NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = L.F.Canto Found 126 matches. Showing 1 to 100. [Next]2023CO12 Phys.Rev. C 108, 054601 (2023) M.R.Cortes, V.A.B.Zagatto, J.L.Ferreira, J.Rangel, L.F.Canto, J.Lubian Fusion reactions in 6Li + 90Zr scattering
doi: 10.1103/PhysRevC.108.054601
2023FE03 Phys.Rev. C 107, 034603 (2023) J.L.Ferreira, J.Rangel, J.Lubian, L.F.Canto Fusion reactions in collisions of neutron halo nuclei with heavy targets NUCLEAR REACTIONS 209Bi(11Be, X), E(cm)=35-55 MeV; 209Bi(6He, X), E(cm)=15-30 MeV; 238U(6He, X), E(cm)=14-30 MeV; calculated complete and incomplete fusion σ(E), fusion functions. Investigated the static and dynamic effects of the low breakup threshold. Comparison to available experimental data and to the calculations performed with barrier penetration method.
doi: 10.1103/PhysRevC.107.034603
2022AN21 XLIV Brazilian Meeting on Nuclear Physics, Brazil, 9-11 Nov 2021 p.012041 (2022); J.Phys.:Conf.Ser. 2340 M.B.Angelo, V.Guimaraes, M.Assuncao, L.F.Canto, J.Lubian Damping of Mott oscillations as a guide for planning a 6Li +6Li scattering experiment NUCLEAR REACTIONS 6Li(6Li, 6Li), E=6-10 MeV; analyzed available data; deduced σ(θ), Sfresco corrections for the potentials depths and the subsequent Transverse Isotropy (TI) energies.
doi: 10.1088/1742-6596/2340/1/012041
2022LU04 Phys.Rev. C 105, 054601 (2022) J.Lubian, J.L.Ferreira, J.Rangel, M.R.Cortes, L.F.Canto Fusion processes in collisions of 6Li beams on heavy targets NUCLEAR REACTIONS 124Sn(6Li, X), E=15-35 MeV; 197Au(6Li, X), E=20-45 MeV; 198Pt(6Li, X), E=20-45 MeV; 209Bi(6Li, X), E=25-45 MeV; calculated complete, incomplete and total σ(E). Continuum discretized coupled-channel (CDCC) method. Comparison to experimental data.
doi: 10.1103/PhysRevC.105.054601
2021CA10 Eur.Phys.J. A 57, 11 (2021) Semi-classical approaches to heavy-ion reactions: fusion, rainbow, and glory NUCLEAR REACTIONS 208Pb(11Li, X), 209Bi(6Li, X), (7Li, X), E(cm)=10-40 MeV; analyzed available data; deduced fusion σ.
doi: 10.1140/epja/s10050-020-00312-8
2021GU11 Eur.Phys.J. A 57, 90 (2021) V.Guimaraes, E.N.Cardozo, J.Lubian, M.Assuncao, K.C.C.Pires, L.F.Canto, B.Mukeru, G.Kaur, E.F.Aguilera Role of cluster configurations in the elastic scattering of light projectiles on 58Ni and 64Zn targets: a phenomenological analysis NUCLEAR REACTIONS 58Ni(16O, 16O), E=31-45 MeV; 64Zn(9Be, 9Be), (11Be, 11Be), E=17-28.7 MeV; analyzed available data; deduced σ.
doi: 10.1140/epja/s10050-021-00403-0
2020CA31 Eur.Phys.J. A 56, 281 (2020) L.F.Canto, V.Guimaraes, J.Lubian, M.S.Hussein The total reaction cross section of heavy-ion reactions induced by stable and unstable exotic beams: the low-energy regime NUCLEAR REACTIONS 208Pb(16O, 16O), E not given; 12C(12C, X)24Mg, E<40 MeV; 28Si(16O, X), E(cm)=35 MeV; 208Pb(16O, X)224Th, E(cm)<120 MeV; analyzed available data; deduced σ.
doi: 10.1140/epja/s10050-020-00277-8
2020CO13 Phys.Rev. C 102, 064628 (2020) M.R.Cortes, J.Rangel, J.L.Ferreira, J.Lubian, L.F.Canto Complete and incomplete fusion of 7Li projectiles on heavy targets NUCLEAR REACTIONS 124Sn, 197Au, 198Pt, 209Bi(7Li, X), E(cm)=25-48 MeV; calculated complete fusion σ(E), inclusive σ(E) and incomplete fusion σ(E) for weakly bound systems using a new method based on continuum-discretized coupled-channels (CDCC) approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.102.064628
2019BE40 Int.J.Mod.Phys. E28, 1950109(2019) C.A.Bertulani, L.F.Canto, M.S.Hussein, Shubhchintak, T.V.Nhan Hao The neutron within the deuteron as a surrogate for neutron-induced reactions NUCLEAR REACTIONS 59Co, 58Ni, 63Cu, 103Rh, 135Xe, 149Sm, 157Gd, 159Tb, 232Th, 238U(d, p), E<300 MeV; analyzed available data; deduced (n, γ) σ.
doi: 10.1142/S021830131950109X
2018CA25 Phys.Rev. C 98, 044617 (2018) L.F.Canto, R.Donangelo, M.S.Hussein, P.Lotti, J.Lubian, J.Rangel Theoretical considerations about heavy-ion fusion in potential scattering NUCLEAR REACTIONS 208Pb(16O, X), E(cm)=80-200 MeV; 12C(6Li, X), E(cm)=2-50 MeV; calculated fusion σ(E) as function of diffuseness parameter, radial parameters, imaginary potential strengths, and nuclear potentials using Wentzel, Kramers, and Brillouin (WKB) method, and optical model calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.98.044617
2018KO22 Phys.Rev. C 98, 044604 (2018) G.D.Kolinger, L.F.Canto, R.Donangelo, S.R.Souza Semiclassical calculations of complete and incomplete fusion in collisions of weakly bound nuclei NUCLEAR REACTIONS 159Tb, 197Au(6Li, X), (7Li, X), E(cm)=20-42 MeV; calculated complete fusion (CF) and total fusion (TF) σ(E) using an improved version of a semiclassical coupled-channels method. Comparison with experimental values, and with previous theoretical predictions.
doi: 10.1103/PhysRevC.98.044604
2017DE03 Phys.Rev. C 95, 014604 (2017) P.Descouvemont, L.F.Canto, M.S.Hussein Coulomb and nuclear effects in breakup and reaction cross sections NUCLEAR REACTIONS 208Pb(7Li, X), E(cm)=26.34, 42 MeV; calculated breakup and reaction σ(E), angular-momentum distribution of the breakup cross sections; deduced nuclear and Coulomb contributions. Continuum Discretized Coupled Channel (CDCC) method.
