NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.A.Caballero Found 91 matches. 2024FR03 Phys.Rev. D 109, 013004 (2024) J.M.Franco-Patino, S.Dolan, R.Gonzalez-Jimenez, M.B.Barbaro, J.A.Caballero, G.D.Megias New model comparison for semi-inclusive charged-current electron and muon neutrino scattering by 40Ar in the energy range of the MicroBooNE experiment NUCLEAR REACTIONS 40Ar(ν, X), E<1.5 GeV; measured reaction products, En, In; deduced missing energy profile of neutrons, σ(θ). Comparison with the relativistic distorted wave impulse approximation (RDWIA) calculations using ED-RMF and ROP FSI models, and the SuSAν2 model implemented in GENIE.
doi: 10.1103/PhysRevD.109.013004
2023AB32 Phys.Rev. D 108, 092009 (2023) K.Abe, N.Akhlaq, R.Akutsu, A.Ali, S.Alonso Monsalve, C.Alt, C.Andreopoulos, M.Antonova, S.Aoki, T.Arihara, Y.Asada, Y.Ashida, E.T.Atkin, M.Barbi, G.J.Barker, G.Barr, D.Barrow, M.Batkiewicz-Kwasniak, V.Berardi, L.Berns, S.Bhadra, A.Blanchet, A.Blondel, S.Bolognesi, T.Bonus, S.Bordoni, S.B.Boyd, A.Bravar, C.Bronner, S.Bron, A.Bubak, M.Buizza Avanzini, J.A.Caballero, N.F.Calabria, S.Cao, D.Carabadjac, A.J.Carter, S.L.Cartwright, M.P.Casado, M.G.Catanesi, A.Cervera, J.Chakrani, D.Cherdack, P.S.Chong, G.Christodoulou, A.Chvirova, M.Cicerchia, J.Coleman, G.Collazuol, L.Cook, A.Cudd, C.Dalmazzone, T.Daret, Yu.I.Davydov, A.De Roeck, G.De Rosa, T.Dealtry, C.C.Delogu, C.Densham, A.Dergacheva, F.Di Lodovico, S.Dolan, D.Douqa, T.A.Doyle, O.Drapier, J.Dumarchez, P.Dunne, K.Dygnarowicz, A.Eguchi, S.Emery-Schrenk, G.Erofeev, A.Ershova, G.Eurin, D.Fedorova, S.Fedotov, M.Feltre, A.J.Finch, G.A.Fiorentini Aguirre, G.Fiorillo, M.D.Fitton, J.M.Franco Patino, M.Friend, Y.Fujii, Y.Fukuda, Y.Furui, L.Giannessi, C.Giganti, V.Glagolev, M.Gonin, J.Gonzalez Rosa, E.A.G.Goodman, A.Gorin, M.Grassi, M.Guigue, D.R.Hadley, J.T.Haigh, P.Hamacher-Baumann, D.A.Harris, M.Hartz, T.Hasegawa, S.Hassani, N.C.Hastings, Y.Hayato, D.Henaff, M.Hogan, J.Holeczek, A.Holin, T.Holvey, N.T.Hong Van, T.Honjo, A.K.Ichikawa, M.Ikeda, T.Ishida, M.Ishitsuka, H.T.Israel, A.Izmaylov, M.Jakkapu, B.Jamieson, S.J.Jenkins, C.Jesus-Valls, J.J.Jiang, J.Y.Ji, P.Jonsson, S.Joshi, C.K.Jung, P.B.Jurj, M.Kabirnezhad, A.C.Kaboth, T.Kajita, H.Kakuno, J.Kameda, S.P.Kasetti, Y.Kataoka, T.Katori, M.Kawaue, E.Kearns, M.Khabibullin, A.Khotjantsev, T.Kikawa, S.King, V.Kiseeva, J.Kisiel, H.Kobayashi, T.Kobayashi, L.Koch, S.Kodama, A.Konaka, L.L.Kormos, Y.Koshio, T.Koto, K.Kowalik, Y.Kudenko, Y.Kudo, S.Kuribayashi, R.Kurjata, T.Kutter, M.Kuze, M.La Commara, L.Labarga, K.Lachner, J.Lagoda, S.M.Lakshmi, M.Lamers James, M.Lamoureux, A.Langella, J.-F.Laporte, D.Last, N.Latham, M.Laveder, L.Lavitola, M.Lawe, Y.Lee, C.Lin, S.-K.Lin, R.P.Litchfield, S.L.Liu, W.Li, A.Longhin, K.R.Long, A.Lopez Moreno, L.Ludovici, X.Lu, T.Lux, L.N.Machado, L.Magaletti, K.Mahn, M.Malek, M.Mandal, S.Manly, A.D.Marino, L.Marti-Magro, D.G.R.Martin, M.Martini, J.F.Martin, T.Maruyama, T.Matsubara, V.Matveev, C.Mauger, K.Mavrokoridis, E.Mazzucato, N.McCauley, J.McElwee, K.S.McFarland, C.McGrew, J.McKean, A.Mefodiev, G.D.Megias, P.Mehta, L.Mellet, C.Metelko, M.Mezzetto, E.Miller, A.Minamino, O.Mineev, S.Mine, M.Miura, L.Molina Bueno, S.Moriyama, S.Moriyama, P.Morrison, Th.A.Mueller, D.Munford, L.Munteanu, K.Nagai, Y.Nagai, T.Nakadaira, K.Nakagiri, M.Nakahata, Y.Nakajima, A.Nakamura, H.Nakamura, K.Nakamura, K.D.Nakamura, Y.Nakano, S.Nakayama, T.Nakaya, K.Nakayoshi, C.E.R.Naseby, T.V.Ngoc, V.Q.Nguyen, K.Niewczas, S.Nishimori, Y.Nishimura, K.Nishizaki, T.Nosek, F.Nova, P.Novella, J.C.Nugent, H.M.O'Keeffe, L.O'Sullivan, T.Odagawa, W.Okinaga, K.Okumura, T.Okusawa, N.Ospina, Y.Oyama, V.Palladino, V.Paolone, M.Pari, J.Parlone, J.Pasternak, M.Pavin, D.Payne, G.C.Penn, D.Pershey, L.Pickering, C.Pidcott, G.Pintaudi, C.Pistillo, B.Popov, K.Porwit, M.Posiadala-Zezula, Y.S.Prabhu, F.Pupilli, B.Quilain, T.Radermacher, E.Radicioni, B.Radics, M.A.Ramirez, P.N.Ratoff, M.Reh, C.Riccio, E.Rondio, S.Roth, N.Roy, A.Rubbia, A.C.Ruggeri, C.A.Ruggles, A.Rychter, K.Sakashita, F.Sanchez, C.M.Schloesser, K.Scholberg, M.Scott, Y.Seiya, T.Sekiguchi, H.Sekiya, D.Sgalaberna, A.Shaikhiev, F.Shaker, M.Shiozawa, W.Shorrock, A.Shvartsman, N.Skrobova, K.Skwarczynski, D.Smyczek, M.Smy, J.T.Sobczyk, H.Sobel, F.J.P.Soler, Y.Sonoda, A.J.Speers, R.Spina, I.A.Suslov, S.Suvorov, A.Suzuki, S.Y.Suzuki, Y.Suzuki, M.Tada, S.Tairafune, S.Takayasu, A.Takeda, Y.Takeuchi, K.Takifuji, H.K.Tanaka, M.Tani, A.Teklu, V.V.Tereshchenko, N.Thamm, L.F.Thompson, W.Toki, C.Touramanis, T.Towstego, K.M.Tsui, T.Tsukamoto, M.Tzanov, Y.Uchida, M.Vagins, D.Vargas, M.Varghese, G.Vasseur, C.Vilela, E.Villa, W.G.S.Vinning, U.Virginet, T.Vladisavljevic, T.Wachala, J.G.Walsh, Y.Wang, L.Wan, D.Wark, M.O.Wascko, A.Weber, R.Wendell, M.J.Wilking, C.Wilkinson, J.R.Wilson, K.Wood, C.Wret, J.Xia, Y.