NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.S.Hussein Found 199 matches. Showing 1 to 100. [Next]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
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
2018LI67 Eur.Phys.J. A 54, 221 (2018) V.Liccardo, M.Malheiro, M.S.Hussein, B.V.Carlson, T.Frederico Nuclear processes in astrophysics: Recent progress
doi: 10.1140/epja/i2018-12648-5
2018ZA02 Phys.Rev. C 97, 054608 (2018) V.A.B.Zagatto, F.Cappuzzello, J.Lubian, M.Cavallaro, R.Linares, D.Carbone, C.Agodi, A.Foti, S.Tudisco, J.S.Wang, J.R.B.Oliveira, M.S.Hussein Important role of projectile excitation in 16O + 60Ni and 16O + 27Al scattering at intermediate energies NUCLEAR REACTIONS 60Ni(16O, 16O), (16O, 16O'), E=260 MeV; 27Al(16O, 16O), (16O, 16O'), E=100, 280 MeV; measured scattered particles, σ(θ, E) for elastic scattering, and inelastic scattering to the first 2+ and 3- states in 60Ni and five low-lying states in 27Al using MAGNEX spectrometer at INFN-LNS-Catania; deduced summed total inelastic cross sections; calculated real and imaginary polarization potential shapes for several calculations. Comparison of cross section data with coupled-channel calculations using deformed optical potential.
doi: 10.1103/PhysRevC.97.054608
2017BA17 Eur.Phys.J. A 53, 126 (2017) Dipole-dipole dispersion interactions between neutrons NUCLEAR STRUCTURE 1n; calculated electric, magnetic polarizability vs photon energy, CP-interaction between two neutrons, neutron and a wall, neutron and two walls.
doi: 10.1140/epja/i2017-12313-7
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
2017HU06 Eur.Phys.J. A 53, 110 (2017) Two-step nuclear reactions: The Surrogate Method, the Trojan Horse Method and their common foundations
doi: 10.1140/epja/i2017-12321-7
2017HU16 Acta Phys.Pol. B48, 1837 (2017) The Casimir-Polder Interaction Between Two Neutrons and Possible Relevance to Tetraneutron States
doi: 10.5506/APhysPolB.48.1837
2017PO13 Eur.Phys.J. A 53, 178 (2017) G.Potel, G.Perdikakis, B.V.Carlson, M.C.Atkinson, W.H.Dickhoff, J.E.Escher, M.S.Hussein, J.Lei, W.Li, A.O.Macchiavelli, A.M.Moro, F.M.Nunes, S.D.Pain, J.Rotureau Toward a complete theory for predicting inclusive deuteron breakup away from stability NUCLEAR REACTIONS 93Nb(d, pn), E=10, 25.5 MeV; calculated σ(ln), σ(θn) assuming both elastic and nonelastic breakup. Compared with published calculations. 40,48,60Ca(d, pn), E=20, 40 MeV; calculated σ(Ep) vs En and vs ln using both elastic and nonelastic breakup and using Hussein-McVoy theory.
doi: 10.1140/epja/i2017-12371-9
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
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
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
2013DE26 Phys.Rev.Lett. 111, 082701 (2013) Towards a Microscopic Description of Reactions Involving Exotic Nuclei NUCLEAR REACTIONS 208Pb(7Li, 7Li), (7Li, 7Li'), E=27, 35 MeV; calculated σ(θ). Microscopic generalization of the continuum discretized coupled channels method, comparison with available data.
doi: 10.1103/PhysRevLett.111.082701
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
2010BA35 Nucl.Phys. A834, 599c (2010) E.Bauer, A.P.Galeao, M.S.Hussein, F.Krmpotic Weak nonmesonic decay spectra of hypernuclei RADIOACTIVITY 4,5He, 12C, 16O, 28Si(p); calculated energy spectra, p-spectra for non-mesonic weak decay of hypernuclei. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.103
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
2009AN15 Phys.Rev. C 80, 034610 (2009) Jensen inequalities for tunneling probabilities in complex systems NUCLEAR REACTIONS 2H(d, X), E=0-0.45 MeV; 3H(t, X), E=0-0.375 MeV; 64Ni(64Ni, X), E=90-102 MeV; 150Sm(16O, X), E=55-67 MeV; calculated tunneling probabilities using the Jensen inequality.