doi: 10.1103/PhysRevC.95.014604
2017TO02 Eur.Phys.J. A 53, 34 (2017) A.J.Toubiana, L.F.Canto, M.S.Hussein Improved WKB approximation for quantum tunneling: Application to heavy-ion fusion NUCLEAR REACTIONS 12C(6Li, x), E=1-6 MeV; calculated fusion σ using WKB-based extended Kemble approximation and using quantum mechanics.
doi: 10.1140/epja/i2017-12225-6
2017TO17 Phys.Rev. C 96, 064615 (2017) A.J.Toubiana, L.F.Canto, R.Donangelo, M.S.Hussein Scattering and fusion of identical heavy ions with arbitrary spin NUCLEAR REACTIONS 4He(α, α), (α, X), E=1.0, 1.5 MeV; calculated transverse isotropy (TI) energy and barrier height. 6Li(6Li, 6Li), (6Li, X), E(cm)=1-10 MeV; 7Li(7Li, 7Li), (7Li, X), E(cm)=1-15 MeV; 10B(10B, 10B), (10B, X), E(cm)=4.8, 7.8, 9.0 MeV; calculated transverse isotropy (TI) energy, barrier height, second derivatives of the differential σ for elastic scattering, angular distributions, fusion σ(E) and oscillations in energy in the fusion cross section. 12C(12C, 12C), (12C, X), VB=6.1 MeV; 24Mg(24Mg, 24Mg), (24Mg, X), VB=21.8 MeV; calculated barrier parameters. Akyuz-Winther (AW) and Woods-Saxon (WS) potential parametrizations.
doi: 10.1103/PhysRevC.96.064615
2016GO11 Few-Body Systems 57, 165 (2016) P.R.S.Gomes, J.Lubian, L.F.Canto, D.R.Otomar, D.R.Mendes, Jr., P.N.de Faria, R.Linares, L.Sigaud, J.Rangel, J.L.Ferreira, E.Ferioli, B.Paes, E.N.Cardozo, M.R.Cortes, M.J.Ermamatov, P.Lotti, M.S.Hussein Reactions with Weakly Bound Nuclei, at near Barrier Energies, and the Breakup and Transfer Influences on the Fusion and Elastic Scattering
doi: 10.1007/s00601-015-1036-2
2016GO12 Few-Body Systems 57, 205 (2016) P.R.S.Gomes, D.R.Mendes, Jr., L.F.Canto, J.Lubian, P.N.de Faria Reduction Methods for Total Reaction Cross Sections
doi: 10.1007/s00601-015-1042-4
2016HU03 Few-Body Systems 57, 195 (2016) M.S.Hussein, L.F.Canto, R.Donangelo, W.Mittig Disappearance of Mott Oscillations in-Sub-barrier Elastic Scattering of Identical Nuclei and Atomic Ions NUCLEAR REACTIONS 4He(α, α), 6li(6Li, 6Li), 10B(10B, 10B), E<10 MeV; calculated Mott oscillations, transverse isotropy, critical value of Sommerfeld parameter. Comparison with available data.
doi: 10.1007/s00601-015-1041-5
2016RA18 Phys.Rev. C 93, 054610 (2016) J.Rangel, J.Lubian, L.F.Canto, P.R.S.Gomes Effect of Coulomb breakup on the elastic cross section of the 8B proton-halo projectile on a heavy, 208Pb target NUCLEAR REACTIONS 208Pb(8B, 8B), (8B, X), E=170.3, 60, 44 MeV; calculated elastic, breakup and non-capture breakup differential σ(θ), polarization potentials, ground-state wavefunction of relative motion of the halo nucleon with respect to the core. Compared effects of the breakup channel in proton-halo and neutron-halo nuclei. Comparison with available experimental data. Continuum discretized coupled-channel (CDCC) calculations.
doi: 10.1103/PhysRevC.93.054610
2015CA10 Phys.Rev. C 92, 014626 (2015) L.F.Canto, D.R.Mendes, Jr., P.R.S.Gomes, J.Lubian Reduction of fusion and reaction cross sections at near-barrier energies NUCLEAR REACTIONS 27Al, 64Zn(7Li, X), 209Bi(6Li, X), 144,154Sm(16O, X), 208Pb(40Ca, X), E not given; calculated reduced fusion excitation functions. 9Be(6He, X), 27Al(6He, X), (6Li, X), (7Li, X), (7Be, X), (9Be, X), (16O, X), 40Ca(16O, X), 58Ni(α, X), (6He, X), (6Li, X), (7Be, X), (8B, X), (16O, X), (18O, X), (64Ni, X), 90Zr(6Li, X), 64Zn(9Be, X), (10Be, X), (11Be, X), 120Sn(α, X), (6He, X), (16O, X), 138Ba(6Li, X), (7Li, X), (16O, X), 144Sm(α, X), (9Be, X), (16O, X), 154Sm(16O, X), 197Au(α, X), 208Pb(α, X), (6He, X), (9Be, X), (12C, X), (16O, X), (17F, X), 209Bi(α, X), (6He, X), (6Li, X), (7Li, X), (11B, X), (12C, X), (16O, X), E not given; analyzed experimental fusion reaction cross section data by traditional, and fusion function methods. Single-channel calculations based on standard optical potentials and fusion function method.
doi: 10.1103/PhysRevC.92.014626
2015DE04 Phys.Rev. C 91, 024606 (2015) P.Descouvemont, T.Druet, L.F.Canto, M.S.Hussein Low-energy 9Be 208Pb scattering, breakup, and fusion within a four-body model NUCLEAR STRUCTURE 9Be; calculated electric quadrupole moment, magnetic dipole moment, rms radius, B(E2), pseudostates using the hyperspherical coordinate method for α+α+n three-body model. Comparison with experimental data. NUCLEAR REACTIONS 208Pb(9Be, 9Be), (9Be, X), E=38, 50 MeV; calculated elastic scattering σ(θ), fusion σ, breakup σ using continuum discretized coupled channel method. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.024606
2015OT03 Phys.Rev. C 92, 064609 (2015) D.R.Otomar, P.R.S.Gomes, J.Lubian, L.F.Canto, M.S.Hussein Theoretical study of the elastic breakup of weakly bound nuclei at near-barrier energies NUCLEAR REACTIONS 59Co, 144Sm, 208Pb(7Li, 7Li), (7Li, X), (6Li, 6Li), (6Li, X), E/VB=0.84-1.30; calculated σ(θ) at 33 MeV, integrated, total, Coulomb and nuclear breakup cross sections, ratio between Coulomb and nuclear breakup cross sections as a function of incident beam energy. Breakup of weakly bound nuclei into a two-cluster projectile. Coulomb-nuclear interference. Scaling laws. Continuum discretized coupled channel (CDCC) calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.92.064609
2014CA02 Phys.Rev. C 89, 024610 (2014) L.F.Canto, M.S.Hussein, W.Mittig Disappearance of Mott oscillations in sub-barrier elastic scattering of identical heavy ions, and the nuclear interaction NUCLEAR REACTIONS 4He(α, α), E=2.0, 3.0, 3.84, 5.26.6.47, 7.47, 8.87, 9.88, 10.88, 11.88, 12.3, 15.2 MeV; analyzed σ(θ) data; deduced sensitivity of Mott cross section to short-range nuclear interaction. Transverse isotropy.