-h.Xu, K.Yamamoto, T.Yamamoto, C.Yanagisawa, G.Yang, T.Yano, K.Yasutome, N.Yershov, U.Yevarouskaya, M.Yokoyama, Y.Yoshimoto, N.Yoshimura, M.Yu, R.Zaki, A.Zalewska, J.Zalipska, K.Zaremba, G.Zarnecki, X.Zhao, T.Zhu, M.Ziembicki, E.D.Zimmerman, M.Zito, S.Zsoldos Measurements of the νμ and ν-barμ-induced coherent charged pion production cross sections on 12C by the T2K experiment NUCLEAR REACTIONS 12C(ν, μ-), (ν-bar, μ+), E ∼ 0.8 GeV; measured reaction products; deduced coherent charged pion production σ in the Tokai-to-Kamioka experiment.
doi: 10.1103/PhysRevD.108.092009
2022GO04 Phys.Rev. C 105, 025502 (2022) R.Gonzalez-Jimenez, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, N.Jachowicz, G.D.Megias, K.Niewczas, A.Nikolakopoulos, J.W.Van Orden, J.M.Udias Neutrino energy reconstruction from semi-inclusive samples NUCLEAR REACTIONS 16O(ν, μ-p)E<4061 MeV; calculated σ(θ, E) with DUNE and T2K neutrino fluxes, missing energy-missing momentum trajectories. Discussing the usefulness of semi-inclusive charged-current neutrino scattering in extracting the neutrino spectrum.
doi: 10.1103/PhysRevC.105.025502
2021FR09 Phys.Rev. D 104, 073008 (2021) J.M.Franco-Patino, M.B.Barbaro, J.A.Caballero, G.D.Megias Theoretical description of semi-inclusive T2K, MINERνA and MicroBooNE neutrino-nucleus data in the relativistic plane wave impulse approximation NUCLEAR REACTIONS 40Ar(ν, X), E not given; calculated σ. MicroBooNE data sets.
doi: 10.1103/PhysRevD.104.073008
2020AM06 J.Phys.(London) G46, 124001 (2020) J.E.Amaro, M.B.Barbaro, J.A.Caballero, R.Gonzalez-Jimenez, G.D.Megias, I.Ruiz Simo Electron- versus neutrino-nucleus scattering NUCLEAR REACTIONS 12C(ν, μ-), (e-, e-'), E=1, 1.5 GeV; calculated σ(θ, E).
doi: 10.1088/1361-6471/abb128
2020CR01 Nucl.Phys. A994, 121667 (2020) Analysis of quasielastic (e, e') electromagnetic responses and scaling for nuclear matter in the relativistic mean field model
doi: 10.1016/j.nuclphysa.2019.121667
2020FR14 Phys.Rev. C 102, 064626 (2020) J.M.Franco-Patino, J.Gonzalez-Rosa, J.A.Caballero, M.B.Barbaro Semi-inclusive charged-current neutrino-nucleus cross sections in the relativistic plane-wave impulse approximation NUCLEAR REACTIONS 12C, 40Ar(ν, ν), (ν-bar, ν-bar), E<6 GeV; calculated momentum distributions, semi-inclusive cross sections, flux-averaged single-differential and double-differential inclusive cross sections for quasielastic neutrino-nucleus scattering and corresponding to experimental data from DUNE for 40Ar and T2K for 12C. Plane-wave impulse approximation using three nuclear models: relativistic Fermi gas (RFG), independent-particle shell model (IPSM), and the natural orbitals (NO) model with Lorentzian dependence of the excitation energy. Discussed off-shell effects.
doi: 10.1103/PhysRevC.102.064626
2020GO01 Phys.Rev. C 101, 015503 (2020) R.Gonzalez-Jimenez, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, N.Jachowicz, G.D.Megias, K.Niewczas, A.Nikolakopoulos, J.M.Udias Constraints in modeling the quasielastic response in inclusive lepton-nucleus scattering NUCLEAR REACTIONS 12C, 40Ar, 48Ti(e, e'), momentum transfer q=100, 200, 600, 1000, 1500 MeV; calculated vector and scalar potentials as a function of the position in the nucleus, quasielastic (QE) scaling functions, differential σ(E) by superscaling approach (SuSAv2) model and relativistic mean-field models. Comparison with the recent Jefferson Laboratory (JLab) data.
doi: 10.1103/PhysRevC.101.015503
2020IV04 Nucl.Phys. A1003, 122029 (2020) M.V.Ivanov, A.N.Antonov, J.A.Caballero Nucleon momentum distribution extracted from the experimental scaling function
doi: 10.1016/j.nuclphysa.2020.122029
2019BA15 Phys.Rev. C 99, 042501 (2019) M.B.Barbaro, J.A.Caballero, A.De Pace, T.W.Donnelly, R.Gonzalez-Jimenez, G.D.Megias Mean-field and two-body nuclear effects in inclusive electron scattering on argon, carbon, and titanium: The superscaling approach NUCLEAR REACTIONS 12C, 40Ar, 48Ti(E, E'), E=2.222 GeV; calculated double differential σ(E, θ) for quasielastic scattering, and superscaling function extracted from JLab data using superscaling (SuSAv2-MEC) model, including two-particle two-hole meson-exchange currents. Application to experimental data from MINERνA, MicroBooNE and J-PARC (T2K) collaborations.
