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NSR database version of April 11, 2024.

Search: Author = J.M.Udias

Found 77 matches.

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2024GA09      Phys.Rev. C 109, 024608 (2024)

J.Garcia-Marcos, T.Franco-Munoz, R.Gonzalez-Jimenez, A.Nikolakopoulos, N.Jachowicz, J.M.Udias

Towards a more complete description of nucleon distortion in lepton-induced single-pion production at low-Q2

doi: 10.1103/PhysRevC.109.024608
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2024YU02      Phys.Lett. B 849, 138452 (2024)

Z.Yue, A.N.Andreyev, A.E.Barzakh, I.N.Borzov, J.G.Cubiss, A.Algora, M.Au, M.Balogh, S.Bara, R.A.Bark, C.Bernerd, M.J.G.Borge, D.Brugnara, K.Chrysalidis, T.E.Cocolios, H.De Witte, Z.Favier, L.M.Fraile, H.O.U.Fynbo, A.Gottardo, R.Grzywacz, R.Heinke, A.Illana, P.M.Jones, D.S.Judson, A.Korgul, U.Koster, M.Labiche, L.Le, R.Lica, M.Madurga, N.Marginean, B.Marsh, C.Mihai, E.Nacher, C.Neacsu, C.Nita, B.Olaizola, J.N.Orce, C.A.A.Page, R.D.Page, J.Pakarinen, P.Papadakis, G.Penyazkov, A.Perea, M.Piersa-Silkowska, Zs.Podolyak, S.D.Prosnyak, E.Reis, S.Rothe, M.Sedlak, L.V.Skripnikov, C.Sotty, S.Stegemann, O.Tengblad, S.V.Tolokonnikov, J.M.Udias, P.Van Duppen, N.Warr, W.Wojtaczka

Magnetic moments of thallium isotopes in the vicinity of magic N=126

NUCLEAR MOMENTS 207,209Tl; measured frequencies; deduced magnetic dipole moments. Comparison with the self-consistent theory of finite Fermi systems based on the energy density functional. The in-source laser resonance-ionization spectroscopy technique with the Laser Ion Source and Trap (LIST) at ISOLDE (CERN).

doi: 10.1016/j.physletb.2024.138452
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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
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2023FR07      Phys.Rev. C 108, 064608 (2023)

T.Franco-Munoz, J.Garcia-Marcos, R.Gonzalez-Jimenez, J.M.Udias

Relativistic two-body currents for one-nucleon knockout in electron-nucleus scattering

doi: 10.1103/PhysRevC.108.064608
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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
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2022NI07      Phys.Rev. C 105, 054603 (2022)

A.Nikolakopoulos, R.Gonzalez-Jimenez, N.Jachowicz, K.Niewczas, F.Sanchez, J.M.Udias

Benchmarking intranuclear cascade models for neutrino scattering with relativistic optical potentials

NUCLEAR REACTIONS 16O, 12C, 40Ca(ν, p), E=21-1040 MeV; calculated σ(E). 16O() 12C(n, n'), (p, p), E=10-1000 MeV; calculated σ(E). 40Ca(e, ep), E>400 MeV; calculated σ(θ, E). Distorted-wave impulse approximation (RDWIA) calculation that uses the real part of an optical potential (rROP) and simulations with NEUT cascade model. Comparison to experimental data.

doi: 10.1103/PhysRevC.105.054603
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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
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2019GO23      Phys.Rev. C 100, 045501 (2019)

R.Gonzalez-Jimenez, A.Nikolakopoulos, N.Jachowicz, J.M.Udias

Nuclear effects in electron-nucleus and neutrino-nucleus scattering within a relativistic quantum mechanical framework

NUCLEAR REACTIONS 12C(e, e'), (e, e'π), E<140 MeV; 12C(ν, ν'), (ν, ν'π), E<3 GeV; calculated differential σ(E) for quasielastic scattering and single-pion production (SPP); deduced impact of the description of the knockout nucleon on these cross sections. Fully relativistic and quantum mechanical framework, with models based on impulse approximation, and the first-order Born approximation (RPWIA, Pauli-blocked RPWIA and RPWIA with a cutoff), with the target nucleus described by the relativistic mean-field (RMF) model. Comparison with experimental data.

