NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = M.Rodriguez-Gallardo Found 41 matches. 2021AL13 Phys.Rev. C 103, 054614 (2021) M.A.G.Alvarez, M.Rodriguez-Gallardo, J.P.Fernandez-Garcia, J.Casal, J.A.Lay Systematic calculations of reactions with exotic and stable nuclei to establish a unified theoretical approach NUCLEAR REACTIONS 208Pb(11Li, 11Li), E=29.8 MeV; 208Pb(9Li, 9Li), E=29.5 MeV; 208Pb(9Be, 9Be), E=44.0 MeV; 208Pb(12C, 12C), E=75 MeV; 197Au(11Be, 11Be), E=39.6 MeV; 120Sn(6He, 6He), E=18 MeV; calculated and analyzed experimental data for elastic scattering cross sections; deduced systematic free optical model (OM) parameters using continuum discretized coupled channel (CDCC) calculations; deduced Coulomb dipole polarization (CDP) potential and trivial equivalent local potential (TELP).
doi: 10.1103/PhysRevC.103.054614
2021GA14 Phys.Rev. C 103, 034616 (2021) L.R.Gasques, M.A.G.Alvarez, A.Arazi, B.V.Carlson, L.C.Chamon, J.P.Fernandez-Garcia, A.Lepine-Szily, J.Lubian, J.Rangel, M.Rodriguez-Gallardo, V.Scarduelli, V.A.B.Zagatto Understanding the mechanisms of nuclear collisions: A complete study of the 10B + 120Sn reaction NUCLEAR REACTIONS 120Sn(10Be, 10Be), (10B, X)4He/6He/6Li/7Li/9Be/10Be/10B/11B/11C/12C, E≈39.70 MeV; measured reaction products, particle spectra, σ(θ) for elastic and inelastic scattering using SATURN and STAR particle-detector arrays of semiconductor silicon surface barrier detectors and single sided silicon strip detector (SSSSD) at the 8 MV tandem accelerator of the University of Sao Paulo; deduced σ(θ) for the 1-neutron transfer channel, energy projection of 9Be nuclei, σ(θ) for 6,7Li, 9,10Be, 11B and 12C. Comparison with coupled reaction channels (CRC) calculations using the SPP as the bare interaction.
doi: 10.1103/PhysRevC.103.034616
2021LI22 Phys.Rev. C 103, 044613 (2021) R.Linares, M.Sinha, E.N.Cardozo, V.Guimaraes, G.V.Rogachev, J.Hooker, E.Koshchiy, T.Ahn, C.Hunt, H.Jayatissa, S.Upadhyayula, B.Roeder, A.Saastomoinen, J.Lubian, M.Rodriguez-Gallardo, J.Casal, K.C.C.Pires, M.Assuncao, Y.Penionzhkevich, S.Lukyanov Elastic scattering measurements for the 10C+ 208Pb system at Elab = 66 MeV NUCLEAR REACTIONS 208Pb(10C, 10C), E=66 MeV, [10C secondary beam from 1H(10B, 10C), E=9.6 MeV/nucleon primary reaction, followed by selection of 10C beam by the Momentum Achromatic Recoil Spectrometer (MARS) at the K500 superconducting Cyclotron Institute of Texas A and M University]; measured elastically scattered 10C ions, angular distribution of scattered 10C, total σ using ΔE-E telescope of double-sided silicon strip detectors (DSSSDs); deduced suppression of the Fresnel peak. Comparison with optical model, coupled channels, and 3-body and 4-body continuum-discretized coupled-channels (CDCC) calculations using 9B+p, 6Be+α, and 8Be+p+p cluster configurations of 10C with a Brunnian (super-Borromean) structure; analyzed reaction cross sections in literature for the several projectiles on 208Pb target.
doi: 10.1103/PhysRevC.103.044613
2020CA30 Phys.Rev. C 102, 069801 (2020) J.Casal, M.Rodriguez-Gallardo, J.M.Arias, E.Garrido, R.de Diego Comment on "From Coulomb excitation cross sections to nonresonant astrophysical rates in three-body systems: The 17Ne case" NUCLEAR REACTIONS 15O(2p, γ)17Ne, T=0.3-10 GK; calculated contribution to the reaction rate from 1/2+ states, and 1/2+ resonance. 208Pb(17Ne, X), E=500 MeV/nucleon; calculated Coulomb dissociation cross sections for the 1/2+ B(E1) distribution, for the total (1/2+ + 3/2+) B(E1) distribution, and from shifting of the 1/2+ resonance position. Comparison with experimental data. This comment is in response to critique by 2018Pa43 on the calculations in 2016Ca38 about the radiative capture for 17Ne formation.