doi: 10.1103/PhysRevC.99.042501
2019IV02 Phys.Rev. C 99, 014610 (2019) M.V.Ivanov, A.N.Antonov, G.D.Megias, J.A.Caballero, M.B.Barbaro, J.E.Amaro, I.Ruiz Simo, T.W.Donnelly, J.M.Udias Realistic spectral function model for charged-current quasielastic-like neutrino and antineutrino scattering cross sections on 12C NUCLEAR REACTIONS 12C(ν, X), (ν-bar, X), E=0-1.6 GeV muon neutrinos and antineutrinos; analyzed experimental data for double-differential, single-differential, and total integrated cross sections of charged current quasielastic (CCQE) scattering, fluxes of νμ and ν-barμ for MiniBooNE, T2K and Minerva experiments using spectral functions with and without nucleon-nucleon short-range correlations through the Jastrow method. Three different theoretical calculations using harmonic oscillator (HO), natural orbitals (NO), both including final-state interactions (FSI), and SuSAv2 based on the relativistic meanfield (RMF) model.
doi: 10.1103/PhysRevC.99.014610
2018BA35 Phys.Rev. C 98, 035501 (2018) M.B.Barbaro, A.De Pace, T.W.Donnelly, J.A.Caballero, G.D.Megias, J.W.Van Orden Asymmetric relativistic Fermi gas model for quasielastic lepton-nucleus scattering NUCLEAR REACTIONS 40Ar, 208Pb(e, e'), (ν, ν'), (ν-bar, ν-bar'), 12C, 40Ar, 208Pb(ν, μ-), (ν-bar, μ+), E(transfer)=0-500 MeV; calculated longitudinal and transverse electromagnetic, weak neutral-current, and weak charged current response functions using symmetric and asymmetric relativistic Fermi gas (SRFG and ARFG) models. Relevance to analysis of neutrino oscillation experiments.
doi: 10.1103/PhysRevC.98.035501
2017AM03 Phys.Rev. C 95, 065502 (2017) J.E.Amaro, M.B.Barbaro, J.A.Caballero, A.De Pace, T.W.Donnelly, G.D.Megias, I.Ruiz Simo Density dependence of 2p-2h meson-exchange currents
doi: 10.1103/PhysRevC.95.065502
2016SI25 Phys.Rev. C 94, 054610 (2016) I.Ruiz Simo, J.E.Amaro, M.B.Barbaro, A.De Pace, J.A.Caballero, G.D.Megias, T.W.Donnelly Emission of neutron-proton and proton-proton pairs in electron scattering induced by meson-exchange currents NUCLEAR REACTIONS 12C(e, e'np), (e, e'pp), E=961, 3595, 4621 MeV; calculated differential cross sections, transverse and longitudinal electromagnetic response functions for np and pp pair emissions using relativistic Fermi gas model with relativistic model of meson exchange currents (MECs).
doi: 10.1103/PhysRevC.94.054610
2015AN10 Phys.Rev. C 92, 025501 (2015) A.M.Ankowski, M.B.Barbaro, O.Benhar, J.A.Caballero, C.Giusti, R.Gonzalez-Jimenez, G.D.Megias, A.Meucci Estimate of the theoretical uncertainty of the cross sections for nucleon knockout in neutral-current neutrino-oxygen interactions NUCLEAR REACTIONS 16O(ν, ν')n, (ν, ν')p, (ν-bar, ν'-bar)n, (ν-bar, ν'-bar)p, E<2.0 GeV; calculated σ(E) for neutron and proton knockouts induced by neutral-current (NC) quasielastic (QE) scattering of atmospheric neutrinos and antineutrinos using relativistic plane-wave impulse approximation (RPWIA), relativistic mean-field (RMF), relativistic Green's function (RGF), and superscaling (SuSA) approaches and comparison with realistic nuclear spectral functions (SF). Relevance to ongoing and future experiments at the Super- and Hyper-Kamiokande including searches of diffuse supernova neutrinos (DSN) and sterile neutrinos in the beam of T2K experiment.
doi: 10.1103/PhysRevC.92.025501
2015GO06 Phys.Rev. C 91, 045502 (2015) R.Gonzalez-Jimenez, J.A.Caballero, T.W.Donnelly Parity violation in quasielastic electron-nucleus scattering within the relativistic impulse approximation NUCLEAR REACTIONS 12C, 16O, 40Ca(e, e), q=0.5, 1.0 GeV; calculated parity-violating quasielastic (PVQE) asymmetry, electromagnetic (EM) and longitudinal, transverse, and transverse axial interference scaling functions. Final-state interactions, nucleon off-shell effects, and current gauge ambiguities. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.045502
2015GO07 Phys.Rev. C 91, 045503 (2015) R.Gonzalez-Jimenez, J.A.Caballero, T.W.Donnelly Parity violation and dynamical relativistic effects in (e-pol, e'N) reactions
doi: 10.1103/PhysRevC.91.045503
2015IV03 Phys.Rev. C 91, 034607 (2015) M.V.Ivanov, A.N.Antonov, M.B.Barbaro, C.Giusti, A.Meucci, J.A.Caballero, R.Gonzalez-Jimenez, E.Moya de Guerra, J.M.Udias Neutral current quasielastic (anti)neutrino scattering beyond the Fermi gas model at MiniBooNE and BNL kinematics
doi: 10.1103/PhysRevC.91.034607
2014GO21 Phys.Rev. C 90, 035501 (2014) R.Gonzalez-Jimenez, G.D.Megias, M.B.Barbaro, J.A.Caballero, T.W.Donnelly Extensions of superscaling from relativistic mean field theory: The SuSAv2 model
doi: 10.1103/PhysRevC.90.035501
2014IV01 Phys.Rev. C 89, 014607 (2014) M.V.Ivanov, A.N.Antonov, J.A.Caballero, G.D.Megias, M.B.Barbaro, E.Moya de Guerra, J.M.Udias Charged-current quasielastic neutrino scattering cross sections on 12C with realistic spectral and scaling functions NUCLEAR REACTIONS 12C(ν, ν), (ν-bar, ν-bar), E=0.1-100 GeV; calculated differential σ(E) for quasielastic neutrino scattering based on impulse approximation, and realistic spectral and scaling functions. Comparison with MiniBooNE and NOMAD experimental data. Discussed role of the final-state interactions.