doi: 10.1103/PhysRevC.100.045501
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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
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2019NI09      Phys.Rev.Lett. 123, 052501 (2019)

A.Nikolakopoulos, N.Jachowicz, N.Van Dessel, K.Niewczas, R.Gonzalez-Jimenez, J.M.Udias, V.Pandey

Electron versus Muon Neutrino Induced Cross Sections in Charged Current Quasielastic Processes

NUCLEAR REACTIONS 40Ar, 12C(ν, ν), E=200 MeV; calculated σ.

doi: 10.1103/PhysRevLett.123.052501
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2019OL02      Phys.Rev. C 99, 024321 (2019)

B.Olaizola, L.M.Fraile, H.Mach, F.Nowacki, A.Poves, A.Aprahamian, J.A.Briz, J.Cal-Gonzalez, D.Ghita, U.Koster, W.Kurcewicz, S.R.Lesher, D.Pauwels, E.Picado, D.Radulov, G.S.Simpson, J.M.Udias

Properties of low-lying states in 65Co from lifetime measurements

RADIOACTIVITY 65Fe(β-)[from U(p, F), E=1.4 GeV followed by ionization using a Resonance Ionization Laser Ion Source (RILIS) at ISOLDE-CERN facility]; measured Eγ, Iγ, βγ- and γγ-coin, half-life of 65Fe g.s. from decay curves for γ rays, level half-lives by βγ(t) and βγγ(t) using fast timing technique. 65Co; deduced levels, J, π, β feedings, logft, B(M1), and B(E2). Comparison with large-scale shell model calculations.

NUCLEAR STRUCTURE 65Co; calculated levels, J, π, occupation numbers using shell-model with LNPS effective interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.99.024321
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2018PI07      Acta Phys.Pol. B49, 523 (2018)

M.Piersa, A.Korgul, L.M.Fraile, J.Benito, E.Adamska, R.Alvarez, A.E.Barzakh, G.Benzoni, T.Berry, M.J.G.Borge, M.Carmona, K.Chrysalidis, G.Correia, C.Costache, T.Day Goodacre, D.V.Fedorov, V.N.Fedosseev, G.Fernandez-Martinez, M.Fila, D.Galaviz, R.Grzywacz, C.Henrich, A.Illana, Z.Janas, K.Johnston, V.Karanyonchev, M.Kicinska-Habior, R.Lica, M.Madurga, I.Marroquin, B.Marsh, C.Martinez, C.Mazzocchi, K.Miernik, R.Mihai, B.Olaizola, S.Paulaskalas, J.-M.Regis, S.Rothe, V.Sanchez-Tembleque, G.Simpson, Ch.Sotty, L.Stan, M.Stanoiu, M.Stryjczyk, A.Turturica, J.M.Udias, V.Vedia, A.Villa, W.B.Walters

Investigation of Low-lying States in 133Sn Populated in the β Decay of 133In Using Isomer-selective Laser Ionization

RADIOACTIVITY 133In(β-)[from ISOLDE facility, where 1.4 GeV protons are directed on uranium carbide target]; measured Eβ, Iβ, β-gated γ-ray spectra using isomer selective ionization of ISOLDE facility LDE RILIS with clear distinction between decaying gs (9/2+) and isomer (1/2-); deduced, identified γ-rays following 133In to 133Sn as βγγ coin with 513 keV transition; deduced levels, J, π participating in 133In β-decay; deduced consistency with previous results on low-lying structure in 133Sn.

doi: 10.5506/aphyspolb.49.523
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2017OL03      Phys.Rev. C 95, 061303 (2017)

B.Olaizola, L.M.Fraile, H.Mach, A.Poves, F.Nowacki, A.Aprahamian, J.A.Briz, J.Cal-Gonzalez, D.Ghita, U.Koster, W.Kurcewicz, S.R.Lesher, D.Pauwels, E.Picado, D.Radulov, G.S.Simpson, J.M.Udias