doi: 10.1103/PhysRevC.89.024610
2014CA14 Eur.Phys.J. A 50, 89 (2014) L.F.Canto, P.R.S.Gomes, J.Lubian, M.S.Hussein, P.Lotti Assessing the adequacy of the bare optical potential in near-barrier fusion calculation NUCLEAR REACTIONS 209Bi(α, x), E=15-30 MeV; calculated fusion σ using single-channel and CC calculations with different potentials. Compared to data. 238U(6He, x); calculated halo nucleus fusion σ using single-channel with different potentials with and without considering halo. 144Sm(16O, x), E≈55-85 MeV;209Bi(6He, x), E≈18-30 MeV; calculated fusion σ, halo nucleus fusion σ using single-channel and CC calculations; deduced potential barrier parameters. Compared with data and 1/E trend.
doi: 10.1140/epja/i2014-14089-6
2014MA12 Phys.Rev. C 89, 034625 (2014) H.D.Marta, L.F.Canto, R.Donangelo Complete and incomplete fusion of weakly bound nuclei NUCLEAR REACTIONS 209Bi(6Li, X), (7Li, X), E=25-50 MeV; calculated complete and total fusion σ(E), incomplete fusion + transfer σ(E). Semi-classical model to study the effect of breakup process in the fusion reaction of a weakly bound projectile with a heavy target. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.034625
2013HU09 Phys.Rev. C 88, 047601 (2013) M.S.Hussein, P.R.S.Gomes, J.Lubian, D.R.Otomar, L.F.Canto Scaling laws for near-barrier Coulomb and nuclear breakup NUCLEAR REACTIONS 59Co, 120Sn, 144Sm, 208Pb(6Li, X), E/VB=0.84, 1.0, 1.07, 2.07, 2.99; calculated nuclear breakup σ(E) as function of A and Z for incident beam energy near Coulomb barrier VB, and compared with experimental data; validation by continuum-discretized coupled-channels (CDCC) calculations. Scaling laws.
doi: 10.1103/PhysRevC.88.047601
2013OT01 Phys.Rev. C 87, 014615 (2013) D.R.Otomar, P.R.S.Gomes, J.Lubian, L.F.Canto, M.S.Hussein Nuclear and Coulomb breakup of the weakly bound 6Li nucleus with targets in the range from A=59 to 208 NUCLEAR REACTIONS 59Co(6Li, X), (6Li, 6Li), E=11, 13, 14 MeV; 144Sm(6Li, X), (6Li, 6Li), E=225, 25, 27 MeV; 208Pb(6Li, X), (6Li, 6Li), E=27, 29, 33 MeV; calculated elastic σ(θ, E), breakup σ(θ, E), integrated breakup σ, Coulomb breakup and fusion σ(E). Continuum discretized coupled channel (CDCC) calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.87.014615
2012GO18 J.Phys.(London) G39, 115103 (2012) P.R.S.Gomes, D.R.Otomar, T.Correa, L.F.Canto, J.Lubian, R.Linares, D.H.Luong, M.Dasgupta, D.J.Hinde, M.S.Hussein Complete fusion enhancement and suppression of weakly bound nuclei at near barrier energies NUCLEAR REACTIONS 209Bi(6Li, X), (7Li, X), E not given; 144Sm(7Li, X), E∼25 MeV; analyzed available data; calculated the ratio between the complete fusion σ, dynamic polarization potential. Comparison with available data.
doi: 10.1088/0954-3899/39/11/115103
2011GO14 Int.J.Mod.Phys. E20, 929 (2011) P.R.S.Gomes, J.Lubian, L.F.Canto, L.C.Chamon, E.Crema, M.S.Hussein Fusion enhancement/suppression and irreversibility in reactions induced by weakly bound nuclei NUCLEAR REACTIONS 238U, 209Bi(6He, X), E<30 MeV; calculated fusion σ; deduced halo effects. comparison with experimental data.
doi: 10.1142/S021830131101899X
2010GO07 Nucl.Phys. A833, 156 (2010) A.Gomez Camacho, E.F.Aguilera, E.Martinez-Quiroz, P.R.S.Gomes, J.Lubian, L.F.Canto The Threshold Anomaly of weakly bound projectiles from recent elastic scattering measurements around the Coulomb barrier NUCLEAR REACTIONS 58Ni(6Li, 6Li), E=9.85, 11.21, 12.00, 12.13, 13.04, 14.00, 14.04, 16.00, 18.00, 20.00 MeV; 58Ni(7Be, 7Be), E=15.09, 17.13, 18.53, 19.93, 21.43 MeV; 58Ni(8B, 8B), E=20.7, 23.4, 25.3, 27.2, 29.3 MeV; calculated σ, σ(θ); deduced optical potential parameters. Compared Sao Paulo and Woods-Saxon potentials and experimental data. Discussed presence of Breakup Threshold Anomaly (BTA).
doi: 10.1016/j.nuclphysa.2009.12.002
2010GO14 Phys.Rev. C 82, 014616 (2010) A.Gomez Camacho, P.R.S.Gomes, J.Lubian, L.F.Canto Simultaneous analysis of near-barrier elastic scattering and fusion of 9Be with 27Al NUCLEAR REACTIONS 27Al(9Be, 9Be), (9Be, X), E(cm)=9.0-35.25 MeV; analyzed elastic σ(θ) and fusion σ, nuclear polarization potentials as a function of radius and energy. Optical model calculations. Comparison with results for 144Sm(9Be, 9Be), (9Be, X) reaction.
doi: 10.1103/PhysRevC.82.014616
2010GO19 Nucl.Phys. A834, 151c (2010) P.R.S.Gomes, L.F.Canto, L.Lubian, P.Lotti, L.C.Chamon, E.Crema, J.M.B.Shorto Breakup Coupling Effects on Fusion of Weakly Bound Nuclei NUCLEAR REACTIONS 27Al, 144Sm, 208Pb(9Be, X), 59Co, 64Zn, 209Bi(6Li, X), (7Li, X), 64Zn(α, X), 64Zn, 209Bi, 238U(6He, X), 154Sm(16O, X), (32S, X), 208Pb(17F, X), E not given; analyzed fusion function, reduced σ; calculated universal fusion function. Comparison with data.