doi: 10.1103/PhysRevC.89.014607
2013GO13 Phys.Rev. C 88, 025502 (2013) R.Gonzalez-Jimenez, J.A.Caballero, A.Meucci, C.Giusti, M.B.Barbaro, M.V.Ivanov, J.M.Udias Relativistic description of final-state interactions in neutral-current neutrino and antineutrino cross sections
doi: 10.1103/PhysRevC.88.025502
2012AM04 Phys.Rev.Lett. 108, 152501 (2012) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly Meson-Exchange Currents and Quasielastic Antineutrino Cross Sections in the Superscaling Approximation
doi: 10.1103/PhysRevLett.108.152501
2012CA43 J.Phys.:Conf.Ser. 366, 012006 (2012) J.A.Caballero, J.E.Amaro, M.B.Barbaro, T.W.Donnelly, J.M.Udias Scaling ideas in neutrino scattering reactions: application to the MiniBooNE experiment NUCLEAR REACTIONS 12C(ν, μ), E=0.2-2 GeV; calculated CCQE (Charged-Current QuasiElastic) σ using RIA (Relativistic Impulse Approximation). Compared with RFG (Relativistic Fermi Gas), SuSA, SuSA+MEC and MiniBoone data.
doi: 10.1088/1742-6596/366/1/012006
2011AN09 Phys.Rev. C 83, 045504 (2011) A.N.Antonov, M.V.Ivanov, J.A.Caballero, M.B.Barbaro, J.M.Udias, E.Moya de Guerra, T.W.Donnelly Scaling function, spectral function, and nucleon momentum distribution in nuclei NUCLEAR REACTIONS 12C, 16O(e, e'), E at 1 GeV/c; analyzed σ, spectral function and momentum distribution, scaling function using different nuclear models based on the independent particle shell model with short-range nucleon correlations through the use of natural orbits (NOs) within the Jastrow method.
doi: 10.1103/PhysRevC.83.045504
2011ME07 Phys.Rev. C 83, 064614 (2011) A.Meucci, J.A.Caballero, C.Giusti, J.M.Udias Relativistic descriptions of quasielastic charged-current neutrino-nucleus scattering: Application to scaling and superscaling ideas NUCLEAR REACTIONS 12C(ν, μ-), E=1000, 1500, 2000 MeV for νμ; calculated inclusive quasielastic differential cross sections and scaling function using relativistic impulse approximation. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.064614
2011ME14 Phys.Rev.Lett. 107, 172501 (2011) A.Meucci, M.B.Barbaro, J.A.Caballero, C.Giusti, J.M.Udias Relativistic Descriptions of Final-State Interactions in Charged-Current Quasielastic Neutrino-Nucleus Scattering at MiniBooNE Kinematics
doi: 10.1103/PhysRevLett.107.172501
2010AM01 Phys.Rev. C 81, 014606 (2010) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, C.Maieron, J.M.Udias Meson-exchange currents and final-state interactions in quasielastic electron scattering at high momentum transfers NUCLEAR REACTIONS 12C(e, e'), E at 1, 1.3, 1.5 GeV/c; calculated transverse response function, and effects of meson-exchange currents (MEC) using continuum semirelativistic (SR) shell model and the Dirac equation based (DEB) potential for the final states.
doi: 10.1103/PhysRevC.81.014606
2010AM06 Phys.Rev. C 82, 044601 (2010) J.E.Amaro, C.Maieron, M.B.Barbaro, J.A.Caballero, T.W.Donnelly Pionic correlations and meson-exchange currents in two-particle emission induced by electron scattering NUCLEAR REACTIONS 56Fe(e, e'), E at 370, 410, 550, 1140 MeV/c; calculated 2p-2h transverse and longitudinal response and structure functions using relativistic Fermi gas (RFG) model. Pionic correlations.
doi: 10.1103/PhysRevC.82.044601
2010CA14 Phys.Rev. C 81, 055502 (2010) J.A.Caballero, M.B.Barbaro, A.N.Antonov, M.V.Ivanov, T.W.Donnelly Scaling function and nucleon momentum distribution NUCLEAR REACTIONS 12C(e, e'), E at 0.5-1.0 GeV/c; calculated superscaling function and nucleon momentum distribution using relativistic Fermi gas (RFG) model. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.055502
2009AN06 Phys.Rev. C 79, 044602 (2009) A.N.Antonov, M.V.Ivanov, M.B.Barbaro, J.A.Caballero, E.Moya de Guerra Longitudinal and transverse scaling functions within the coherent density fluctuation model. NUCLEAR REACTIONS 12C, 16O, 27Al, 56Fe, 197Au, 208Pb(e, e'), E not given; calculated longitudinal and transverse scaling functions, quasielastic scaling functions, and differential cross sections as function of energy loss in the framework of coherent density fluctuation model (CDFM). Comparison with experimental data. 12C(ν, μ-), (ν-bar, μ-), E=1 GeV; calculated differential σ using the SDFM approach.
doi: 10.1103/PhysRevC.79.044602
2009MA57 Phys.Rev. C 80, 035504 (2009) C.Maieron, J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, C.F.Williamson Superscaling of non-quasielastic electron-nucleus scattering NUCLEAR REACTIONS 12C(e, e'), E not given; analyzed differential σ and superscaling function using superscaling model for quasielastic scattering (SSM-QE).
doi: 10.1103/PhysRevC.80.035504
2009ME07 Phys.Rev. C 80, 024605 (2009) A.Meucci, J.A.Caballero, C.Giusti, F.D.Pacati, J.M.Udias Relativistic descriptions of inclusive quasielastic electron scattering: Application to scaling and superscaling ideas NUCLEAR REACTIONS 12C(e, e'), E=620, 1000, 1299, 2020 MeV; calculated σ(θ), scaling functions using the relativistic impulse approximations. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.024605
2008IV01 Phys.Rev. C 77, 034612 (2008) M.V.Ivanov, M.B.Barbaro, J.A.Caballero, A.N.Antonov, E.Moya de Guerra, M.K.Gaidarov Superscaling and charge-changing neutrino scattering from nuclei in the Δ region beyond the relativistic Fermi gas model NUCLEAR REACTIONS 12C(ν, μ-), E=1, 1.5 GeV; 12C(ν-bar, μ+), E=1 GeV; calculated coherent density fluctuation model scaling functions, σ.