doi: 10.1103/PhysRevC.102.069801
2020GA11 Phys.Rev. C 101, 044604 (2020) L.R.Gasques, L.C.Chamon, A.Lepine-Szily, V.Scarduelli, V.A.B.Zagatto, D.Abriola, A.Arazi, M.A.Cardona, E.de Barbara, J.de Jesus, D.Hojman, G.V.Marti, A.J.Pacheco, D.Ramos Lopez, M.A.G.Alvarez, J.P.Fernandez-Garcia, M.Rodriguez-Gallardo, M.Cubero, L.F.Umana, S.Achi-Prado Investigation of the reaction mechanisms for 10B + 197Au at near-barrier energies NUCLEAR REACTIONS 197Au(10B, 10B), (10B, 10B'), (10B, 11B), (10B, 9Be), E=38-61 MeV; measured reaction products, beam-like recoils, and σ(E, θ) using E-ΔE silicon surface barrier telescopes at the 8-MV Pelletron accelerator of the University of Sao Paulo, and at the 20-MV tandem accelerator TANDAR; deduced total integrated cross sections. 10B, 197Au; deduced levels, J, π, yields. Comparison with coupled reaction channel (CRC) calculations, with double-folding Sao Paulo potential. Discussed breakup process of 10B.
doi: 10.1103/PhysRevC.101.044604
2020SO22 Phys.Rev. C 102, 064622 (2020) V.Soukeras, O.Sgouros, A.Pakou, F.Cappuzzello, J.Casal, C.Agodi, G.A.Brischetto, S.Calabrese, D.Carbone, M.Cavallaro, I.Ciraldo, I.Dimitropoulos, S.Koulouris, L.La Fauci, I.Martel, M.Rodriguez-Gallardo, A.M.Sanchez-Benitez, G.Souliotis, A.Spatafora, D.Torresi Global study of 9Be + p at 2.72A MeV NUCLEAR REACTIONS 1H(9Be, 9Be), (9Be, d)8Be, (9Be, 6Li)4He, E=24.5 MeV; measured reaction products, elastically scattered 9Be, α, 6Li, σ(θ), triple α-α-p coincidence for breakup process in a full kinematic approach using MAGNEX magnetic spectrometer and GLORIA detector array at INFN-LNS in Catania; deduced ΔE-E spectrum, reconstructed sum α+α+n energy versus the energy of an individual α, reconstructed Q-value spectra, reconstructed energy spectra for the unobserved neutron and the recoiling proton. Comparison with four-body continuum discretized coupled-channel (CDCC) formalism.
doi: 10.1103/PhysRevC.102.064622
2019AL32 Phys.Rev. C 100, 064602 (2019) M.A.G.Alvarez, J.P.Fernandez-Garcia, J.L.Leon-Garcia, M.Rodriguez-Gallardo, L.R.Gasques, L.C.Chamon, V.A.B.Zagatto, A.Lepine-Szily, J.R.B.Oliveira, V.Scarduelli, B.V.Carlson, J.Casal, A.Arazi, D.A.Torres, F.Ramirez Systematic study of optical potential strengths in reactions on 120Sn involving strongly bound, weakly bound, and exotic nuclei NUCLEAR REACTIONS 120Sn(6Li, 6Li), E=19, 24, 27 MeV; measured scattered 6Li, σ(E, θ) using SATURN array of Si detectors at the tandem accelerator of LAFN, University of Sao Paulo. 120Sn(α, α), E(reduced)=5.1, 12.0, 15.6, 19.1 MeV; 120Sn(6He, 6He), E(reduced)=3.8, 4.4, 6.1, 6.7, 8.4 MeV; 120Sn(7Li, 7Li), E(reduced)=0.6, 1.3, 3.2, 5.1, 7.0, 8.9 MeV; 120Sn(9Be, 9Be), E(reduced)=0.3, 0.7, 1.6, 1.7, 3.1, 13.3, 20.7 MeV; 120Sn(10B, 10B), E(reduced)=0.2, 1.6, 2.1, 3.4 MeV; 120Sn(16O, 16O), E(reduced)=2.3, 3.1, 4.0 MeV; 120Sn(18O, 18O), E(reduced)=2.1 MeV; analyzed previous σ(E, θ) data as part of the E-125 experimental campaign, developed at the LAFN, with experiments carried out at Sao Paulo and TANDAR facility in Buenos Aires. Optical model analyses based on the double-folding Sao Paulo potential. NUCLEAR STRUCTURE 6Li, 6He, 9,10Be; calculated matter densities using Hartree-Bogoliubov (HB) theory with NL3 and DDME1 interactions, and from charge densities obtained in (e, e') experiments. 4,6He, 6,7Li, 9,10Be, 16,18O; calculated s-wave barrier parameters using double-folding Sao Paulo potential (SPP) for systems with projectiles focusing on 120Sn.