Search for shape-coexisting 0+ states in 66Ni from lifetime measurements

RADIOACTIVITY 66Co(β-)[from 66Mn -> 66Fe decay, 66Mn from U(p, F), E=1.4 GeV at ISOLDE-CERN facility using RILIS]; measured Eγ, half-life of an excited 0+ state by βγγ(t) method using LaBr3(Ce) crystals and two HPGe detectors for γ rays, and a fast plastic scintillator for beta particles. 66Ni; deduced levels, B(E2). Comparison with large-scale shell model calculations, and with previous experimental data.

doi: 10.1103/PhysRevC.95.061303
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2017OL08      J.Phys.(London) G44, 125103 (2017)

B.Olaizola, L.M.Fraile, H.Mach, A.Poves, A.Aprahamian, J.A.Briz, J.Cal-Gonzalez, D.Ghita, U.Koster, W.Kurcewicz, S.R.Lesher, D.Pauwels, E.Picado, D.Radulov, G.S.Simpson, J.M.Udias

Beta decay of 66Mn to the N = 40 nucleus 66Fe

RADIOACTIVITY 66Mn(β-), (β-n) [from U(p, X), E=1.4 GeV]; measured decay products, Eγ, Iγ; deduced 66Fe T1/2, γ-ray energies and intensities, B(E2), B(M1) limits. Comparison with shell model calculations.

doi: 10.1088/1361-6471/aa915e
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2016IV03      Phys.Rev. C 94, 014608 (2016)

M.V.Ivanov, J.R.Vignote, R.Alvarez-Rodriguez, A.Meucci, C.Giusti, J.M.Udias

Global relativistic folding optical potential and the relativistic Green's function model

NUCLEAR REACTIONS 12C(p, p), E=20-1040 MeV; analyzed σ(θ, E) data using global relativistic folding optical potential (GRFOP) fits; deduced differential cross sections, analyzing powers, and the spin rotation parameter. 12C(e, e), E=150-747 MeV; 12C(ν, μ-), (ν-bar, μ-), E=3-100 GeV muon neutrinos; 12C(ν, ν), (ν-bar, ν-bar), E=0.2-2.5 GeV; analyzed σ(E) and σ(θ) data from MiniBooNE collaboration using new GRFOP potential within the relativistic Green's function model.

doi: 10.1103/PhysRevC.94.014608
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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
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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
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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
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2013OL06      Phys.Rev. C 88, 044306 (2013)

B.Olaizola, L.M.Fraile, H.Mach, A.Aprahamian, J.A.Briz, J.Cal-Gonzalez, D.Ghita, U.Koster, W.Kurcewicz, S.R.Lesher, D.Pauwels, E.Picado, A.Poves, D.Radulov, G.S.Simpson, J.M.Udias

β- decay of 65Mn to 65Fe

RADIOACTIVITY 65Mn(β-), (β-n)[from U(p, X), E=1.4 GeV, RILIS]; measured Eγ, Iγ, Eβ, βγ-, βγγ-, γγ-coin, βγγ(t), half-life of 65Mn ground state, half-lives of 65Fe levels by fast timing, β-delayed neutron emission probability Pn at ISOLDE, CERN facility. 65Fe; deduced levels, isomer, J, π, multipolarity, B(M1), B(E1), B(E2), β feedings, logft. 64Fe, 64Co, 65mFe, 65Ni(β-); measured Eγ, Iγ of selected γ rays to deduce ground state β feeding in the decay of 65Mn to 65Fe. Comparison with shell-model calculations. 64Fe; deduced levels populated by β-n decay mode. Systematics of energies and B(E2) values of first 2+ states in Z=24, 26, 28, N=34-46 nuclei.

doi: 10.1103/PhysRevC.88.044306
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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
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2012CO25      J.Phys.:Conf.Ser. 381, 012101 (2012)

J.C.Cornejo, J.L.Herraiz, A.Camsonne, A.Saha, J.M.Udias, G.Urciuoli, J.R.Vignote, K.A.Aniol, for the Jefferson Lab Hall A Collaboration

Quasi elastic cross sections for the 209Bi(e, e'p)208Pb reaction: Jefferson Lab experiment E06007