doi: 10.1103/PhysRevC.77.034612
2008MA05 Phys.Rev.Lett. 100, 052502 (2008) M.C.Martinez, J.A.Caballero, T.W.Donnelly, J.M.Udias Superscaling Predictions for Neutral Current Quasielastic Neutrino-Nucleus Scattering
doi: 10.1103/PhysRevLett.100.052502
2008MA21 Phys.Rev. C 77, 064604 (2008) M.C.Martinez, J.A.Caballero, T.W.Donnelly, J.M.Udias Final-state interactions in the superscaling analysis of neutral-current quasielastic neutrino scattering NUCLEAR REACTIONS 12C, 16O, 40Ca(ν, n), (ν, p), (ν-bar, n), (ν-bar, p), E=1-2 GeV; calculated σ(θ), response functions, scaling functions. Relativistic impulse approximation.
doi: 10.1103/PhysRevC.77.064604
2007AM01 Phys.Rev. C 75, 034613 (2007) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, J.M.Udias Final-state interactions and superscaling in the semi-relativistic approach to quasielastic electron and neutrino scattering NUCLEAR REACTIONS 12C(e, e'), E=high; calculated longitudinal and transverse scaling functions, final state interaction effects. 12C(ν, μ), E=1, 1.5 GeV; calculated σ(E, θ). Semi-relativistic approach.
doi: 10.1103/PhysRevC.75.034613
2007AM05 Phys.Rev.Lett. 98, 242501 (2007) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly Quasielastic Charged-Current Neutrino-Nucleus Scattering NUCLEAR REACTIONS 12C(ν, μ-), E=0.5, 1.0, 1.5 GeV; calculated integrated cross sections for quasielastic charged-current neutrino-nucleus scattering.
doi: 10.1103/PhysRevLett.98.242501
2007AN17 Phys.Rev. C 75, 064617 (2007) A.N.Antonov, M.V.Ivanov, M.B.Barbaro, J.A.Caballero, E.Moya de Guerra, M.K.Gaidarov Superscaling and neutral current quasielastic neutrino-nucleus scattering beyond the relativistic Fermi gas model
doi: 10.1103/PhysRevC.75.064617
2006AM02 Phys.Rev. C 73, 035503 (2006) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly Superscaling and neutral current quasielastic neutrino-nucleus scattering NUCLEAR REACTIONS 12C(ν, ν'pX), (ν, ν'nX), E=1 GeV; calculated σ(E, θ), response functions, strangeness contribution.
doi: 10.1103/PhysRevC.73.035503
2006AN29 Phys.Rev. C 74, 054603 (2006) A.N.Antonov, M.V.Ivanov, M.K.Gaidarov, E.Moya de Guerra, J.A.Caballero, M.B.Barbaro, J.M.Udias, P.Sarriguren Superscaling analysis of inclusive electron scattering and its extension to charge-changing neutrino-nucleus cross sections beyond the relativistic Fermi gas approach NUCLEAR REACTIONS 12C(e, e'X), E ≈ 0.5-2 GeV; calculated σ(E, θ), scaling functions. Superscaling analysis, coherent density fluctuation model, relativistic Fermi gas model.
doi: 10.1103/PhysRevC.74.054603
2006BA17 Nucl.Phys. B(Proc.Supp.) S155, 257 (2006) M.B.Barbaro, J.E.Amaro, J.A.Caballero, T.W.Donnelly, A.Molinari, I.Sick Superscaling and Charge-changing Neutrino Cross Sections NUCLEAR REACTIONS 12C(ν, μ-), E at 1000 MeV/c; calculated σ(E, θ).
doi: 10.1016/j.nuclphysbps.2006.02.065
2006CA22 Phys.Rev. C 74, 015502 (2006) General study of superscaling in quasielastic (e, e') and (ν, μ) reactions using the relativistic impulse approximation NUCLEAR REACTIONS 12C(e, e'), E ≈ 500-2000 MeV; 12C(ν, μ), E=1 GeV; analyzed σ(E, θ), scaling and superscaling functions. Relativistic impulse approximation.
doi: 10.1103/PhysRevC.74.015502
2005AM03 Phys.Rev. C 71, 015501 (2005) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari, I.Sick Using electron scattering superscaling to predict charge-changing neutrino cross sections in nuclei NUCLEAR REACTIONS 12C(e, e'), E=1.3, 1.5 GeV; 16O(e, e'), E=0.88 GeV; analyzed σ(E, θ); deduced electromagnetic response. 12C(ν, μ), E=1 GeV; calculated σ(E, θ). Superscaling analysis.
doi: 10.1103/PhysRevC.71.015501
2005AM07 Nucl.Phys. A753, 189 (2005) J.E.Amaro, J.A.Caballero, T.W.Donnelly, F.K.Tabatabaei Final-state interaction and recoil polarization in (e, e'p) reactions: comparison with the polarized target case NUCLEAR REACTIONS 40Ca(e, e'p), E=high; calculated proton knockout σ(E, θ), recoil polarization, final state interaction effects. Comparison of polarized and unpolarized target data.
doi: 10.1016/j.nuclphysa.2005.02.077
2005AM09 Phys.Rev. C 71, 065501 (2005) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, C.Maieron Semirelativistic description of quasielastic neutrino reactions and superscaling in a continuum shell model NUCLEAR REACTIONS 12C, 16O(ν, μ-), E=1, 1.5 GeV; calculated σ(E, θ), response functions, scaling and superscaling behaviors.
doi: 10.1103/PhysRevC.71.065501
2005AM10 Ann.Phys.(New York) 319, 123 (2005) J.E.Amaro, M.B.Barbaro, J.A.Caballero Skewed recoil polarization in (e, e'p) reactions from polarized nuclei NUCLEAR REACTIONS 39K(polarized e, e'p), E not given; calculated polarization asymmetries, polarization transfer, related observables. Polarized target.
doi: 10.1016/j.aop.2005.03.004
2005CA54 Phys.Rev.Lett. 95, 252502 (2005) J.A.Caballero, J.E.Amaro, M.B.Barbaro, T.W.Donnelly, C.Maieron, J.M.Udias Superscaling in Charged Current Neutrino Quasielastic Scattering in the Relativistic Impulse Approximation NUCLEAR REACTIONS 12C, 16O(ν, μ-), E=1-2 GeV; calculated σ(E, θ), scaling functions. Relativistic impulse approximation.
doi: 10.1103/PhysRevLett.95.252502
2005MA01 Nucl.Phys. B(Proc.Supp.) S139, 226 (2005) C.Maieron, M.C.Martinez, J.A.Caballero, J.M.Udias Final state interaction effects in neutrino-nucleus quasielastic scattering NUCLEAR REACTIONS 16O(ν, μ), E=200, 500, 1000 MeV; calculated σ(E), final state interaction effects.
