NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = D.R.Entem Found 37 matches. 2023SA11 Phys.Rev. C 107, 034002 (2023) S.K.Saha, D.R.Entem, R.Machleidt, Y.Nosyk Local position-space two-nucleon potentials from leading to fourth order of chiral effective field theory NUCLEAR REACTIONS 1H(p, X), (n, X), E<290 MeV; calculated phase shifts, cutoff variations for phase shifts, scattering lengths, effective ranges. Local, position-space chiral NN potential through four orders of chiral effective field theory ranging from LO to N3LO. Comparison with phenomenological Argonne ν18 (AV18) potential. NUCLEAR STRUCTURE 2H; calculated binding energy, asymptotic S state, asymptotic D/S state, quadrupole moment, D-state probability from the nucleon-nucleon potentials of the present study. 3H; calculated binding energy.
doi: 10.1103/PhysRevC.107.034002
2023TA05 Eur.Phys.J. A 59, 40 (2023) U.Taboada-Nieto, P.G.Ortega, D.R.Entem, F.Fernandez, J.Segovia Kaon spectrum revisited: bound states of high energy and spin
doi: 10.1140/epja/s10050-023-00963-3
2021NO12 Phys.Rev. C 104, 054001 (2021) Y.Nosyk, D.R.Entem, R.Machleidt Nucleon-nucleon potentials from Δ-full chiral effective-field-theory and implications NUCLEAR REACTIONS 1H(n, X), E<200 MeV; calculated neutron-proton scattering phase parameters predicted by Goteborg-Oak Ridge (GO) potentials: NNLO(450)GO, NNLO(394)GO, NNLO(450)Rf and NNLO(394)Rf with fits in the present work, scattering lengths and effective ranges, energy per nucleon in symmetric nuclear matter; investigated chiral nucleon-nucleon potentials at NNLO including Δ-isobar degrees. 2H; predicted binding energy, asymptotic S state, asymptotic D/S state, structure radius, quadrupole moment, D-state probability from the nucleon-nucleon potentials of the present study.
doi: 10.1103/PhysRevC.104.054001
2017EN03 Phys.Rev. C 96, 024004 (2017) D.R.Entem, R.Machleidt, Y.Nosyk High-quality two-nucleon potentials up to fifth order of the chiral expansion
doi: 10.1103/PhysRevC.96.024004
2016PE12 Nucl.Phys. A954, 213 (2016) A.Perez-Obiol, D.R.Entem, B.Julia-Diaz, A.Parreno Next-to-leading order effective field theory ΛN → NN potential in coordinate space
doi: 10.1016/j.nuclphysa.2016.04.039
2015EN01 Phys.Rev. C 91, 014002 (2015) D.R.Entem, N.Kaiser, R.Machleidt, Y.Nosyk Peripheral nucleon-nucleon scattering at fifth order of chiral perturbation theory
doi: 10.1103/PhysRevC.91.014002
2015EN05 Phys.Rev. C 92, 064001 (2015) D.R.Entem, N.Kaiser, R.Machleidt, Y.Nosyk Dominant contributions to the nucleon-nucleon interaction at sixth order of chiral perturbation theory
doi: 10.1103/PhysRevC.92.064001
2013MA80 Phys.Rev. C 88, 054002 (2013) E.Marji, A.Canul, Q.MacPherson, R.Winzer, Ch.Zeoli, D.R.Entem, R.Machleidt Nonperturbative renormalization of the chiral nucleon-nucleon interaction up to next-to-next-to-leading order
doi: 10.1103/PhysRevC.88.054002
2013PE05 Phys.Rev. C 87, 044614 (2013) A.Perez-Obiol, D.R.Entem, B.Julia-Diaz, A.Parreno One-loop contributions in the effective field theory for the ΛN → NN transition
doi: 10.1103/PhysRevC.87.044614
2013PE17 Nucl.Phys. A914, 199c (2013) A.Perez-Obiol, D.R.Entem, B.Julia-Diaz, A.Parreno Higher order contributions to the weak ΛN → NN interaction in effective field theory
doi: 10.1016/j.nuclphysa.2013.12.122
2013SE15 Nucl.Phys. A915, 125 (2013) J.Segovia, D.R.Entem, F.Fernandez Strong charmonium decays in a microscopic model