NUCLEAR REACTIONS 209Bi(e, e'p), E=2.652 GeV; measured reaction products; deduced σ(θ). Compared with RDWIA calculations of Madrid group.

doi: 10.1088/1742-6596/381/1/012101
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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
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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
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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
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2011MO35      J.Phys.:Conf.Ser. 312, 092044 (2011)

O.Moreno, P.Sarriguren, E.Moya de Guerra, J.M.Udias, T.W.Donnelly, I.Sick

Neutron densities from parity-violating elastic electron scattering

NUCLEAR STRUCTURE 12C, 208Pb; calculated parity-violation asymmetry vs transferred momentum in elastic scattering of polarized electrons using HF+BCS.

doi: 10.1088/1742-6596/312/9/092044
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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
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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
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2009MO35      Nucl.Phys. A828, 306 (2009)

O.Moreno, P.Sarriguren, E.Moya de Guerra, J.M.Udias, T.W.Donnelly, I.Sick

Nuclear isospin mixing and elastic parity-violating electron scattering

NUCLEAR REACTIONS 12C, 24Mg, 28Si, 32S(e, e), E=400, 1000 MeV; analyzed σ(θ, E), parity-violating asymmetry, related features using a self consistent axially symmetric mean field approximation with density dependent effective two body Skyrme interactions. Plane- and distorted-wave Born approximations.

doi: 10.1016/j.nuclphysa.2009.07.011
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2008FE09      Phys.Lett. B 664, 57 (2008)

C.Fernandez-Ramirez, M.C.Martinez, J.R.Vignote, J.M.Udias

Spin asymmetry for the 16O(γ(pol), π-p) reaction in the Δ(1232) region within an effective Lagrangian approach

NUCLEAR REACTIONS 16O(polarized γ, π-p), E≈300 MeV; calculated spin asymmetry. Comparison with data.

doi: 10.1016/j.physletb.2008.05.003
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2008FE13      Phys.Rev. C 77, 065212 (2008)

C.Fernandez-Ramirez, E.Moya de Guerra, A.Udias, J.M.Udias

Properties of nucleon resonances by means of a genetic algorithm

doi: 10.1103/PhysRevC.77.065212
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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
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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
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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
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2007DA29      Phys.Rev. C 76, 044005 (2007)

E.M.Darwish, C.Fernandez-Ramirez, E.Moya de Guerra, J.M.Udias

Helicity dependence and contribution to the Gerasimov-Drell-Hearn sum rule of the γ(pol) d(pol) → π NN reaction channels in the energy region from threshold up to the Δ(1232) resonance

doi: 10.1103/PhysRevC.76.044005
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2007FE06      Eur.Phys.J. A 31, 572 (2007)

C.Fernandez-Ramirez, E.Moya de Guerra, J.M.Udias

Analysis of the quadrupole deformation of Δ(1232) within an effective Lagrangian model for pion photoproduction from the nucleon

NUCLEAR STRUCTURE 1n, 1H; analyzed pion photoproduction data for quadrupole deformation of the Δ(1232) through the E2/M1 ratio.

doi: 10.1140/epja/i2006-10198-1
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2006AN12      Phys.Rev. C 73, 047302 (2006), Erratum Phys.Rev. C 73, 059901 (2006)

A.N.Antonov, M.V.Ivanov, M.K.Gaidarov, E.Moya de Guerra, P.Sarriguren, J.M.Udias

Scaling functions and superscaling in medium and heavy nuclei

NUCLEAR STRUCTURE 62Ni, 82Kr, 118Sn, 197Au; calculated scaling functions. Coherent density fluctuation model, relativistic Fermi gas model, deformed self-consistent mean-field calculations.

doi: 10.1103/PhysRevC.73.047302
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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
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2006FE03      Phys.Rev. C 73, 042201 (2006)

C.Fernandez-Ramirez, E.Moya de Guerra, J.M.Udias

Hints on the quadrupole deformation of the Δ(1232)

doi: 10.1103/PhysRevC.73.042201
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2006FE04      Ann.Phys.(New York) 321, 1408 (2006)