doi: 10.1103/PhysRevC.100.064602
2019AP01 Phys.Rev. C 99, 014601 (2019) S.Appannababu, R.Lichtenthaler, M.A.G.Alvarez, M.Rodriguez-Gallardo, A.Lepine-Szily, K.C.C.Pires, O.C.B.Santos, U.U.Silva, P.N.de Faria, V.Guimaraes, E.O.N.Zevallos, V.Scarduelli, M.Assuncao, J.M.B.Shorto, A.Barioni, J.Alcantara-Nunez, V.Morcelle Two-neutron transfer in the 6He + 120Sn reaction NUCLEAR REACTIONS 120Sn(6He, α), E=20.3, 22.2, 22.4, 24.5 MeV; 120Sn(6He, 6He), E=22.2 MeV, [secondary 6He beam from 9Be(7Li, 6He) primary reaction]; measured reaction products, Eα, Iα, 6He scattered particles, differential σ(E, θ), and σ(θ) for elastic scattering using RIBRAS facility at Sao Paulo University; deduced Q-value centroids, transferred angular momentum, dependence of excitation energy of the residual system on the transferred angular momentum using Brink's formula, and square of the final angular momentum. Comparison with four body continuum discretized coupled channel (CDCC) calculations. Discussed formation of di-nuclear rotating system that could be formed after the reaction.
doi: 10.1103/PhysRevC.99.014601
2019FE05 Phys.Rev. C 99, 054605 (2019) J.P.Fernandez-Garcia, A.Di Pietro, P.Figuera, J.Gomez-Camacho, M.Lattuada, J.Lei, A.M.Moro, M.Rodriguez-Gallardo, V.Scuderi Breakup mechanisms in the 6He + 64Zn reaction at near-barrier energies NUCLEAR REACTIONS 64Zn(α, α), E=17.4 MeV; measured scattered α particles, differential σ(θ) using LEDA-type detectors and single-sided silicon strip detectors for particle detection at the Louvain la Neuve (Belgium) cyclotron facility; analyzed present data and previous experimental data at E(α)=13.2 MeV by optical model calculations based on the Sao Paulo potential. 64Zn(6He, 6He), (6He, α), E=14.85, 17.9 MeV; measured scattered particles, differential σ(θ) for outgoing 6He and α particles, the latter from 2n transfer process; analyzed present data and previous experimental data at E(6He)=9.8 and 13.5 MeV by optical model calculations, coupled-reaction-channel (CRC), continuum-discretized coupled channel (CDCC), and DWBA inclusive-breakup models.
doi: 10.1103/PhysRevC.99.054605
2018AL29 Phys.Rev. C 98, 024621 (2018) M.A.G.Alvarez, M.Rodriguez-Gallardo, L.R.Gasques, L.C.Chamon, J.R.B.Oliveira, V.Scarduelli, A.S.Freitas, E.S.Rossi, V.A.B.Zagatto, J.Rangel, J.Lubian, I.Padron Elastic scattering, inelastic excitation, and 1n pick-up transfer cross sections for 10B + 120Sn at energies near the Coulomb barrier NUCLEAR REACTIONS 120Sn(10B, 10B), (10B, 10B'), (10B, 11B), E=31.5, 33.5, 35.0, 37.5 MeV; measured particle spectra, elastic, inelastic and one-neutron pick-up σ(θ, E) using Silicon Array based on Telescopes of USP for Reactions and Nuclear applications (SATURN) at the Open Laboratory of Nuclear Physics (LAFN) of the University of Sao Paulo. Comparison with coupled-reaction channel (CRC), optical optical model (OM), and continuum-discretized coupled-channels calculations (CDCC) calculations using the double-folding Sao Paulo potential (SPP).
