupled-cluster and Lorentz integral transform methods starting from chiral nucleon-nucleon and three-nucleon interactions.
doi: 10.1103/PhysRevLett.127.072501
2020SO16 Phys.Rev. C 102, 024601 (2020) J.E.Sobczyk, J.Nieves, F.Sanchez Exclusive-final-state hadron observables from neutrino-nucleus multinucleon knockout NUCLEAR REACTIONS 12C(ν, X), E=0.2-2 GeV; calculated total σ(E). 12C(ν, X), E=0.5, 1.0, 1.5 GeV; calculated differential cross sections. 12C(ν, 2p), (ν, np), E=1.5 GeV; calculated available energies and outgoing nucleons distribution for two protons and for proton-neutron final states in the primary vertex. Calculation of the two particle-two hole 2p2h and 3p3h contributions to the neutrino induced charge-current cross section using the NEUT generator. Comparison to results from MC event generators. Relevance to neutrino oscillation experiments.
doi: 10.1103/PhysRevC.102.024601
2020SO21 Phys.Rev. C 102, 064312 (2020) J.E.Sobczyk, B.Acharya, S.Bacca, G.Hagen Coulomb sum rule for 4He and 16O from coupled-cluster theory NUCLEAR STRUCTURE 4He, 16O; calculated Coulomb sum rule (CSR), squared elastic form factors, spurious 1- states as functions of the momentum transfer of 0-500 MeV. Coupled-cluster theory using interactions from chiral effective field theory (EFT). Relevance to improving understanding of neutrino-nucleus scattering process.
doi: 10.1103/PhysRevC.102.064312
2019SO10 Phys.Rev. C 99, 065503 (2019) J.E.Sobczyk, N.Rocco, A.Lovato, J.Nieves Weak production of strange and charmed ground-state baryons in nuclei NUCLEAR REACTIONS 12C, 16O, 40Ca(ν-bar, μ+Λ), (ν-bar, μ+Σ-), (ν-bar, μ+Σ0), (ν-bar, μ+Σ+), (ν-bar, μ-Λ), E=0.5-5 GeV; calculated differential σ(E, θ) and total σ(E) for muonic neutrino beams, form factors using realistic hole spectral functions with propagation of hyperons in the nuclear medium via a Monte Carlo cascade. Implications in the analysis of experiments from SciBooNE, MicroBooNE, MINERvA and ArgoNeuT collaborations.
doi: 10.1103/PhysRevC.99.065503
2019SO16 Phys.Rev. C 100, 035501 (2019) J.E.Sobczyk, N.Rocco, J.Nieves Polarization of t in quasielastic (anti)neutrino scattering: The role of spectral functions NUCLEAR REACTIONS 16O(ν, ν), (ν-bar, ν-bar'), E=4, 6 GeV; calculated double-differential σ(θ, E) and polarization components for scattering of τ neutrino or anti-neutrino off 16O; analyzed cross sections and polarization components for the charge-current reaction, focusing on the quasielastic region where the single nucleon knock-out dominates reaction mechanism. Relevance to experiments at SHiP facility, and neutrino oscillations.
doi: 10.1103/PhysRevC.100.035501
2018SO03 Phys.Rev. C 97, 035506 (2018) J.E.Sobczyk, N.Rocco, A.Lovato, J.Nieves Scaling within the spectral function approach NUCLEAR REACTIONS 12C(e, e'), at momentum transfer q=0.57-1.2 GeV; calculated nucleon-density response function, transverse, longitudinal, and nucleon-density scaling functions, nonrelativistic PWIA scaling responses using two approaches, semi-phenomenological model, and hole spectral function (SF) based on correlated basis function (CBF). Comparison with experimental data.
doi: 10.1103/PhysRevC.97.035506
2017SO22 Phys.Rev. C 96, 045501 (2017) Intercomparison of lepton-nucleus scattering models in the quasielastic region NUCLEAR REACTIONS 12C(e, e), (e, e'), E=200-2130 MeV; analyzed quasielastic (QE) scattering data from T2K experiment using various models of electron-nucleus scattering: Benhar's spectral function model with and without the final-state interactions, Valencia spectral function, Giessen Boltzmann-Uehling-Uhlenbeck (GiBUU), and predictions of the global and local Fermi gas models. Relevance to systematic errors in the neutrino oscillation experiments.
doi: 10.1103/PhysRevC.96.045501
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