doi: 10.1016/j.nuclphysbps.2004.11.224
2005MO05 Nucl.Phys. A748, 112 (2005) A.M.Moro, J.A.Caballero, J.Gomez-Camacho Uncorrelated scattering approximation revisited NUCLEAR REACTIONS 58Ni(d, d), E=80 MeV; calculated σ(θ). 58Ni(d, X), E=80 MeV; calculated breakup σ. Uncorrelated scattering approximation, comparison with coupled channels method.
doi: 10.1016/j.nuclphysa.2004.10.030
2005RY02 Nucl.Phys. A755, 511c (2005) J.Ryckebusch, P.Lava, M.C.Martinez, J.M.Udias, J.A.Caballero Nuclear Transparencies in Relativistic A(e, e'p) Models NUCLEAR REACTIONS 56Fe(e, e'p), E not given; calculated nuclear transparency vs momentum transfer.
doi: 10.1016/j.nuclphysa.2005.03.065
2004LA13 Phys.Lett. B 595, 177 (2004) P.Lava, M.C.Martinez, J.Ryckebusch, J.A.Caballero, J.M.Udias Nuclear transparencies in relativistic A(e, e'p) models NUCLEAR REACTIONS 12C, 28Si, 56Fe, 208Pb(e, e'p), E=high; calculated nuclear transparencies. Relativistic models, comparisons with data.
doi: 10.1016/j.physletb.2004.04.088
2004MA22 Phys.Rev. C 69, 034604 (2004) M.C.Martinez, J.R.Vignote, J.A.Caballero, T.W.Donnelly, E.Moya de Guerra, J.M.Udias Analysis of polarized 16O(e(pol), e'p(pol)) observables within the relativistic distorted wave impulse approximation NUCLEAR REACTIONS 16O(polarized e, e'p), E=high; analyzed transferred polarization asymmetries, response functions; deduced dynamical effects. Relativistic PWIA.
doi: 10.1103/PhysRevC.69.034604
2004TA18 Phys.Rev. C 69, 064607 (2004) F.K.Tabatabaei, J.E.Amaro, J.A.Caballero Induced nucleon polarization and meson-exchange currents in (e, e'p) reactions NUCLEAR REACTIONS 12C, 16O(e, e'p), E=high; calculated induced polarization asymmetry, meson-exchange current contributions. Semirelativistic distorted-wave model, comparison with data.
doi: 10.1103/PhysRevC.69.064607
2004VI11 Phys.Rev. C 70, 044608 (2004) J.R.Vignote, M.C.Martinez, J.A.Caballero, E.Moya de Guerra, J.M.Udias A(e(pol), e'p(pol))B responses: From bare nucleons to complex nuclei NUCLEAR REACTIONS 16O, 40Ca(polarized e, e'p), E=2445 MeV; calculated σ(p), analyzing powers, induced polarization, related observables. Relativistic DWBA, comparison of factorized and unfactorized approaches.
doi: 10.1103/PhysRevC.70.044608
2003AM05 Nucl.Phys. A723, 181 (2003) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Delta-isobar relativistic meson exchange currents in quasielastic electron scattering
doi: 10.1016/S0375-9474(03)01269-7
2003AM06 Phys.Rev. C 68, 014604 (2003) J.E.Amaro, M.B.Barbaro, J.A.Caballero, F.K.Tabatabaei Semirelativistic meson-exchange currents in (e, e') and (e, e'p) reactions NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated response functions, asymmetries. Semirelativistic meson-exchange currents.
doi: 10.1103/PhysRevC.68.014604
2003MA58 Phys.Rev. C 68, 048501 (2003) C.Maieron, M.C.Martinez, J.A.Caballero, J.M.Udias Nuclear model effects in charged-current neutrino-nucleus quasielastic scattering NUCLEAR REACTIONS 16O(ν, μ-X), E=0.2-1 GeV; calculated quasielastic scattering σ, muon spectra, final state interaction effects. Relativistic shell model, comparison with data.
doi: 10.1103/PhysRevC.68.048501
2003TA19 Phys.Rev. C 68, 034611 (2003) F.K.Tabatabaei, J.E.Amaro, J.A.Caballero Meson-exchange currents in (e, e'p) recoil polarization observables NUCLEAR REACTIONS 16O(polarized e, e'p), E=high; calculated polarized response functions, polarization transfer observables, meson-exchange current effects.
doi: 10.1103/PhysRevC.68.034611
2002AM01 Nucl.Phys. A697, 388 (2002) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Relativistic Pionic Effects in Quasielastic Electron Scattering NUCLEAR REACTIONS 40Ca(e, e'), E not given; calculated transverse and longitudinal response functions; deduced reaction mechanism features.
doi: 10.1016/S0375-9474(01)01253-2
2002AM09 Eur.Phys.J. A 15, 421 (2002) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Momentum distribution of relativistic nuclei with Hartree-Fock mesonic correlations
doi: 10.1140/epja/i2002-10080-2
2002AM12 Phys.Rep. 368, 317 (2002) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Gauge and Lorentz invariant one-pion exchange currents in electron scattering from a relativistic Fermi gas
doi: 10.1016/S0370-1573(02)00195-3
2002MA51 Nucl.Phys. A707, 83 (2002) M.C.Martinez, J.A.Caballero, T.W.Donnelly RPWIA Analysis of Dynamical Relativistic Contributions in 16O(e(pol), e'p(pol)) Reactions NUCLEAR REACTIONS 16O(polarized e, e'p), E=high; calculated response functions, polarization transfer asymmetries, relativistic effects. Relativistic PWIA.
doi: 10.1016/S0375-9474(02)00878-3
2002MA52 Nucl.Phys. A707, 121 (2002) M.C.Martinez, J.A.Caballero, T.W.Donnelly Kinematical Relativistic Effects in (e(pol), e'N(pol)) Reactions NUCLEAR REACTIONS 16O(e, e'p), E=high; calculated polarized and unpolarized response functions, transferred polarization asymmetry. Relativistic PWIA.
doi: 10.1016/S0375-9474(02)00879-5
2001CA32 Nucl.Phys. A689, 449c (2001) J.A.Caballero, M.C.Martinez, E.Moya de Guerra, J.M.Udias, J.E.Amaro, T.W.Donnelly Role of Relativity in Electron Scattering: Kinematical versus dynamical effects NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated longitudinal-transverse response, asymmetries; deduced relativistic effects.