doi: 10.1016/j.nuclphysa.2009.12.026
2010LU09 Nucl.Phys. A834, 802c (2010) L.Lubian, T.Correa, P.R.S.Gomes, L.F.Canto, M.S.Hussein Interplay between the 8B breakup and other reaction mechanisms by means of CDCC method NUCLEAR REACTIONS 58Ni(8B, 8B), E=23.4 MeV; 58Ni(8B, α)4Li, E=30 MeV; calculated σ(θ) using CDCC code FRESCO; deduced polarization potentials for E=18-30 MeV. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.151
2010SH07 Phys.Rev. C 81, 044601 (2010) J.M.B.Shorto, P.R.S.Gomes, J.Lubian, L.F.Canto, P.Lotti Transfer coupling or neck formation effects on sub-barrier fusion NUCLEAR REACTIONS 154Sm(16O, X), E(cm)=50-100 MeV; 154Sm(28Si, X), E(cm)=90-125 MeV; 154Sm(32S, X), E(cm)=100-130 MeV; 154Sm(48Ca, X), E(cm)=120-160; 74Ge(58Ni, X), E(cm)=95-125 MeV; 74Ge(74Ge, X), E(cm)=105-155 MeV; 132Sn(64Ni, X), E(cm)=150-200 MeV; calculated σ using coupled channel method and optical model. Comparison with experimental data and with universal fusion function (UFF).
doi: 10.1103/PhysRevC.81.044601
2009CA01 J.Phys.(London) G36, 015109 (2009) L.F.Canto, P.R.S.Gomes, J.Lubian, L.C.Chamon, E.Crema Disentangling static and dynamic effects of low breakup threshold in fusion reactions NUCLEAR REACTIONS 209Bi, 238U(α, X), (6He, X), 16O, 59Co, 209Bi(6Li, X), 16O, 209Bi(7Li, X), 16O(11Li, X), 27Al, 208Pb(9Be, X), 144,154Sm(16O, X), E not given; analyzed fusion cross sections. Deduced universal fusion functions. Coupled channel calculations.
doi: 10.1088/0954-3899/36/1/015109
2009CA09 Phys.Rev. C 79, 037601 (2009) Improved determination of the fusion barrier distribution NUCLEAR REACTIONS 144Sm(16O, X); calculated fusion barrier distribution and uncertainties associated with barrier distributions.
doi: 10.1103/PhysRevC.79.037601
2009CA10 Nucl.Phys. A821, 51 (2009) L.F.Canto, P.R.S.Gomes, J.Lubian, L.C.Chamon, E.Crema Dynamic effects of breakup on fusion reactions of weakly bound nuclei NUCLEAR REACTIONS 209Bi(α, X), (6He, X), E(cm)=16-30 MeV; 209Bi(16O, X), (40Ca, X), E≈100-200 MeV; 27Al, 59Co, 63Cu, 64Zn, 238U(α, X), 27Al, 64Zn, 238U(6He, X), 16O(6Li, X), 59Co(6Li, X), (7Li, X), 27Al, 64Zn, 144Sm, 208Pb, 209Bi, 238U(6Li, X), (7Li, X), (9Be, X), 27Al, 144,154Sm, 208Pb(16O, X), 209Bi(10Be, X), (11Be, X), 208Pb(17F, X), (19F, X), 144Sm(40Ca, X), 154Sm(32S, X), E not given; analyzed fusion σ; calculated universal fusion function. Coupled channel calculations.
doi: 10.1016/j.nuclphysa.2009.02.001
2009CA21 Phys.Rev. C 80, 034615 (2009) L.F.Canto, P.R.S.Gomes, J.Lubian, P.Lotti, L.C.Chamon, E.Crema Barrier distributions for weakly bound systems NUCLEAR REACTIONS 144Sm, 148Sm, 154Sm(16O, X), 208Pb(9Be, X), 209Bi(6Li, X), (7Li, X), E not given; analyzed fusion function barrier distributions.
doi: 10.1103/PhysRevC.80.034615
2009CA25 Phys.Rev. C 80, 047601 (2009) L.F.Canto, J.Lubian, P.R.S.Gomes, M.S.Hussein Continuum-continuum coupling and polarization potentials for weakly bound systems NUCLEAR REACTIONS 208Pb(11Be, X), E(cm)=30-50 MeV; analyzed complete fusion σ. 58Ni(8B, X), E(cm)=20.8, 26.4 MeV; analyzed σ(θ) and polarization potential for different processes. Continuum discretized coupled channels method used in the analyses.
doi: 10.1103/PhysRevC.80.047601
2009GA32 Phys.Rev. C 80, 037602 (2009) V.N.Garcia, J.Lubian, P.R.S.Gomes, A.Gomez-Camacho, L.F.Canto 9Be breakup polarization potential at near-barrier energies NUCLEAR REACTIONS 144Sm(9Be, X), E=33-41 MeV; calculated complete fusion σ, real and imaginary parts of the dynamic polarization potentials using an approximate phenomenological treatment. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.037602
2009GO08 Phys.Rev. C 79, 027606 (2009) P.R.S.Gomes, J.Lubian, L.F.Canto Breakup effects in fusion reactions of stable weakly bound nuclei and light targets NUCLEAR REACTIONS 12C, 13C, 27Al, 59Co, 64Zn(6Li, X), (7Li, X), 28Si(7Li, X), 27Al(7Be, X), 27Al, 64Zn(9Be, X), E not given; calculated universal fusion functions (UFF). Analyzed effects of breakup coupling on fusion cross sections. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.027606
2009GO35 Nucl.Phys. A828, 233 (2009) P.R.S.Gomes, J.Lubian, B.Paes, V.N.Garcia, D.S.Monteiro, I.Padron, J.M.Figueira, A.Arazi, O.A.Capurro, L.Fimiani, A.E.Negri, G.V.Marti, J.O.Fernandez Niello, A.Gomez-Camacho, L.F.Canto Near-barrier fusion, breakup and scattering for the 9Be + 144Sm system NUCLEAR REACTIONS 144Sm(9Be, X), E=3048 MeV; measured fusion and elastic σ, σ(θ), σ(E). 144Sm(9Be, X), (16O, X), E=3048 MeV; analyzed fusion σ, breakup mechanism; deduced universal fusion function. Delayed X-ray technique. Coupled channel calculations.
doi: 10.1016/j.nuclphysa.2009.07.008
2009LU12 Phys.Rev. C 79, 064605 (2009) J.Lubian, T.Correa, E.F.Aguilera, L.F.Canto, A.Gomez-Camacho, E.M.Quiroz, P.R.S.Gomes Effects of breakup couplings on 8B+58Ni elastic scattering NUCLEAR REACTIONS 58Ni(8B, 8B), E=20.7, 23.4, 25.3, 27.2, 29.3 MeV; analyzed σ(θ) data using continuum discretized coupled-channel calculations.
doi: 10.1103/PhysRevC.79.064605
2008CA08 Phys.Rev. C 77, 034609 (2008) W.H.Z.Cardenas, M.S.Hussein, L.F.Canto, J.Lubian Local approximations for polarization potentials NUCLEAR REACTIONS 12C(11Li, X), E(cm)=1-6 MeV; calculated polarization potentials, angular distributions, fusion excitation functions. Feshbach formalism.