C.Fernandez-Ramirez, E.Moya de Guerra, J.M.Udias

Effective Lagrangian Approach to pion photoproduction from the nucleon

NUCLEAR REACTIONS 1n, 1H(γ, π0X), E ≈ 150-800 MeV; 1H(γ, π+X), (γ, π-X), E ≈ 300-800 MeV; calculated σ(θ), recoil nucleus polarization, asymmetries, resonance contributions. Effective Lagrangian approach, comparison with data.

doi: 10.1016/j.aop.2006.02.009
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2006MA12      Phys.Rev. C 73, 024607 (2006)

M.C.Martinez, P.Lava, N.Jachowicz, J.Ryckebusch, K.Vantournhout, J.M.Udias

Relativistic models for quasielastic neutrino scattering

NUCLEAR REACTIONS 12C, 56Fe(ν, ν'X), E=150-5000 MeV; calculated quasielastic σ(E). Relativistic PWIA.

doi: 10.1103/PhysRevC.73.024607
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2006MO34      Phys.Rev. C 74, 054308 (2006)

O.Moreno, R.Alvarez-Rodriguez, P.Sarriguren, E.Moya de Guerra, J.M.Udias, J.R.Vignote

Gamow-Teller strength distributions in Xe isotopes

NUCLEAR STRUCTURE 124,126,128,130,132,134,136,138,140,142Xe; calculated deformation and pairing parameters, Gamow-Teller strength distributions. Self-consistent microscopic formalism.

doi: 10.1103/PhysRevC.74.054308
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2005AN05      Phys.Rev. C 71, 014317 (2005)

A.N.Antonov, M.K.Gaidarov, M.V.Ivanov, D.N.Kadrev, E.Moya de Guerra, P.Sarriguren, J.M.Udias

Superscaling, scaling functions, and nucleon momentum distributions in nuclei

NUCLEAR STRUCTURE 4He, 12C, 27Al, 56Fe, 197Au; calculated electron-scattering scaling functions, nucleon momentum distributions.

doi: 10.1103/PhysRevC.71.014317
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2005AN29      Phys.Rev. C 72, 044307 (2005)

A.N.Antonov, D.N.Kadrev, M.K.Gaidarov, E.Moya de Guerra, P.Sarriguren, J.M.Udias, V.K.Lukyanov, E.V.Zemlyanaya, G.Z.Krumova

Charge and matter distributions and form factors of light, medium, and heavy neutron-rich nuclei

NUCLEAR STRUCTURE 4,6,8He, 6,11Li, 56,58,62,74Ni, 82,92,94Kr, 116,118,126,132Sn; calculated particle densities, radii, charge form factors, diffuseness parameters. PWBA, DWBA, large-scale shell model and deformed self-consistent mean-field calculations. Comparisons with data.

doi: 10.1103/PhysRevC.72.044307
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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
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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
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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
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2004AN05      Phys.Rev. C 69, 044321 (2004)

A.N.Antonov, M.K.Gaidarov, D.N.Kadrev, M.V.Ivanov, E.Moya de Guerra, J.M.Udias

Superscaling in nuclei: A search for a scaling function beyond the relativistic Fermi gas model

NUCLEAR STRUCTURE 4He, 12C, 40Ca, 197Au; calculated nucleon momentum distributions, scaling functions for electron scattering. Coherent density fluctuation model.

doi: 10.1103/PhysRevC.69.044321
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2004AN27      Eur.Phys.J. A 22, 449 (2004)

K.A.Aniol, M.B.Epstein, E.Gama, D.J.Margaziotis, W.Bertozzi, J.P.Chen, D.Dale, R.E.J.Florizone, S.Gilad, A.J.Sarty, J.A.Templon, S.P.Van Verst, J.Zhao, Z.-L.Zhou, P.Bartsch, W.U.Boeglin, R.Boehm, M.O.Distler, I.Ewald, J.M.Friedrich, J.M.Friedrich, R.Geiges, P.Jennewein, M.Kahrau, K.W.Krygier, A.Liesenfeld, H.Merkel, K.Merle, U.Muller, R.Neuhausen, E.A.J.M.Offermann, Th.Pospischil, G.Rosner, H.Schmieden, A.Wagner, Th.Walcher, M.Kuss, A.Richter, G.Schrieder, K.Bohinc, M.Potokar, S.Sirca, J.M.Udias, J.R.Vignote, R.Schiavilla