doi: 10.1016/S0375-9474(01)00876-4
2001MO22 Nucl.Phys. A689, 547c (2001) A.M.Moro, J.A.Caballero, J.Gomez-Camacho The Uncorrelated Scattering Approximation for the Scattering of Weakly Bound Systems
doi: 10.1016/S0375-9474(01)00901-0
2001MO38 Nucl.Phys. A695, 143 (2001) A.M.Moro, J.A.Caballero, J.Gomez-Camacho Uncorrelated Scattering Approximation for the Scattering and Breakup of Weakly Bound Nuclei on Heavy Targets NUCLEAR REACTIONS 58Ni(d, d), E=21.6, 56, 80 MeV; calculated σ(θ). Uncorrelated scattering approximation, comparisons with data.
doi: 10.1016/S0375-9474(01)01102-2
2001UD01 Phys.Rev. C64, 024614 (2001) J.M.Udias, J.A.Caballero, E.Moya de Guerra, J.R.Vignote, A.Escuderos Relativistic Mean Field Approximation to the Analysis of 16O(e, e'p)15N Data at |Q2| ≤ 0.4 (GeV/c)2 NUCLEAR REACTIONS 16O(e, e'p), E ≈ 300-600 MeV; analyzed σ(E), response functions, related data; deduced relativistic effects. Relativistic DWIA.
doi: 10.1103/PhysRevC.64.024614
1999AL16 Nucl.Phys. A651, 277 (1999) W.M.Alberico, M.B.Barbaro, S.M.Bilenky, J.A.Caballero, C.Giunti, C.Maieron, E.Moya de Guerra, J.M.Udias Strange Form Factors of the Proton: A new analysis of the ν(ν-bar) data of the BNL-734 experiment
doi: 10.1016/S0375-9474(99)00142-6
1999AM06 Phys.Rev. C60, 014602 (1999) J.E.Amaro, A.M.Lallena, J.A.Caballero Analysis of Meson Exchange and Isobar Currents in (e, e'p) Reactions from 16O NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated response functions; deduced meson exchange current, isobar current effects.
doi: 10.1103/PhysRevC.60.014602
1999AM10 Nucl.Phys. A657, 161 (1999) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Relativistic Effects in Electromagnetic Nuclear Responses in the Quasi-Elastic Delta Region NUCLEAR REACTIONS 1H(e, e'), E(cm)=1100-1400 MeV; calculated transverse σ. 12C(e, e'X), E=620, 1108 MeV; calculated σ(θ), electromagnetic response functions; deduced resonance role. Relativistic Fermi Gas model.
doi: 10.1016/S0375-9474(99)00334-6
1999UD01 Phys.Rev.Lett. 83, 5451 (1999) J.M.Udias, J.A.Caballero, E.Moya de Guerra, J.E.Amaro, T.W.Donnelly Quasielastic Scattering from Relativistic Bound Nucleons: Transverse-longitudinal response NUCLEAR REACTIONS 16O(e, e'p), E=2445 MeV; calculated σ(E, θ), transverse-longitudinal response, left-right asymmetry; deduced relativistic effects.
doi: 10.1103/PhysRevLett.83.5451
1998AL28 Phys.Lett. 438B, 9 (1998) W.M.Alberico, M.B.Barbaro, S.M.Bilenky, J.A.Caballero, C.Giunti, C.Maieron, E.Moya de Guerra, J.M.Udias The Ratio of p and n Yields in NC ν(ν-bar) Nucleus Scattering and Strange Form Factors of the Nucleon
doi: 10.1016/S0370-2693(98)01043-0
1998AM11 Nucl.Phys. A643, 349 (1998) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Relativistic Effects in Electromagnetic Meson-Exchange Currents for One-Particle Emission Reactions
doi: 10.1016/S0375-9474(98)00569-7
1998CA13 Nucl.Phys. A632, 323 (1998) J.A.Caballero, T.W.Donnelly, E.Moya de Guerra, J.M.Udias Analysis of Factorization in (e, e'p) Reactions: A survey of the relativistic plane wave impulse approximation NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated σ(E, θ), response functions; deduced role of negative energy components. Fully relativistic analysis.
doi: 10.1016/S0375-9474(97)00817-8
1998CA46 Nucl.Phys. A643, 189 (1998) J.A.Caballero, T.W.Donnelly, E.Moya de Guerra, J.M.Udias Relativistic Current Densities for Bound Spin-Orbit Partners and the Longitudinal-Transverse Response in (e, e'p) Processes NUCLEAR STRUCTURE 16O, 40Ca, 208Pb; calculated orbitals baryonic, scalar, vector current densities. Relativistic bound orbitals. NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated longitudinal-transverse response functions; deduced negative-energy projections role.
doi: 10.1016/S0375-9474(98)00486-2
1997AL21 Nucl.Phys. A623, 471 (1997) W.M.Alberico, M.B.Barbaro, S.M.Bilenky, J.A.Caballero, C.Giunti, C.Maieron, E.Moya de Guerra, J.M.Udias Inelastic ν and (ν-bar) Scattering on Nuclei and ' Strangeness ' of the Nucleon NUCLEAR REACTIONS 12C(ν, ν'X), (ν-bar, ν-bar'X), E=200-1000 GeV; calculated differential σ vs ejected nucleon energy, proton to neutron production ratio, asymmetry related quantity; deduced nucleon strangeness role. Shell, Fermi gas models.
doi: 10.1016/S0375-9474(97)00416-8
1996AM04 Nucl.Phys. A602, 263 (1996) J.E.Amaro, J.A.Caballero, T.W.Donnelly, A.M.Lallena, E.Moya de Guerra, J.M.Udias Parity Violation in Quasielastic Electron Scattering from Closed-Shell Nuclei NUCLEAR REACTIONS 16O, 40Ca, 208Pb(e, e'X), E not given; calculated response functions, parity-violating asymmetries sensitivity to nucleon form factors.
doi: 10.1016/0375-9474(96)00034-6
1996AM11 Nucl.Phys. A611, 163 (1996) J.E.Amaro, J.A.Caballero, T.W.Donnelly, E.Moya de Guerra Inclusive Quasielastic Scattering of Polarized Electrons from Polarized Nuclei NUCLEAR STRUCTURE 39K; calculated inclusive quasielastic response functions. Polarized electrons scattered by polarized nuclei, plane wave impulse approximation, distorted wave in continuum shell model.