doi: 10.1016/j.nuclphysa.2013.07.004
2011MA28 Phys.Rep. 503, 1 (2011) Chiral effective field theory and nuclear forces
doi: 10.1016/j.physrep.2011.02.001
2010MA07 Phys.Rev. C 81, 024001 (2010) R.Machleidt, P.Liu, D.R.Entem, E.R.Arriola Renormalization of the leading-order chiral nucleon-nucleon interaction and bulk properties of nuclear matter
doi: 10.1103/PhysRevC.81.024001
2009EN04 Phys.Rev. C 80, 047001 (2009) Renormalization of the off-shell chiral two-pion exchange NN interactions
doi: 10.1103/PhysRevC.80.047001
2008EN01 Phys.Rev. C 77, 044006 (2008) D.R.Entem, E.Ruiz Arriola, M.Pavon Valderrama, R.Machleidt Renormalization of chiral two-pion exchange NN interactions: Momentum space versus coordinate space
doi: 10.1103/PhysRevC.77.044006
2007CO04 Phys.Rev. C 75, 024311 (2007) L.Coraggio, A.Covello, A.Gargano, N.Itaco, D.R.Entem, T.T.S.Kuo, R.Machleidt Low-momentum nucleon-nucleon interactions and shell-model calculations NUCLEAR STRUCTURE 18,20,22,24,26O; calculated ground and excited states energies. Low-momentum potential.
doi: 10.1103/PhysRevC.75.024311
2007EN03 Phys.Rev. D 75, 014004 (2007) Final state interaction effects in near threshold enhancement of the p(p-bar) mass spectrum in B and J/ψ decays
doi: 10.1103/PhysRevD.75.014004
2007EN04 Eur.Phys.J. A 31, 649 (2007) X(1859) Baryonium or something else? NUCLEAR REACTIONS 1H(p-bar, X), (n-bar, X), E ≈ 100-800 MeV; analyzed total and annihilation σ; deduced possible resonance states features. Constituent-quark model.
doi: 10.1140/epja/i2006-10209-3
2007EN06 Nucl.Phys. A790, 340c (2007) N N-bar quasibound states: J/ψ decay and p-bar -atomic evidences
doi: 10.1016/j.nuclphysa.2007.03.176
2006EN03 Phys.Rev. C 73, 045214 (2006) The N(N-bar) interaction in a constituent quark model: Baryonium states and protonium level shifts NUCLEAR REACTIONS 1H(p-bar, X), (n-bar, X), E ≈ 100-900 MeV; analyzed σ, possible bound states features.
doi: 10.1103/PhysRevC.73.045214
2005MA58 J.Phys.(London) G31, S1235 (2005) Towards a consistent approach to nuclear structure: EFT of two- and many-body forces
doi: 10.1088/0954-3899/31/8/001
2004MA43 Nucl.Phys. A737, 223 (2004) The nuclear force problem: Are we seeing the end of the tunnel?
doi: 10.1016/j.nuclphysa.2004.03.080
2003BO37 Phys.Lett. B 576, 265 (2003) S.K.Bogner, T.T.S.Kuo, A.Schwenk, D.R.Entem, R.Machleidt Towards a model-independent low momentum nucleon-nucleon interactions
doi: 10.1016/j.physletb.2003.10.012
2003EN01 Phys.Rev. C 67, 014001 (2003) D.R.Entem, F.Fernandez, A.Valcarce Two-nucleon system above pion threshold: Quark model study
doi: 10.1103/PhysRevC.67.014001
2003EN09 Phys.Rev. C 68, 041001 (2003) Accurate charge-dependent nucleon-nucleon potential at fourth order of chiral perturbation theory NUCLEAR REACTIONS 1H(n, n), E=0-300 MeV; calculated phase shift parameters, scattering lengths. Fourth-order chiral perturbation theory. NUCLEAR STRUCTURE 2H; calculated binding energy, radius, quadrupole moment, D-state probability. 3H; calculated binding energy. Fourth-order chiral perturbation theory.
doi: 10.1103/PhysRevC.68.041001
2002CO20 Phys.Rev. C66, 021303 (2002) L.Coraggio, A.Covello, A.Gargano, N.Itaco, T.T.S.Kuo, D.R.Entem, R.Machleidt Microscopic nuclear structure based upon a chiral NN potential NUCLEAR STRUCTURE 18O, 134Te, 210Po; calculated levels, J, π, binding energies. Shell model, chiral effective field theory, comparison with data.