doi: 10.1103/PhysRevC.98.024621
2018AR02 Phys.Rev. C 97, 044609 (2018) A.Arazi, J.Casal, M.Rodriguez-Gallardo, J.M.Arias, R.Lichtenthaler Filho, D.Abriola, O.A.Capurro, M.A.Cardona, P.F.F.Carnelli, E.de Barbara, J.Fernandez Niello, J.M.Figueira, L.Fimiani, D.Hojman, G.V.Marti, D.Martinez Heimann, A.J.Pacheco 9Be + 120Sn scattering at near-barrier energies within a four-body model NUCLEAR REACTIONS 120Sn(9Be, 9Be), (9Be, 9Be'), E=26, 27, 28, 29.5, 31, 42, 50 MeV; measured scattered particles, differential σ(E, θ) of elastic and inelastic channels using 20 UD tandem accelerator TANDAR at Buenos Aires; deduced excitation to first 2+ and 3- states in 120Sn. Comparison with optical model (OM) and four-body continuum-discretized coupled-channels (CDCC) calculations.
doi: 10.1103/PhysRevC.97.044609
2016CA16 Phys.Rev. C 93, 041602 (2016) J.Casal, M.Rodriguez-Gallardo, J.M.Arias, J.Gomez-Camacho Determining astrophysical three-body radiative capture reaction rates from inclusive Coulomb break-up measurements NUCLEAR REACTIONS 208Pb(11Li, X), E=24.3, 29.8 MeV; Pb(6He, X), E=18, 22 MeV; calculated breakup probability of 11Li in 9Li+n+n and 6He in α+n+n as a function of collision time, B(E1) distribution, and compared with experimental data. 9Li(2n, γ)11Li, T9=0.5-2.5; 4He(2n, γ)6He, T9=2.75-4; calculated reaction rates. Established a relation between radiative capture reaction rate and the inclusive Coulomb break-up probability.
doi: 10.1103/PhysRevC.93.041602
2016CA38 Phys.Rev. C 94, 054622 (2016) J.Casal, E.Garrido, R.de Diego, J.M.Arias, M.Rodriguez-Gallardo Radiative capture reaction for 17Ne formation within a full three-body model NUCLEAR STRUCTURE 17Ne; calculated energy and probability distribution of the ground state, matter and charge radii of 17Ne Borromean nucleus in a full three-body (15O+p+p) model using analytical transformed harmonic oscillator (THO), and the hyperspherical adiabatic (HA) expansion methods. Comparison with experimental values. NUCLEAR REACTIONS 15O(2p, γ)17Ne, T9=0.1-10; calculated two-proton capture reaction rate using the THO method, including sequential and direct, resonant and nonresonant contributions, dominant E1 contributions to the reaction rate from the inverse photodissociation process. Comparison with previous theoretical calculations. Relevance to CNO cycles and rp-process.
doi: 10.1103/PhysRevC.94.054622
2015CA25 Phys.Rev. C 92, 054611 (2015) J.Casal, M.Rodriguez-Gallardo, J.M.Arias 9Be elastic scattering on 208Pb and 27Al within a four-body reaction framework NUCLEAR REACTIONS 208Pb(9Be, 9Be), E=38, 44, 60 MeV; 27Al(9Be, 9Be), E=14, 22, 32 MeV; calculated σ(θ, E); deduced effects of model space truncation, continuum couplings, dipolar contribution, and position of the projectile low-energy resonances. Four-body framework using the continuum-discretized coupled-channels (CDCC) method, with 9Be described in a three-body (α+α+n) model using the analytical transformed harmonic oscillator (THO) basis in hyperspherical coordinates. Comparison with available experimental data. NUCLEAR STRUCTURE 9Be; calculated levels energies of 3/2-, 1/2+ and 5/2- states up to 10 MeV for an analytical THO basis.