doi: 10.1103/PhysRevC.77.034609
2008LU16 Phys.Rev. C 78, 064615 (2008) J.Lubian, T.Correa, P.R.S.Gomes, L.F.Canto Effect of breakup on fusion cross sections of the 8B + 58Ni system by means of quasi-elastic angular distributions NUCLEAR REACTIONS 58Ni(8B, X), E=0-32 MeV; calculated quasi-elastic barrier distributions, fusion barrier distributions. Continuum discretized coupled channel calculations.
doi: 10.1103/PhysRevC.78.064615
2008MA41 Phys.Rev. C 78, 034612 (2008) H.D.Marta, L.F.Canto, R.Donangelo Semiclassical calculations of observable cross sections in breakup reactions NUCLEAR REACTIONS 58Ni(8B, 7Be), E=26 MeV; calculated σ(θ) using semi-classical procedure. Comparison with experimental data.
doi: 10.1103/PhysRevC.78.034612
2007CA29 Nucl.Phys. A787, 243c (2007) L.F.Canto, R.Donangelo, M.S.Hussein Theoretical treatments of fusion processes in collisions of weakly bound nuclei NUCLEAR REACTIONS 208Pb(11Be, X), E(cm)=30-50 MeV; 208Pb(6He, X), (6Li, X), E not given; analyzed fusion σ. Continuum discretized coupled channels model.
doi: 10.1016/j.nuclphysa.2006.12.039
2006CA02 Phys.Rep. 424, 1 (2006) L.F.Canto, P.R.S.Gomes, R.Donangelo, M.S.Hussein Fusion and breakup of weakly bound nuclei
doi: 10.1016/j.physrep.2005.10.006
2006CA03 Phys.Rep. 424, 1 (2006) L.F.Canto, P.R.S.Gomes, R.Donangelo, M.S.Hussein Fusion and breakup of weakly bound nuclei
doi: 10.1016/j.physrep.2005.10.006
2006CA14 Phys.Rev. C 73, 034608 (2006) L.F.Canto, R.Donangelo, H.D.Marta Semiclassical treatment of fusion processes in collisions of weakly bound nuclei NUCLEAR REACTIONS 238U(6He, X), E(cm)=15-35 MeV; calculated fusion σ. Semiclassical approach.
doi: 10.1103/PhysRevC.73.034608
2006CA16 Phys.Rev. C 73, 047603 (2006) W.H.Z.Cardenas, L.F.Canto, M.S.Hussein Low-energy transfer cross section for Borromean halo nuclei NUCLEAR REACTIONS 238U(6He, X), (6He, α), E(cm) ≈ 12-32 MeV; calculated fusion, transfer σ; deduced reaction mechanism features.
doi: 10.1103/PhysRevC.73.047603
2005CA45 Phys.Rev. C 72, 041603 (2005) B.V.Carlson, L.F.Canto, M.S.Hussein Semiclassical Coulomb interaction
doi: 10.1103/PhysRevC.72.041603
2005CA53 Braz.J.Phys. 35, 884 (2005) L.F.Canto, R.Donangelo, H.D.Marta Upper Bounds for Fusion Processes in Collisions of Weakly Bound Nuclei NUCLEAR REACTIONS 238U(6He, X), 209Bi(7Li, X), E(cm) ≈ 10-30 MeV; calculated fusion σ, upper bounds for contributions from incomplete fusion and sequential complete fusion.
doi: 10.1590/S0103-97332005000500045
2004CA51 Braz.J.Phys. 34, 859 (2004) B.V.Carlson, L.F.Canto, M.S.Hussein Semiclassical Coulomb Excitation Matrix Elements
doi: 10.1590/s0103-97332004000500040
2004HU05 Nucl.Phys. A731, 163 (2004) M.S.Hussein, B.V.Carlson, L.F.Canto Multiple giant resonances in nuclei: their excitation and decay NUCLEAR STRUCTURE 40Ca, 120Sn, 132Xe, 165Ho, 208Pb, 238U; calculated double and triple GDR excitation and decay features.
doi: 10.1016/j.nuclphysa.2003.11.029
2003CA39 Phys.Rev. C 68, 054614 (2003) W.H.Z.Cardenas, L.F.Canto, N.Carlin, R.Donangelo, M.S.Hussein Interplay of static and dynamic effects in 6He + 238U fusion NUCLEAR REACTIONS 238U(α, X), (6He, X), E(cm)=15-35 MeV; calculated fusion σ, role of neutron halo and breakup channel effects.
doi: 10.1103/PhysRevC.68.054614
2003HU14 Nucl.Phys. A722, 321c (2003) M.S.Hussein, L.F.Canto, R.Donangelo Fusion and breakup of halo nuclei
doi: 10.1016/S0375-9474(03)01384-8
2003LE36 Braz.J.Phys. 33, 328 (2003) A.Leistenschneider, T.Aumann, K.Boretzky, L.F.Canto, B.V.Carlson, D.Cortina, U.Datta Pramanik, Th.W.Elze, H.Emling, H.Geissel, A.Grunschloss, K.Helariutta, M.Hellstrom, M.S.Hussein, S.Ilievski, K.Jones, J.V.Kratz, R.Kulessa, H.K.Le, E.Lubkiewicz, G.Munzenberg, R.Palit, P.Reiter, C.Scheidenberger, K.-H.Schmidt, H.Simon, K.Summerer, E.Wajda, W.Walus Fragmentation of Exotic Oxygen Isotopes NUCLEAR STRUCTURE C, Pb(17O, X), (18O, X), (19O, X), (20O, X), (21O, X), E ≈ 600, 1700 MeV/nucleon; analyzed fragment yields. Abrasion-ablation models.
doi: 10.1590/s0103-97332003000200033
2002CA25 Nucl.Phys. A703, 633 (2002) W.H.Z.Cardenas, L.F.Canto, R.Donangelo, M.S.Hussein, J.Lubian, A.Romanelli Approximations in Fusion and Breakup Reactions Induced by Radioactive Beams NUCLEAR REACTIONS 12C(11Li, X), E(cm)=0.5-5 MeV; calculated fusion, breakup σ. Effects of several numerical approximations discussed.
doi: 10.1016/S0375-9474(01)01672-4
2002DE14 Phys.Rev. C65, 034326 (2002) E.J.V.de Passos, M.S.Hussein, L.F.Canto, B.V.Carlson Mean Energy, Strength, and Width of Triple Giant Dipole Resonances
doi: 10.1103/PhysRevC.65.034326
2002HU13 Phys.Rev. C66, 034615 (2002) M.S.Hussein, B.V.Carlson, L.F.Canto, A.F.R.de Toledo Piza Excitation of Triple Giant Resonances in Heavy-Ion Reactions NUCLEAR REACTIONS 208Pb(40Ca, 40Ca'), (120Sn, 120Sn'), (132Xe, 132Xe'), (165Ho, 165Ho'), (208Pb, 208Pb'), (238U, 238U'), E=100, 1000 MeV; calculated double and triple GDR excitation σ, coherent and fluctuation components, decay properties.