doi: 10.1016/S0375-9474(96)00334-X
1996UD01 Phys.Rev. C53, R1488 (1996) J.M.Udias, P.Sarriguren, E.Moya de Guerra, J.A.Caballero Relativistic Analysis of the 208Pb(e, e'p)207Tl Reaction at High Momentum NUCLEAR REACTIONS 208Pb(e, e'p), E not given; analyzed data; deduced missing momentum dependence of relativistic, nonrelativistic treatments.
doi: 10.1103/PhysRevC.53.R1488
1995CA41 Ann.Phys.(New York) 239, 351 (1995) J.A.Caballero, E.Garrido, E.Moya de Guerra, P.Sarriguren, J.M.Udias Spin Dependent Momentum Distributions in Deformed Nuclei NUCLEAR STRUCTURE 21,20Ne, 37,36Ar; calculated binding energies, proton, mass quadrupole moments, rms radii, moments of inertia, momentum distribution, transition densities.
doi: 10.1006/aphy.1995.1038
1995GA05 Nucl.Phys. A584, 256 (1995) E.Garrido, J.A.Caballero, E.Moya de Guerra, P.Sarriguren, J.M.Udias Probing Deformed Orbitals with A(e, e'N)B Reactions NUCLEAR STRUCTURE 37Ar, 37K; calculated binding energies, charge rms radii, μ, quadrupole moments, moments of inertia, decoupling parameters. NUCLEAR REACTIONS 37Ar(polarized e, e'n), 37K(polarized e, e'p), E not given; calculated response functions, asymmetries; deduced deformed orbitals probing features. PWIA, DWIA approaches.
doi: 10.1016/0375-9474(94)00512-L
1995UD01 Phys.Rev. C51, 3246 (1995) J.M.Udias, P.Sarriguren, E.Moya de Guerra, E.Garrido, J.A.Caballero Relativistic Versus Nonrelativistic Optical Potential in A(e, e'p)B Reactions NUCLEAR REACTIONS 40Ca, 208Pb(e, e'p), E not given; calculated reduced σ, ratios for relativistic, nonrelativistic optical potentials; deduced relativistic nucleon current depletion role.
doi: 10.1103/PhysRevC.51.3246
1994CA27 Nucl.Phys. A577, 528 (1994) J.A.Caballero, T.W.Donnelly, G.I.Poulis, E.Garido, E.Moya de Guerra Polarized Spectral Function of Deformed Nuclei Modeling the Reaction 21Ne(pol)(e(pol), e'n)20Ne NUCLEAR REACTIONS 21Ne(polarized e, e'n), (e, e'n), E not given; calculated differential σ, asymmetry, polarized spectral function. Polarized target.
doi: 10.1016/0375-9474(94)90932-6
1993CA11 Nucl.Phys. A555, 709 (1993) J.A.Caballero, T.W.Donnelly, G.I.Poulis Scattering of Polarized Electrons from Polarized Targets: Coincidence reactions and prescriptions for polarized half-off-shell single-nucleon cross sections NUCLEAR REACTIONS 39K, 7Li(polarized e, e'p), 7Li(polarized e, e'n), E not given; calculated polarization ratio vs inbound nucleon momentum. Polarized electrons, polarized targets, plane wave impulse approximations.
doi: 10.1016/0375-9474(93)90503-P
1993LA16 Nucl.Phys. A560, 811 (1993) J.B.J.M.Lanen, H.P.Blok, H.J.Bulten, J.A.Caballero, E.Moya de Guerra, M.N.Harakeh, G.J.Kramer, L.Lapikas, M.van der Schaar, P.K.A.de Witt Huberts, A.Zondervan The (e, e'p) Reaction on 142Nd and 146Nd: A search for deformation effects NUCLEAR REACTIONS 142,146Nd(e, e'p), E=261, 450 MeV; measured spectra. 141,145Pr levels deduced momentum distributions, deformation effects, C2S. CDWIA calculations, Nilsson plus BCS model calculations.
doi: 10.1016/0375-9474(93)90172-T
1993UD01 Phys.Rev. C48, 2731 (1993) J.M.Udias, P.Sarriguren, E.Moya de Guerra, E.Garrido, J.A.Caballero Spectroscopic Factors in 40Ca and 208Pb from (e, e'p): Fully relativistic analysis NUCLEAR REACTIONS 208Pb, 40Ca(e, e'p), E=375 MeV; analyzed reduced σ vs missing momentum. 208Pb, 40Ca deduced inner shell spectroscopic factors. Fully relativistic analysis.
doi: 10.1103/PhysRevC.48.2731
1991MO12 Nucl.Phys. A529, 68 (1991) E.Moya de Guerra, P.Sarriguren, J.A.Caballero, M.Casas, D.W.L.Sprung Momentum Distributions from Deformed Hartree-Fock Calculations NUCLEAR STRUCTURE 142,146,150Nd; calculated deformation parameters, rms radii, quadrupole moments, nucleon momentum distributions. Density-dependent Hartree-Fock calculations, deformed nuclei.
doi: 10.1016/0375-9474(91)90786-6
1991ZA11 Ann.Phys.(New York) 212, 402 (1991) L.Zamick, D.C.Zheng, S.J.Lee, J.A.Caballero, E.Moya de Guerra Comparison of the Nilsson and Skyrme Hartree-Fock Results for the Properties of Highly Deformed States in Nuclei NUCLEAR STRUCTURE 8Be, 12C, 16O, 40Ca; calculated levels. 40Ca; calculated deformation parameter, binding energies. Nilsson, Skyrme Hartree-Fock models.
doi: 10.1016/0003-4916(91)90121-N
1990CA07 Nucl.Phys. A509, 117 (1990) J.A.Caballero, E.Moya de Guerra Momentum Distributions in Axially Symmetric Deformed Nuclei: The Nilsson model NUCLEAR STRUCTURE 20Ne, 150,146,142Nd; calculated intrinsic mass quadrupole moments vs deformation, charge rms radii, Nilsson model.
doi: 10.1016/0375-9474(90)90377-X
1988MO04 Nucl.Phys. A477, 445 (1988) E.Moya de Guerra, J.A.Caballero, P.Sarriguren Effects of Nuclear Deformation in Quasi-Elastic Electron Scattering NUCLEAR REACTIONS 28Si(e, e'p), E not given; analyzed proton momentum distribution; deduced deformation role. PWIA.
doi: 10.1016/0375-9474(88)90350-8
1987MO30 J.Phys.(Paris), Colloq.C-2, 295 (1987) E.Moya De Guerra, J.A.Caballero, P.Sarriguren Momentum Distributions in Deformed Nuclei NUCLEAR REACTIONS 28Si(e, e'p), E not given; calculated proton momentum distribution.
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