doi: 10.1103/PhysRevC.66.021303
2002EN01 Phys.Lett. 524B, 93 (2002) Accurate Nucleon-Nucleon Potential Based Upon Chiral Perturbation Theory NUCLEAR REACTIONS 1H(n, n), E < 300 MeV; calculated phase shifts. Chiral effective Lagrangians, comparison with data. NUCLEAR STRUCTURE 2,3H; calculated binding energy. 2H calculated radius, quadrupole moment. Chiral effective Lagrangians, comparison with data.
doi: 10.1016/S0370-2693(01)01363-6
2002EN04 Phys.Rev. C65, 064005 (2002) D.R.Entem, R.Machleidt, H.Witala Chiral NN Model and Ay Puzzle NUCLEAR REACTIONS 2H(n, n), (p, p), E=3, 10, 65 MeV; calculated σ(θ), Ay(θ), other polarization observables. Chiral NN model, comparison with data.
doi: 10.1103/PhysRevC.65.064005
2002EN08 Phys.Rev. C66, 014002 (2002) Chiral 2π Exchange at Fourth Order and Peripheral NN Scattering NUCLEAR REACTIONS 1H(n, X), E<300 MeV; calculated phase shifts, two-pion exchange contributions. Effective chiral Lagrangians, fourth-order contributions.
doi: 10.1103/PhysRevC.66.014002
2002FR06 Phys.Rev. C65, 034316 (2002) T.Frick, S.Kaiser, H.Muther, A.Polls, D.R.Entem, R.Machleidt Δ(1232) Isobar Excitations and the Ground State of Nuclei NUCLEAR STRUCTURE 16O; calculated ground-state binding energy, radius, Δ probability.
doi: 10.1103/PhysRevC.65.034316
2002JU11 Phys.Rev. C66, 047002 (2002) B.Julia-Diaz, D.R.Entem, A.Valcarce, F.Fernandez Deuteron NN*(1440) components from a chiral quark model NUCLEAR STRUCTURE 2H; calculated resonance components. Chiral quark model.
doi: 10.1103/PhysRevC.66.047002
2002MO08 Phys.Rev. C65, 034006 (2002) R.D.Mota, A.Valcarce, F.Fernandez, D.R.Entem, H.Garcilazo Nonlocal Calculation for Nonstrange Dibaryons and Tribaryons NUCLEAR STRUCTURE A=2-3; calculated two- and three-baryon systems binding energies. Chiral quark cluster model, nonlocal potentials, resonating group method.
doi: 10.1103/PhysRevC.65.034006
2001EN04 J.Phys.(London) G27, 1537 (2001) D.R.Entem, F.Fernandez, A.Valcarce Separable Representation of the Nucleon-Nucleon Chiral Quark Cluster Model Potential NUCLEAR STRUCTURE 2H; calculated binding energy. Quark cluster model nucleon-nucleon potential.
2000EN06 Nucl.Phys. A663-664, 699c (2000) D.R.Entem, F.Fernandez, A.Valcarce Chrial Quark Cluster Model Description of Isospin Violation in the Nuclear Force
doi: 10.1016/S0375-9474(99)00725-3
2000EN11 Phys.Rev. C62, 034002 (2000) D.R.Entem, F.Fernandez, A.Valcarce Chiral Quark Model of the NN System within a Lippmann-Schwinger Resonating Group Method
doi: 10.1103/PhysRevC.62.034002
1999EN05 Phys.Lett. 463B, 153 (1999) D.R.Entem, F.Fernandez, A.Valcarce Chsrge Dependence and Charge Asymmetry of Nuclear Forces in Chiral Quark Cluster Models
doi: 10.1016/S0370-2693(99)00970-3
1996EN04 Nucl.Phys. A602, 308 (1996) D.R.Entem, A.I.Machavariani, A.Valcarce, A.J.Buchmann, A.Faessler, F.Fernandez A Chiral Quark Model and the Spin Observables in Nucleon-Nucleon Scattering NUCLEAR REACTIONS 1n, 1H(p, p), E=25-250 MeV; analyzed σ(θ), polarization observables data; deduced sensitivity to phase shifts modifications. Nonrelativistic constituent quark model.
doi: 10.1016/0375-9474(96)00111-X
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