doi: 10.1103/PhysRevC.66.034615
2002LE19 Phys.Rev. C65, 064607 (2002) A.Leistenschneider, T.Aumann, K.Boretzky, L.F.Canto, B.V.Carlson, D.Cortina, U.D.Pramanik, Th.W.Elze, H.Emling, H.Geissel, A.Grunschloss, K.Helariutta, M.Hellstrom, M.S.Hussein, S.Ilievski, K.L.Jones, J.V.Kratz, R.Kulessa, L.H.Khiem, E.Lubkiewicz, G.Munzenberg, R.Palit, P.Reiter, C.Scheidenberger, K.-H.Schmidt, H.Simon, K.Summerer, E.Wajda, W.Walus Fragmentation of Unstable Neutron-Rich Oxygen Beams NUCLEAR REACTIONS C(17O, X), (18O, X), (19O, X), (20O, X), (21O, X), E ≈ 600 MeV/nucleon; measured fragments isotopic production σ; deduced isospin dependence in fragmentation process. Comparison with model predictions.
doi: 10.1103/PhysRevC.65.064607
2002MA53 Phys.Rev. C66, 024605 (2002) H.D.Marta, L.F.Canto, R.Donangelo, P.Lotti Validity of the semiclassical approximation for the breakup of weakly bound nuclei NUCLEAR REACTIONS 58Ni(8B, p7Be), E=26 MeV; calculated breakup σ(θ). Semiclassical method, comparison with previous results.
doi: 10.1103/PhysRevC.66.024605
2001DE48 Phys.Rev. C64, 064605 (2001) D.T.de Paula, T.Aumann, L.F.Canto, B.V.Carlson, H.Emling, M.S.Hussein Anharmonicities of Giant Dipole Excitations NUCLEAR REACTIONS 208Pb(208Pb, 208Pb'), E=640 MeV/nucleon; 208Pb(136Xe, 136Xe'), E=700 MeV/nucleon; calculated double GDR excitation σ enhancement factor; deduced role of anharmonic effects. Macroscopic model.
doi: 10.1103/PhysRevC.64.064605
1999CA14 Phys.Rev. C59, 2689 (1999) B.V.Carlson, L.F.Canto, S.Cruz-Barrios, M.S.Hussein, A.F.R.de Toledo Piza Coulomb Excitation of a Damped Oscillator and the Brink-Axel Mechanism
doi: 10.1103/PhysRevC.59.2689
1999CA26 Phys.Rev. C60, 014604 (1999) B.V.Carlson, M.S.Hussein, A.F.R.de Toledo Piza, L.F.Canto Theory of Multiple Giant Dipole Resonance Excitation NUCLEAR REACTIONS 208Pb(208Pb, 208Pb'), E=100-1000 MeV/nucleon; calculated multiple giant resonance excitation σ(E), related features; deduced role of incoherent contributions. Semiclassical description.
doi: 10.1103/PhysRevC.60.014604
1999CA42 Ann.Phys.(New York) 276, 111 (1999) B.V.Carlson, L.F.Canto, S.Cruz-Barrios, M.S.Hussein, A.F.R.de Toledo Piza Multiphonon and ' Hot ' -Phonon Isovector Electric-Dipole Excitations
doi: 10.1006/aphy.1999.5925
1999CA49 Phys.Rev. C60, 064624 (1999) L.F.Canto, B.V.Carlson, M.S.Hussein, A.F.R.de Toledo Piza Effective Widths and Effective Number of Phonons of Multiphonon Giant Resonances NUCLEAR REACTIONS 208Pb(208Pb, X), E=100-950 MeV/nucleon; calculated multiphonon giant resonance σ, effective widths. Direct plus fluctuation model.
doi: 10.1103/PhysRevC.60.064624
1999DE17 Phys.Rev. C59, 3093 (1999) A.F.R.de Toledo Piza, M.S.Hussein, B.V.Carlson, C.A.Bertulani, L.F.Canto, S.Cruz-Barrios Isospin Structure of One- and Two-Phonon Giant Dipole Resonance Excitations NUCLEAR REACTIONS 48Ca, 208Pb(208Pb, 208Pb'), E=640 MeV/nucleon; calculated σ for single, double GDR excitation following Coulomb excitation; deduced role of isospin degree of freedom.
doi: 10.1103/PhysRevC.59.3093
1998CA27 Phys.Rev. C58, 1107 (1998) L.F.Canto, R.Donangelo, L.M.de Matos, M.S.Hussein, P.Lotti Complete and Incomplete Fusion in Heavy Ion Collisions NUCLEAR REACTIONS 12C(6Li, X), (7Li, X), (9Be, X), E not given; calculated fusion σ; deduced projectile breakup effects. Coupled channels calculations.
doi: 10.1103/PhysRevC.58.1107
1997CA04 Phys.Rev. C55, R570 (1997) L.F.Canto, R.Donangelo, A.Romanelli, M.S.Hussein, A.F.R.de Toledo Piza Postacceleration in the Elastic Breakup of the Deuteron NUCLEAR REACTIONS 208Pb(d, X), E=25-300 MeV/nucleon; calculated projectile dissociation spectra, longitudinal velocity distribution; deduced postaccelration related features.
doi: 10.1103/PhysRevC.55.R570
1997CA52 J.Phys.(London) G23, 1465 (1997) L.F.Canto, R.Donangelo, M.S.Hussein, P.Lotti Complete and Incomplete Fusion of Two-Cluster Nuclei NUCLEAR REACTIONS, ICPND 12C(6Li, X), E not given; calculated complete, incomplete fusion σ(E); deduced projectile break-up role, halo nucleus implications.
doi: 10.1088/0954-3899/23/10/037
1997MA43 Int.J.Mod.Phys. E6, 301 (1997) H.D.Marta, L.F.Canto, R.Donangelo On the Effect of Transmission-Coefficients Approximations in Sub-Barrier Fusion NUCLEAR REACTIONS, ICPND 28Si(16O, X), E=20-32 MeV; calculated fusion σ(E); deduced transmission coefficients treatment role. Coupled channels approach, constant coupling, parabolic approximations.
doi: 10.1142/S0218301397000196
1997TA01 Phys.Rev.Lett. 78, 30 (1997) J.Takahashi, M.Munhoz, E.M.Szanto, N.Carlin, N.Added, A.A.P.Suaide, M.M.de Moura, R.Liguori Neto, A.Szanto de Toledo, L.F.Canto Is Fusion Inhibited for Weakly Bound Nuclei ( Question ) NUCLEAR REACTIONS 12C, 9Be(6Li, X), (7Li, X), E=6-33 MeV; measured evaporation residue spectra; deduced fusion probability vs E, effective separation energy.
doi: 10.1103/PhysRevLett.78.30
1996BE03 Phys.Rev. C53, 334 (1996) C.A.Bertulani, L.F.Canto, M.S.Hussein, A.F.R.de Toledo Piza Theory of Multiphonon Excitation in Heavy-Ion Collisions NUCLEAR REACTIONS 208Pb(208Pb, 208Pb'), E=640 MeV/nucleon; calculated GDR, other giant resonances excitation probability, σ ratio. Channel coupling, semi-classical method.