doi: 10.1103/PhysRevC.92.054611
2015FE09 Phys.Rev. C 92, 044608 (2015) J.P.Fernandez-Garcia, M.Cubero, L.Acosta, M.Alcorta, M.A.G.Alvarez, M.J.G.Borge, L.Buchmann, C.A.Diget, H.A.Falou, B.Fulton, H.O.U.Fynbo, D.Galaviz, J.Gomez-Camacho, R.Kanungo, J.A.Lay, M.Madurga, I.Martel, A.M.Moro, I.Mukha, T.Nilsson, M.Rodriguez-Gallardo, A.M.Sanchez-Benitez, A.Shotter, O.Tengblad, P.Walden Simultaneous analysis of the elastic scattering and breakup channel for the reaction 11Li+208Pb at energies near the Coulomb barrier NUCLEAR REACTIONS 208Pb(11Li, 11Li), (11Li, X), (9Li, X), E=24.3, 29.8 MeV, [11Li beam from Ta(p, X), E=500 MeV from radioactive ion beam facility at TRIUMF]; measured 9,11Li elastic scattering and 9Li fragment spectra using detector telescopes, σ(θ), reaction and breakup σ; deduced energy distributions of the outgoing 9Li fragments from breakup of 11Li, B(E1) distributions of 11Li. Comparison to coupled-reaction-channel (CRC) and continuum-discretized coupled-channel (CDCC) calculations.
doi: 10.1103/PhysRevC.92.044608
2014CA36 Phys.Rev. C 90, 044304 (2014); Pub.Note Phys.Rev. C 94, 069903 (2016) J.Casal, M.Rodriguez-Gallardo, J.M.Arias, I.J.Thompson Astrophysical reaction rate for 9Be formation within a three-body approach NUCLEAR STRUCTURE 9Be; calculated ground-state energy, matter and charge radii, sum rule ST(E1) using α+α+n three body approach and analytical transformed harmonic oscillator method for 9Be Borromean nucleus. NUCLEAR REACTIONS 8Be(n, γ)9Be; calculated photodissociation σ(E)for α+α+n --> 9Be+γ reaction, reaction rate dependence on temperature, contribution of resonances to total photodissociation cross section, total astrophysical reaction rates using α+α+n three body approach and analytical transformed harmonic oscillator method. Comparison with experimental results.
doi: 10.1103/PhysRevC.90.044304
2014MO06 Phys.Lett. B 732, 228 (2014) V.Morcelle, K.C.C.Pires, M.Rodriguez-Gallardo, R.Lichtenthaler, A.Lepine-Szily, V.Guimaraes, P.N.de Faria, D.R.Mendes, Jr, A.M.Moro, L.R.Gasques, E.Leistenschneider, R.P.Condori, V.Scarduelli, M.C.Morais, A.Barioni, J.C.Zamora, J.M.B.Shorto Four-body effects in the 6He + 58Ni scattering NUCLEAR REACTIONS 58Ni(6He, 6He), E=12.2, 16.5, 21.7 MeV; measured reaction products; deduced σ, four-body effects. Comparison with continuum-discretized coupled-channels calculation.
doi: 10.1016/j.physletb.2014.03.043
2013CA15 Phys.Rev. C 88, 014327 (2013) J.Casal, M.Rodriguez-Gallardo, J.M.Arias Analytical transformed harmonic oscillator basis for three-body nuclei of astrophysical interest: Application to 6He NUCLEAR STRUCTURE 6He; calculated levels, J, π, ground-state energy, matter radius, B(E1) distribution, radiative capture reaction rate of astrophysics interest. Three-body α+n+n Borromean system. Analytical transformed harmonic oscillator (THO) method. Comparison with previous theoretical studies.
doi: 10.1103/PhysRevC.88.014327
2013FE04 Phys.Rev.Lett. 110, 142701 (2013) J.P.Fernandez-Garcia, M.Cubero, M.Rodriguez-Gallardo, L.Acosta, M.Alcorta, M.A.G.Alvarez, M.J.G.Borge, L.Buchmann, C.A.Diget, H.A.Falou, B.R.Fulton, H.O.U.Fynbo, D.Galaviz, J.Gomez-Camacho, R.Kanungo, J.A.Lay, M.Madurga, I.Martel, A.M.Moro, I.Mukha, T.Nilsson, A.M.Sanchez-Benitez, A.Shotter, O.Tengblad, P.Walden 11Li Breakup on 208Pb at Energies Around the Coulomb Barrier NUCLEAR REACTIONS 208Pb(11Li, X), (11Li, 9Li), E=24.3, 29.8 MeV; measured reaction products. 9,11Li; deduced breakup probabilities angular and B(E1) distributions. Comparison with CDCC calculations, available data.
