NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = J.Dohet-Eraly Found 13 matches. 2024DE09 Few-Body Systems 65, 9 (2024) Resonances in the R-Matrix Method NUCLEAR STRUCTURE 6He, 6Be; analyzed available data; deduced resonance parameters, bound state energy with an extension of the traditional R-matrix method, which allows an accurate determination of the energy and width of a resonance.
doi: 10.1007/s00601-023-01876-z
2023DU12 Phys.Rev. C 108, 054003 (2023) P.-Y.Duerinck, R.Lazauskas, J.Dohet-Eraly Antiproton-deuteron hydrogenic states from a coupled-channel approach
doi: 10.1103/PhysRevC.108.054003
2021DO04 Phys.Rev. C 103, 034619 (2021) Exchange effects in nucleus-nucleus reactions NUCLEAR REACTIONS 13C(12C, 12C), (12C, 12C'), E(cm)=7.8, 14.2 MeV; 13N(12C, 12C), E(cm)=7.8, 9.6 MeV; 16O(12C, 12C), E(cm)=23.4 MeV; calculated elastic scattering σ(E, q), inelastic σ(Ε, θ) for 13C+12C, amplitudes of scattering matrices, local effective potentials, contributions of the overlap, kinetic energy, and potentials to the nonlocal kernels. Scattering three-body model with coupled-channel system, including nonlocal terms, and R-matrix method using Lagrange functions, an extension of continuum discretized coupled channel (CDCC) formalism, with treatment of exchange effects in nucleus-nucleus scattering. Comparison with experimental data.
doi: 10.1103/PhysRevC.103.034619
2020BA13 Phys.Rev. A 101, 022507 (2020) Quasibound states of an antiproton and a hydrogen atom ATOMIC PHYSICS H; calculated three-body quantal system composed of a proton, an antiproton, and an electron are performed in perimetric coordinates with the Lagrange-mesh method.
doi: 10.1103/PhysRevA.101.022507
2018VI01 Few-Body Systems 59, 73 (2018) M.Viviani, L.Girlanda, A.Kievsky, L.E.Marcucci, J.Dohet-Eraly Three-nucleon force effects in A=4 scattering NUCLEAR REACTIONS 3H(p, X)4He, E<3 MeV; calculated phase shift, σ(θ). Comparison with available data.
doi: 10.1007/s00601-018-1379-6
2017KU11 Phys.Rev.Lett. 118, 262502 (2017) A.Kumar, R.Kanungo, A.Calci, P.Navratil, A.Sanetullaev, M.Alcorta, V.Bildstein, G.Christian, B.Davids, J.Dohet-Eraly, J.Fallis, A.T.Gallant, G.Hackman, B.Hadinia, G.Hupin, S.Ishimoto, R.Krucken, A.T.Laffoley, J.Lighthall, D.Miller, S.Quaglioni, J.S.Randhawa, E.T.Rand, A.Rojas, R.Roth, A.Shotter, J.Tanaka, I.Tanihata, C.Unsworth Nuclear Force Imprints Revealed on the Elastic Scattering of Protons with 10C NUCLEAR REACTIONS 10C(p, p), E(cm)=4.15, 4.4 eV; measured reaction products, Ep, Ip; deduced σ(θ). Comparison with ab initio no-core shell model with continuum calculations.
doi: 10.1103/PhysRevLett.118.262502
2016CA39 Phys.Rev.Lett. 117, 242501 (2016) A.Calci, P.Navratil, R.Roth, J.Dohet-Eraly, S.Quaglioni, G.Hupin Can Ab Initio Theory Explain the Phenomenon of Parity Inversion in 11Be? NUCLEAR STRUCTURE 11Be; calculated J, π, B(E1). Comparison with experimental data.
doi: 10.1103/PhysRevLett.117.242501
2016DO04 Phys.Lett. B 757, 430 (2016) J.Dohet-Eraly, P.Navratil, S.Quaglioni, W.Horiuchi, G.Hupin, F.Raimondi 3He(α, γ)7Be and 3H(α, γ)7Li astrophysical S factors from the no-core shell model with continuum NUCLEAR REACTIONS 3He, 3H(α, γ), E<4 MeV; calculated S-factors, σ using no-core shell model. Comparison with available data.
doi: 10.1016/j.physletb.2016.04.021
2015SM03 Phys.Rev. C 92, 064314 (2015) D.Smalley, H.Iwasaki, P.Navratil, R.Roth, J.Langhammer, V.M.Bader, D.Bazin, J.S.Berryman, C.M.Campbell, J.Dohet-Eraly, P.Fallon, A.Gade, C.Langer, A.Lemasson, C.Loelius, A.O.Macchiavelli, C.Morse, J.Parker, S.Quaglioni, F.Recchia, S.R.Stroberg, D.Weisshaar, K.Whitmore, K.Wimmer Lifetime measurements of 17C excited states and three-body and continuum effects NUCLEAR REACTIONS 9Be(18C, 17C), E=74.2 MeV/nucleon, [secondary 18C beam from 9Be(22Ne, X), E=120 MeV/nucleon primary reaction using A1900 fragment separator at NSCL-MSU]; measured one-neutron knockout reaction products, Eγ, Iγ, (particle)γ-coin using GRETINA array for γ rays, and S800 spectrograph for particles, level half-lives using RDM method and a plunger device. 17C; deduced levels, J, π, B(M1). Comparison with importance-truncated no-core shell model (IT-NCSM), and importance-truncated no-core shell model with continuum (IT-NCSMC) calculations.
doi: 10.1103/PhysRevC.92.064314
2014DO01 Phys.Rev. C 89, 024617 (2014) Microscopic description of α + N bremsstrahlung by a Siegert approach NUCLEAR REACTIONS 4He(p, X)γ, (n, X)γ, E<16 MeV; calculated σ(E) for E1 E2 bremsstrahlung. Comparison between Siegert and nonsiegert approaches. Microscopic cluster model of bremsstrahlung.
doi: 10.1103/PhysRevC.89.024617
2014DO11 Phys.Rev. C 90, 034611 (2014) Comparison of potential models of nucleus-nucleus bremsstrahlung
doi: 10.1103/PhysRevC.90.034611
2013DO18 Phys.Rev. C 88, 024602 (2013) Siegert approach within a microscopic description of nucleus-nucleus bremsstrahlung NUCLEAR REACTIONS 4He(α, αγ)4He, E<24 MeV; calculated differential σ(E) for nuclear bremsstrahlung; comparison between Siegart and non-Siegart approaches. Microscopic cluster model of nucleus-nucleus bremsstrahlung. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.024602
2011DO13 Phys.Rev. C 84, 014604 (2011) Microscopic cluster model of α + n, α + p, α+ 3He, and α + α elastic scattering from a realistic effective nuclear interaction NUCLEAR REACTIONS 1n, 1H, 3He, 4He(α, α), E<14 MeV; calculated elastic phase shifts. Microscopic cluster model with UCOM realistic nucleon-nucleon interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.014604
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