doi: 10.1103/PhysRevC.53.334
1996CA12 Phys.Rev. C53, 3147 (1996) L.F.Canto, R.Donangelo, A.Romanelli Direct Reaction Calculation of the 11Li Coulomb Dissociation Spectrum NUCLEAR REACTIONS 208Pb(11Li, X), E=28 MeV/nucleon; analyzed projectile dissociation data; deduced breakup mechanism. Two-cluster model, continuum discretization procedure.
doi: 10.1103/PhysRevC.53.3147
1996FA03 Nucl.Phys. A597, 387 (1996) A.R.Farhan, L.F.Canto, J.O.Rasmussen, P.Ring Form Factors for Two-Nucleon Transfer in the Diabolical Region of Rotating Nuclei
doi: 10.1016/0375-9474(95)00456-4
1996RA38 Phys.Rep. 264, 325 (1996) J.O.Rasmussen, S.Y.Chu, M.A.Stoyer, L.F.Canto, R.Donangelo, P.Ring Probes of Pairing Correlations by Heavy-Ion Two-Neutron Transfer Reactions NUCLEAR STRUCTURE 160,162,164Dy; calculated neutron excitations energies vs level spin, moment of inertia vs ω. Hamiltonian matrix diagonalization methods. NUCLEAR REACTIONS 162Dy(58Ni, 60Ni), E=345 MeV; 164,162Dy(116Sn, 118Sn), E=637 MeV; calculated neutron-pair transfer patterns, Eγ vs γ-multiplicity. 164,162Dy(58Ni, 60Ni), E=270 MeV; 164Dy(116Sn, 118Sn), E=470 MeV; calculated five lowest neutron band populations in final nucleus; deduced diabolic pair transfer related features. Hamiltonian matrix diagonalization methods.
doi: 10.1016/0370-1573(95)00046-1
1995BE47 Phys.Lett. 353B, 413 (1995) C.A.Bertulani, L.F.Canto, M.S.Hussein A Coupled-Channels Study of 11Be Coulomb Excitation NUCLEAR REACTIONS 208Pb(11Be, 11Be'), E=45 MeV/nucleon; analyzed Coulomb excitation σ; deduced channel coupling role, model parameters.
doi: 10.1016/0370-2693(95)00595-C
1995BR37 Ann.Phys.(New York) 243, 420 (1995) A.M.S.Breitschaft, V.C.Barbosa, L.F.Canto, M.S.Hussein, E.J.Moniz, J.Christley, I.J.Thompson Coupled-Channel Effects on Heavy-Ion Sub-Barrier Fusion within the Doorway Expansion Method NUCLEAR REACTIONS, ICPND 28Si(16O, X), E ≈ 20-36 MeV; calculated fusion σ(E); deduced coupled-channels role. Doorway expansion method.
doi: 10.1006/aphy.1995.1103
1995CA16 Nucl.Phys. A589, 117 (1995) L.F.Canto, R.Donangelo, P.Lotti, M.S.Hussein Dipole Polarizability of Neutron-Rich Nuclei NUCLEAR REACTIONS 208Pb(11Li, 11Li), E(cm)=50 MeV; calculated σ(θ); deduced Coulomb dipole polarizability. Coulomb coupling of channels.
doi: 10.1016/0375-9474(95)00072-9
1995CA39 Phys.Rev. C52, R2848 (1995) L.F.Canto, R.Donangelo, P.Lotti, M.S.Hussein Effect of Coulomb Dipole Polarizability of Halo Nuclei on Their Near-Barrier Fusion with Heavy Targets NUCLEAR REACTIONS, ICPND 208Pb(11Li, X), E(cm)=15-40 MeV; calculated fusion σ(E); deduced 11Li breakup, Coulomb dipole polarizability roles.
doi: 10.1103/PhysRevC.52.R2848
1995CH35 Phys.Rev. C52, 685 (1995) S.Y.Chu, J.O.Rasmussen, M.A.Stoyer, L.F.Canto, R.Donangelo, P.Ring Multiband Theory for Heavy-Ion Neutron-Pair Transfer Among Deformed Gd Nuclei NUCLEAR REACTIONS 156Gd(58Ni, 60Ni), (206Pb, 208Pb), (206Pb, 204Pb), E not given; calculated two-neutron pair extraction, deposition amplitudes. Multi-band theory.
doi: 10.1103/PhysRevC.52.685
1995CH38 Phys.Rev. C52, 1407 (1995) S.Y.Chu, J.O.Rasmussen, M.A.Stoyer, P.Ring, L.F.Canto Multiparticle-Rotor Model for Rotational Band Structure of 154Gd NUCLEAR STRUCTURE 154Gd; calculated levels, moments of inertia vs angular velocity; analyzed band crossing phenomena. Multi-particle rotor model.
doi: 10.1103/PhysRevC.52.1407
1995HU12 Nucl.Phys. A588, 85c (1995) M.S.Hussein, C.A.Bertulani, L.F.Canto, R.Donangelo, M.P.Pato, A.F.R.de Toledo Piza, and the Rio-Sao Paulo Theory (RSPT) Collaboration Fusion of Halo Nuclei NUCLEAR REACTIONS, ICPND 208Pb(11Li, X), E(cm)=10-40 MeV; calculated fusion σ(E). Coupling to soft dipole mode, breakup channels.
doi: 10.1016/0375-9474(95)00104-9
1995MA86 Int.J.Mod.Phys. E4, 153 (1995) H.D.Marta, L.F.Canto, R.Donangelo Average Trajectory Semiclassical Theory of Heavy Ion Collisions NUCLEAR REACTIONS 160Gd(40Ar, 40Ar'), E=140-180 MeV; calculated rotational levels excitation probability vs spin, E. Average trajectory semi-classical theory, comparison to coupled-channels approach.
doi: 10.1142/S0218301395000067
1995RO13 Nucl.Phys. A588, 71c (1995) A.Romanelli, L.F.Canto, R.Donangelo, P.Lotti Coulomb Dissocation of 11Li NUCLEAR REACTIONS 208Pb(11Li, X), E=28 MeV/nucleon; analyzed dissocation energy spectrum data. Coupled-channels approach, semi-classical treatment.
doi: 10.1016/0375-9474(95)00101-6
1994AB32 Int.J.Mod.Phys. E3, 783 (1994) G.Abal, L.F.Canto, R.J.Donangelo A Mass Parameter for Nuclear Collective Motion from the Generator Coordinate Method NUCLEAR STRUCTURE A=12-100; calculated mass parameter; deduced shell effects evidence. Generator coordinate method.