doi: 10.1103/PhysRevLett.110.142701
2012CU02 Phys.Rev.Lett. 109, 262701 (2012) M.Cubero, J.P.Fernandez-Garcia, M.Rodriguez-Gallardo, L.Acosta, M.Alcorta, M.A.G.Alvarez, M.J.G.Borge, L.Buchmann, C.A.Diget, H.Al Falou, B.R.Fulton, H.O.U.Fynbo, D.Galaviz, J.Gomez-Camacho, R.Kanungo, J.A.Lay, M.Madurga, I.Martel, A.M.Moro, I.Mukha, T.Nilsson, A.M.Sanchez-Benitez, A.Shotter, O.Tengblad, P.Walden Do Halo Nuclei Follow Rutherford Elastic Scattering at Energies Below the Barrier? The Case of 11Li NUCLEAR REACTIONS 208Pb(11Li, 11Li), (9Li, 9Li), E=23.9-43 MeV. 9,11Li; measured reaction products; deduced σ(θ), Rutherford σ. Four-body CDCC calculations with code FRESCO calculations.
doi: 10.1103/PhysRevLett.109.262701
2011CR02 Phys.Rev. C 83, 054613 (2011) R.Crespo, M.Rodriguez-Gallardo, A.M.Moro, A.Deltuva, E.Cravo, A.C.Fonseca Resonant breakup of 19C on a proton target NUCLEAR REACTIONS 1H(19C, p), E=70 MeV/nucleon; calculated differential energy distribution for the resonant breakup, σ(θ). Faddeev-Alt, Grassberger, Sandhas (Faddeev-AGS) and continuum-discretized coupled-channels (CDCC) reaction frameworks using three-body model (18C+n+p) for the reaction.
doi: 10.1103/PhysRevC.83.054613
2011PI08 Phys.Rev. C 83, 064603 (2011) K.C.C.Pires, R.Lichtenthaler, A.Lepine-Szily, V.Guimaraes, P.N.de Faria, A.Barioni, D.R.Mendes, Jr., V.Morcelle, R.P.Condori, M.C.Morais, J.C.Zamora, E.Crema, A.M.Moro, M.Rodriguez-Gallardo, M.Assuncao, J.M.B.Shorto, S.Mukherjee Experimental study of 6He+9Be elastic scattering at low energies NUCLEAR REACTIONS 9Be, 197Au(6He, 6He), E=16.2, 21.3 MeV, [6He secondary beam from 9Be(7Li, 6He), E=22.18, 26.10 MeV primary beam]; measured 6He spectra, cross sections, σ(θ), biparametric spectrum. Effect of the collective couplings to the excited states. Coupled channels calculations, using a double-folding potential, and three- and four-body continuum-discretized coupled-channels (CDCC) calculations.
doi: 10.1103/PhysRevC.83.064603
2011RO14 Int.J.Mod.Phys. E20, 947 (2011) M.Rodriguez-Gallardo, A.M.Moro Four-body continuum-discretized coupled-channel calculations applied to 6He reactions around the Coulomb barrier NUCLEAR REACTIONS 64Zn(6He, X), E=13.6 MeV; 120Sn(6He, X), E=17.4 MeV; 208Pb(6He, X), E=22 MeV; calculated σ. THO method, comparison with experimental data.
doi: 10.1142/S0218301311019039
2010DE14 Phys.Rev. C 81, 044605 (2010) P.N.de Faria, R.Lichtenthaler, K.C.C.Pires, A.M.Moro, A.Lepine-Szily, V.Guimaraes, D.R.Mendes, Jr., A.Arazi, M.Rodriguez-Gallardo, A.Barioni, V.Morcelle, M.C.Morais, O.Camargo, Jr., J.Alcantara Nunez, M.Assuncao Elastic scattering and total reaction cross section of 6He+120Sn NUCLEAR REACTIONS 120Sn(6He, 6He), E=17.40, 18.05, 19.80, 20.5 MeV; σ(E, θ). Comparison with optical model and continuum discretized coupled channels (CDCC) calculations.
doi: 10.1103/PhysRevC.81.044605
2010FE05 Phys.Lett. B 693, 310 (2010) J.P.Fernandez-Garcia, M.A.G.Alvarez, A.M.Moro, M.Rodriguez-Gallardo Simultaneous analysis of elastic scattering and transfer/breakup channels for the 6He + 208Pb reaction at energies near the Coulomb barrier NUCLEAR REACTIONS 208Pb(6He, 6He), (6He, α), E=14, 16, 18, 22, 27 MeV; calculated σ(θ), σ(E), σ, effective potentials. Coupled-Reaction-Channels (CRC) method.