Measurement of RLT and ATL in the 4He(e, e'p)3H reaction at pmiss of 130-300 MeV/c

NUCLEAR REACTIONS 4He(e, e'p), E=675, 855 MeV; measured σ(E, θ), transverse-longitudinal asymmetry, response function. Comparison with model predictions.

doi: 10.1140/epja/i2004-10040-x
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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
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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
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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
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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
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2003ST13      Phys.Rev.Lett. 91, 052301 (2003)

S.Strauch, S.Dieterich, K.A.Aniol, J.R.M.Annand, O.K.Baker, W.Bertozzi, M.Boswell, E.J.Brash, Z.Chai, J.-P.Chen, M.E.Christy, E.Chudakov, A.Cochran, R.De Leo, R.Ent, M.B.Epstein, J.M.Finn, K.G.Fissum, T.A.Forest, S.Frullani, F.Garibaldi, A.Gasparian, O.Gayou, S.Gilad, R.Gilman, C.Glashausser, J.Gomez, V.Gorbenko, P.L.J.Gueye, J.O.Hansen, D.W.Higinbotham, B.Hu, C.E.Hyde-Wright, D.G.Ireland, C.Jackson, C.W.de Jager, X.Jiang, C.Jones, M.K.Jones, J.D.Kellie, J.J.Kelly, C.E.Keppel, G.Kumbartzki, M.Kuss, J.J.LeRose, K.Livingston, N.Liyanage, S.Malov, D.J.Margaziotis, D.Meekins, R.Michaels, J.H.Mitchell, S.K.Nanda, J.Nappa, C.F.Perdrisat, V.A.Punjabi, R.D.Ransome, R.Roche, G.Rosner, M.Rvachev, F.Sabatie, A.Saha, A.Sarty, J.M.Udias, P.E.Ulmer, G.M.Urciuoli, J.F.J.van den Brand, J.R.Vignote, D.P.Watts, L.B.Weinstein, K.Wijesooriya, B.Wojtsekhowski

Polarization Transfer in the 4He(e(pol), e'p(pol))3H Reaction up to Q2=2.6 (GeV/c)2

NUCLEAR REACTIONS 4He(polarized e, e'p), E=3400, 4237, 4239 MeV; measured polarization transfer; deduced medium modification effects. Comparison with model predictions.

doi: 10.1103/PhysRevLett.91.052301
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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
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2001DI06      Phys.Lett. 500B, 47 (2001)

S.Dieterich, P.Bartsch, D.Baumann, J.Bermuth, K.Bohinc, R.Bohm, D.Bosnar, S.Derber, M.Ding, M.Distler, I.Ewald, J.Friedrich, J.M.Friedrich, R.Gilman, C.Glashausser, M.Hauger, P.Jennewein, J.Jourdan, J.J.Kelly, M.Kohl, A.Kozlov, K.W.Krygier, G.Kumbartzki, J.Lac, A.Liesenfeld, H.Merkel, U.Muller, R.Neuhausen, Th.Pospischil, R.D.Ransome, D.Rohe, G.Rosner, H.Schmieden, M.Seimetz, I.Sick, S.Strauch, J.M.Udias, J.R.Vignote, A.Wagner, Th.Walcher, G.Warren, M.Weis

Polarization Transfer in the 4He((pol)e, e'p(pol))3H Reaction

NUCLEAR REACTIONS 4He(polarized e, e'p), E=854.5 MeV; measured polarization transfer vs missing momentum. Comparison with model predictions.

doi: 10.1016/S0370-2693(01)00052-1
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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
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2000UD01      Phys.Rev. C62, 034302 (2000)

J.M.Udias, J.R.Vignote

Relativistic Nuclear Structure Effects in (e, e'p(pol))

NUCLEAR REACTIONS 12C(e, e'p), E=579 MeV; 16O(e, e'p), E=855, 2445 MeV; calculated recoil proton polarization vs missing momentum; deduced contribution from dynamical relativistic effects. Comparison with data.