doi: 10.1142/S0218301394000218
1994BR39 Ann.Phys.(New York) 234, 162 (1994) A.M.S.Breitschaft, L.F.Canto, H.Schechter, M.S.Hussein, E.J.Moniz Doorway State Expansion Approach to Coupled Channels Problems and Application to Heavy Ions NUCLEAR REACTIONS 28Si(16O, 16O), (16O, 16O'), E(cm)=55 MeV; calculated S-matrix. Doorway expansion method, extension to coupled-channels, comparison with DWBA.
doi: 10.1006/aphy.1994.1077
1994CA17 Phys.Rev.Lett. 72, 2147 (1994) L.F.Canto, A.Romanelli, M.S.Hussein, A.F.R.de Toledo Piza Heavy-Ion Excitation of One- and Two-Phonon Giant Dipole States as an Exit Doorway Phenomenon NUCLEAR REACTIONS 208Pb(136Xe, X), E=690 MeV/nucleon; calculated giant, double giant resonance total σ vs Γ.
doi: 10.1103/PhysRevLett.72.2147
1993CA13 Phys.Rev. C47, 2836 (1993) L.F.Canto, P.Ring, Y.Sun, J.O.Rasmussen, S.Y.Chu, M.A.Stoyer Diabolic Effects on Nuclear Rotational State Population in Two-Neutron Transfer NUCLEAR REACTIONS 154,156,158Gd, 172,174,176Hf(206Pb, X), E not given; calculated two-nucleon transfer probabilities vs spin; deduced diabolic effects features.
doi: 10.1103/PhysRevC.47.2836
1993CA34 Phys.Lett. 318B, 415 (1993) L.F.Canto, R.Donangelo, A.Romanelli, H.Schulz A Coupled-Channels Study of 11Li Coulomb Dissociation NUCLEAR REACTIONS Pb(11Li, X), E=28 MeV/nucleon; analyzed projectile breakup data; deduced continuum-continuum coupling role. Coupled-channels approach, semi-classical approximation, breakup into 9Li+2n.
doi: 10.1016/0370-2693(93)91533-S
1993HU02 Phys.Rev. C47, 2398 (1993) M.S.Hussein, M.P.Pato, L.F.Canto, R.Donangelo Real Part of the Polarization Potential for 11Li-Induced Fusion Reactions NUCLEAR REACTIONS 208Pb(11Li, X), E(cm)=10-40 MeV; calculated two-neutron removal polarization potential strength vs l, fusion σ(E).
doi: 10.1103/PhysRevC.47.2398
1992AD02 Nucl.Phys. A540, 328 (1992) N.Added, R.M.Dos Anjos, N.Carlin, L.Fante, Jr., M.C.S.Figueira, R.Matheus, E.M.Szanto, A.Szanto de Toledo, M.S.Hussein, C.A.Bertulani, L.F.Canto Direct Versus Statistical Break-Up Processes in the 16,18O + 27Al, 28Si Reactions at E/A ≤ 4 MeV NUCLEAR REACTIONS 27Al(18O, αX), 27Al, 28Si(16O, αX), E=48-64 MeV; measured Eα, σ(fragment θ, θα) for X=12,14C; deduced breakup, incomplete fusion yields. Direct, statistical models.
doi: 10.1016/0375-9474(92)90207-Z
1992BE04 Nucl.Phys. A539, 163 (1992) Semiclassical Calculation of Coulomb Break-Up of Weakly-Bound Nuclei NUCLEAR REACTIONS 208Pb(11Li, X), E=100 MeV/nucleon; calculated Coulomb breakup probability vs impact parameter. 208Pb(11Li, X), E=69.9-790 MeV/nucleon; calculated Coulomb breakup σ. Semi-classical coupled-channels model.
doi: 10.1016/0375-9474(92)90240-K
1992BE15 Phys.Rev. C45, 2995 (1992) C.A.Bertulani, L.F.Canto, M.S.Hussein Closed Form Theory of Elastic Breakup and Applications to Astrophysically Relevant Heavy Ion Reactions NUCLEAR REACTIONS 28Si(16O, α12C), E=64 MeV; calculated σ(θα, θ(12C)). Closed form theory, separable approximation, breakup process.
doi: 10.1103/PhysRevC.45.2995
1992CA20 Nucl.Phys. A542, 131 (1992) L.F.Canto, R.Donangelo, M.S.Hussein, M.P.Pato The Nuclear Two-Neutron Removal Cross-Section of 11Li A Dynamic Polarization Potential Approach NUCLEAR STRUCTURE 11Li; calculated two-neutron removal dynamic polarization potential. A ≤ 250; calculated two-neutron removal σ vs mass, 11Li induced reactions. NUCLEAR REACTIONS 12C(11Li, X), E ≤ 150 MeV/nucleon; calculated breakup σ(E). Dynamic polarization potential.
doi: 10.1016/0375-9474(92)90402-6
1992FI04 Phys.Rev. C46, 1139 (1992) M.C.S.Figueira, E.M.Szanto, A.Szanto de Toledo, M.P.Pato, M.S.Hussein, L.F.Canto Role of the Breakup Process in the Hindrance of Light-Heavy-Ion Fusion Reactions NUCLEAR REACTIONS, ICPND 29Si(9Be, X), E(cm) ≈ 10-30 MeV; calculated fusion σ(E). 29Si(9Be, X), 19F(19F, X), 26Mg(12C, X), 27Al(11B, X), E(cm)=25 MeV; 10,11B, 12C, 28Si(9Be, X), E not given; calculated σ(fusion)/σ(reaction) vs cluster separation energy. One dimensional barrier penetration model, modified transmission coefficient.
doi: 10.1103/PhysRevC.46.1139
1992HU03 Phys.Rev. C46, 377 (1992) M.S.Hussein, M.P.Pato, L.F.Canto, R.Donangelo Near-Barrier Fusion of 11Li with Heavy Spherical and Deformed Targets NUCLEAR REACTIONS, ICPND 208Pb(11Li, X), E(cm)=10-40 MeV; 238U(11Li, X), E(cm)=10-45 MeV; calculated fusion σ(E); deduced structure near barrier. Coupled-channels description.
doi: 10.1103/PhysRevC.46.377
1991CA14 Nucl.Phys. A529, 243 (1991) L.F.Canto, R.Donangelo, M.S.Hussein Eikonal Form of the Dynamic Polarization Potential and Its Application to the Scattering of Exotic Nuclei NUCLEAR REACTIONS 12C(11Li, 11Li), E=85 MeV/nucleon; calculated σ(θ). Dynamic polarization potential, eikonal form.
doi: 10.1016/0375-9474(91)90794-7
1991RA12 Z.Phys. A339, 141 (1991) J.O.Rasmussen, M.A.Stoyer, L.F.Canto, R.Donangelo, P.Ring Nuclear Rotational Population Patterns in Heavy-Ion Scattering and Transfer Reactions NUCLEAR REACTIONS 238Pu(90Zr, 90Zr'), E=480-520 MeV; calculated rotational state population patterns, Coulomb excitation.
doi: 10.1007/BF01282943
Back to query form [Next] |