doi: 10.1016/j.physletb.2010.07.060
2010FE09 Nucl.Phys. A840, 19 (2010) J.P.Fernandez-Garcia, M.Rodriguez-Gallardo, M.A.G.Alvarez, A.M.Moro Long range effects on the optical model of 6He around the Coulomb barrier NUCLEAR REACTIONS 27Al(6He, 6He), E=9.5, 11, 12, 13.4 MeV; 208Pb(6He, 6He), E=14, 16, 18, 22, 27 MeV; calculated σ(θ) using an optical model with various potentials and coupled-channels approach. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.03.013
2010LE14 Nucl.Phys. A834, 491c (2010) A.Lepine-Szily, R.Lichtenthaler, V.Guimaraes, D.R.Mendes, Jr, P.N.de Faria, A.Barioni, E.A.Benjamim, K.C.C.Pires, V.Morcelle, R.P.Condori, M.C.Morais, P.Descouvemont, A.M.Moro, M.Rodriguez Gallardo, M.M.Assuncao, J.A.Alcantara Nunez, J.M.B.Shorto, J.C.Zamora, E.Leistenschneider, C.E.F.Lima Scientific program of the Radioactive Ion Beams Facility in Brasil (RIBRAS) NUCLEAR REACTIONS 1H(8Li, α), E=13.2, 14.5, 17.4, 19.0 MeV; measured Eα, Iα(θ=forward); deduced σ(θ=forward), effect of halo nuclei. 9Be(6He, 6He), E=16.2 MeV; measured σ(θ); deduced effect of halo nuclei.
doi: 10.1016/j.nuclphysa.2010.01.074
2009CR01 Phys.Rev. C 79, 014609 (2009) R.Crespo, A.Deltuva, M.Rodriguez-Gallardo, E.Cravo, A.C.Fonseca Spectroscopy of unbound states under quasifree scattering conditions: One-neutron knockout reaction of 14Be NUCLEAR REACTIONS 1H(14Be, 12Be), (14Be, 13Be), E=69 MeV/nucleon; calculated σ, transverse momentum distributions. Full Faddeev-type calculations.
doi: 10.1103/PhysRevC.79.014609
2009CR07 Eur.Phys.J. A 42, 609 (2009) R.Crespo, A.Deltuva, E.Cravo, M.Rodriguez-Gallardo, A.C.Fonseca One-neutron knockout reaction of halo nuclei NUCLEAR REACTIONS 1H(11Be, 10Be), E=38.4, 200 MeV/nucleon; calculated σ(θ, E) in a three-body multiple scattering framework. Comparison with PWIA.
doi: 10.1140/epja/i2008-10757-4
2009RO26 Phys.Rev. C 80, 051601 (2009) M.Rodriguez-Gallardo, J.M.Arias, J.Gomez-Camacho, A.M.Moro, I.J.Thompson, J.A.Tostevin Four-body continuum-discretized coupled-channels calculations NUCLEAR REACTIONS 208Pb(6He, X), E=22 MeV; calculated σ(θ), angular distributions , B(E1) and B(E2) distributions using continuum-discretized coupled channels calculations. calculated . Comparison with experimental data.
doi: 10.1103/PhysRevC.80.051601
2009RO31 Eur.Phys.J. A 42, 601 (2009) M.Rodriguez-Gallardo, A.Deltuva, R.Crespo, E.Cravo, A.C.Fonseca Two-body scattering without angular-momentum decomposition: Fully off-shell T-matrices NUCLEAR REACTIONS 12C(10Be, 10Be), E=49.3 MeV/nucleon; calculated σ(θ) relative to Rutherford and related features using the Lippmann-Schwinger method.
doi: 10.1140/epja/i2008-10744-9
2008CR01 Phys.Rev. C 77, 024601 (2008) R.Crespo, A.Deltuva, E.Cravo, M.Rodriguez-Gallardo, A.C.Fonseca Multiple scattering effects in quasifree scattering from halo nuclei: A test of the distorted-wave impulse approximation NUCLEAR REACTIONS p(11Be, n10Be), (11Be, np), E=38.4, 100, 200 MeV/nucleon; calculated cross sections. Faddeev calculations.