doi: 10.1103/PhysRevC.62.034302
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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
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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
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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
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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
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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
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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
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1997AM08      Nucl.Phys. A625, 633 (1997)

K.Amir-Azimi-Nili, J.M.Udias, H.Muther, L.D.Skouras, A.Polls

Correlations and the Cross Section of Exclusive (e, e'p) Reactions for 16O

NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated reduced σ vs missing momentum; deduced long-range correlations role. DWIA analysis. Comparison with data.

doi: 10.1016/S0375-9474(97)00595-2
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1997UD01      J.Phys.(London) G23, 1673 (1997)

J.M.Udias, R.Nojarov, A.Faessler

M1 (e, e') Excitations in 30Si and 32S from the Quasiparticle Random-Phase Approximation

NUCLEAR REACTIONS 30Si, 32S(e, e'), E=20-100 MeV; analyzed σ(θ). DWBA analysis, QRPA calculations.

NUCLEAR STRUCTURE 30Si, 32S; calculated M1 spectra, transition densities. QRPA calculations, Woods-Saxon potential, comparison with shell model.

doi: 10.1088/0954-3899/23/11/015
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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
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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
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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
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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
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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
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1995UM02      Phys.Rev.Lett. 74, 4993 (1995)

Y.Umino, J.M.Udias, P.J.Mulders

Exchange Current Correlations to Neutrino-Nucleus Scattering

NUCLEAR REACTIONS 12C(ν, ν'p), (ν, μ-), E not given; calculated differential σ. Relativistic exchange current corrections.

doi: 10.1103/PhysRevLett.74.4993
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1995UM03      Phys.Rev. C52, 3399 (1995)

Y.Umino, J.M.Udias

Exchange Current Corrections to Neutrino-Nucleus Scattering. I. Nuclear Matter

NUCLEAR REACTIONS 12C(e, e'), E not given; calculated longitudinal, transverse form factors. 12C(ν, μ-X), E ≤ 300 MeV; calculated σ(E). 12C(ν, ν'p), E not given; calculated σ vs ejected nucleon kinetic energy. Impulse approximation, relativistic exchange current corrections.

doi: 10.1103/PhysRevC.52.3399
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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
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1992GA22      Nucl.Phys. A550, 391 (1992)

E.Garrido, E.Moya de Guerra, P.Sarriguren, J.M.Udias

Scattering of Polarized Electrons from Deformed Nuclei: The case of elastic and inelastic scattering to discrete state in 21Ne

NUCLEAR REACTIONS 21Ne(polarized e, e'), (polarized e, e), E not given; calculated electric, magnetic multipole form factors. Deformed Hartree-Fock intrinsic wave functions, polarized target, Skyrme type effective interactions.

doi: 10.1016/0375-9474(92)90016-D
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1991GA17      Phys.Rev. C44, R1250 (1991)

E.Garrido, E.Moya de Guerra, P.Sarriguren, J.M.Udias

Orbital 1+ Strengths from Self-Consistent Deformed Mean Field Calculations

NUCLEAR STRUCTURE 144,148,150,152,154Sm, 142,146,148,150Nd; calculated mass quadrupole deformation parameter, charge quadrupole moments, B(M1). Hartree-Fock+BCS formalism.

doi: 10.1103/PhysRevC.44.R1250
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1990RE06      Nucl.Phys. A511, 221 (1990)

J.Retamosa, J.M.Udias, A.Poves, E.Moya de Guerra

1+ Excitations in Light Nuclei: SU(3) versus realistic shell model results

NUCLEAR STRUCTURE 20,22Ne, 24Mg, 44Ti; calculated levels, B(λ), form factor. Shell model.

doi: 10.1016/0375-9474(90)90157-H
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1987MO22      Phys.Lett. 196B, 409 (1987)

E.Moya de Guerra, P.Sarriguren, J.M.Udias

On the Scissors Type Mode in 46Ti and Lighter Nuclei

NUCLEAR STRUCTURE 20,22Ne, 44,46Ti; calculated form factors, B(M1). Projected Hartree-Fock model.

doi: 10.1016/0370-2693(87)90791-X
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