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NSR database version of May 24, 2024.

Search: Author = L.F.Canto

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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
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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
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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
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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
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2021CA10      Eur.Phys.J. A 57, 11 (2021)

L.F.Canto, K.Hagino, M.Ueda

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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,, 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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2009CA09      Phys.Rev. C 79, 037601 (2009)

L.F.Canto, R.Donangelo

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
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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
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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
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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
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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
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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
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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=3048 MeV; measured fusion and elastic σ, σ(θ), σ(E). 144Sm(9Be, X), (16O, X), E=3048 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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0583.

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0407.

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
Citations: PlumX Metrics

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1992BE04      Nucl.Phys. A539, 163 (1992)

C.A.Bertulani, L.F.Canto

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
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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
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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
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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
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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
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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
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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
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