doi: 10.1103/PhysRevC.77.024601
2008RO16 Phys.Rev. C 77, 064609 (2008) M.Rodriguez-Gallardo, J.M.Arias, J.Gomez-Camacho, R.C.Johnson, A.M.Moro, I.J.Thompson, J.A.Tostevin Four-body continuum-discretized coupled-channels calculations using a transformed harmonic oscillator basis NUCLEAR REACTIONS 12C(6He, 6He), E=229.8 MeV; 64Zn(6He, 6He), E=10.0, 13.6 MeV; 208Pb(6He, 6He), E=22 MeV; calculated energy spectra, σ(θ). Comparison with experimental data.
doi: 10.1103/PhysRevC.77.064609
2008RO24 Phys.Rev. C 78, 034602 (2008) M.Rodriguez-Gallardo, A.Deltuva, E.Cravo, R.Crespo, A.C.Fonseca Two-body scattering without angular-momentum decomposition NUCLEAR REACTIONS 10Be, 16O(p, p), E=50, 100, 150, 200 MeV; 10Be(12C, 12C), E=49.3 MeV/nucleon; calculated σ(θ), analyzing powers. Lippman Schwinger equation.
doi: 10.1103/PhysRevC.78.034602
2007CR04 Phys.Rev. C 76, 014620 (2007) R.Crespo, E.Cravo, A.Deltuva, M.Rodriguez-Gallardo, A.C.Fonseca Rescattering effects in proton elastic scattering from halo nuclei: A test of the Glauber approximation NUCLEAR REACTIONS 11Be(p, p), E=100-200 MeV/nucleon; calculated σ and angular distributions using the Faddeev/AGS three-body scattering framework.
doi: 10.1103/PhysRevC.76.014620
2007CR07 Eur.Phys.J. Special Topics 150, 13 (2007) R.Crespo, A.M.Moro, I.J.Thompson, M.Rodriguez-Gallardo, J.Gomez-Camacho, J.M.Arias Exploring the 6He continuum sea through proton inelastic collisions NUCLEAR REACTIONS 6He(p, p'), E=717 MeV; calculated σ(θ) using the MST framework.
doi: 10.1140/epjst/e2007-00253-1
2007MO02 Phys.Rev. C 75, 017603 (2007) A.M.Moro, M.Rodriguez-Gallardo, R.Crespo, I.J.Thompson Continuum description with pseudostate wave functions NUCLEAR REACTIONS 1H(6He, 6He'), E=717 MeV/nucleon; calculated σ(θ). Comparison of two pseudostate bases.
doi: 10.1103/PhysRevC.75.017603
2007MO19 Phys.Rev. C 75, 064607 (2007) A.M.Moro, K.Rusek, J.M.Arias, J.Gomez-Camacho, M.Rodriguez-Gallardo Improved di-neutron cluster model for 6He scattering NUCLEAR REACTIONS 64Zn, 197Au, 208Pb, 209Bi(6He, 6He), E=10-40 MeV; calculated cross sections and angular distributions using a two-body di-neutron cluster model to describe the structure of 6He.
doi: 10.1103/PhysRevC.75.064607
2007RO29 Eur.Phys.J. Special Topics 150, 51 (2007) M.Rodriguez-Gallardo, J.M.Arias, J.Gomez-Camacho, R.C.Johnson, A.M.Moro, I.J.Thompson, J.A.Tostevin Continuum effects: Structure and reactions of 6He NUCLEAR STRUCTURE 6He; calculated B(E1), B(E2) distributions using the Transformed Harmonic Oscillator method. NUCLEAR REACTIONS 12C(6He, 6He), E=229.8 MeV; calculated elastic scattering σ(θ).
doi: 10.1140/epjst/e2007-00264-x
2005RO27 Phys.Rev. C 72, 024007 (2005) M.Rodriguez-Gallardo, J.M.Arias, J.Gomez-Camacho, A.M.Moro, I.J.Thompson, J.A.Tostevin Three-body continuum discretization in a basis of transformed harmonic oscillator states NUCLEAR STRUCTURE 6He; calculated B(E1), B(E2) distributions, sum rules. Transformed harmonic oscillator method, three-body continuum.
doi: 10.1103/PhysRevC.72.024007
2004RO15 Phys.Rev. C 69, 034308 (2004) M.Rodriguez-Gallardo, J.M.Arias, J.Gomez-Camacho Describing resonances in a discrete basis
doi: 10.1103/PhysRevC.69.034308
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