doi: 10.1103/PhysRevC.80.034610
2009BA16 Phys.Lett. B 674, 103 (2009) E.Bauer, A.P.Galeao, M.S.Hussein, F.Krmpotic, J.D.Parker Nonmesonic weak decay spectra of 4ΛHe NUCLEAR STRUCTURE 4H, 4,5He; calculated hypernucleus non-mesonic weak decay widths, particle energy spectra and related features based on an independent-particle shell model. Comparison with data and other models.
doi: 10.1016/j.physletb.2009.01.072
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
2008BA40 Phys.Rev. C 78, 044312 (2008), Publishers note Phys.Rev. C 78, 059902 (2008) C.Barbero, A.P.Galeao, M.S.Hussein, F.Krmpotic Kinetic energy sum spectra in nonmesonic weak decay of hypernuclei NUCLEAR STRUCTURE 4,5He, 12C, 16O, 28Si; calculated energy spectra in the nonmesonic weak decay of hypernuclei. Independent-particle shell model.
doi: 10.1103/PhysRevC.78.044312
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
2008HU06 Phys.Rev. C 77, 054609 (2008) Exit doorway model for nuclear elastic breakup of weakly bound projectiles NUCLEAR REACTIONS A=5-210(7Be, X), E=100 MeV/nucleon; A=5-210(8B, X), E=44 MeV/nucleon; A=5-210(11Be, X), E=200 MeV/nucleon; calculated deformation parameters, σ. Doorway model for elastic breakup process.
doi: 10.1103/PhysRevC.77.054609
2007BE19 Phys.Lett. B 647, 30 (2007) E.A.Benjamim, A.Lepine-Szily, D.R.Mendes, Jr., R.Lichtenthaler, V.Guimaraes, P.R.S.Gomes, L.C.Chamon, M.S.Hussein, A.M.Moro, A.Arazi, I.Padron, J.Alcantara Nunez, M.Assuncao, A.Barioni, O.Camargo, Jr., R.Z.Denke, P.N.de Faria, K.C.C.Pires Elastic scattering and total reaction cross section for the 6He + 27Al system NUCLEAR REACTIONS 27Al(6He, 6He), E=9.5, 11.0, 12.0, 13.4 MeV; measured σ, σ(θ). 6He deduced radius, deformation parameters. 27Al(6Li, 6Li), (7Li, 7Li), (9Be, 9Be), (16O, 16O), E≈7-45 MeV; analysed total σ. 6,7Li, 9Be, 16O deduced deformation parameters. Sao Paulo potential.
doi: 10.1016/j.physletb.2007.01.048
2007BE58 Phys.Rev. C 76, 051602 (2007) Geometry of Borromean halo nuclei NUCLEAR STRUCTURE 6He, 11Li, 14Be, 17Ne; analyzed B(E1), rms charge radii; deduced geometry and angle between halo neutrons.
doi: 10.1103/PhysRevC.76.051602
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
2007SA50 Nucl.Phys. A791, 36 (2007) A.R.Samana, T.Tarutina, F.Krmpotic, M.S.Hussein, T.T.S.Kuo Pairing correlations in odd-mass carbon isotopes and effect of Pauli principle in particle-core coupling in 13C and 11Be NUCLEAR STRUCTURE 11Be, 13,15,17,19C; calculated level energies, J, π, and deformation parameters using one-quasiparticle PBCS model.
doi: 10.1016/j.nuclphysa.2007.03.115
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
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
2006HU05 Phys.Rev. C 73, 044610 (2006); Erratum Phys.Rev. C 76, 019902 (2007) M.S.Hussein, P.R.S.Gomes, J.Lubian, L.C.Chamon New manifestation of the dispersion relation: Breakup threshold anomaly NUCLEAR REACTIONS 208Pb(6Li, 6Li), E=27-39 MeV; analyzed σ(θ); deduced optical potential features.
doi: 10.1103/PhysRevC.73.044610
2006HU12 Phys.Lett. B 640, 91 (2006) M.S.Hussein, R.Lichtenthaler, F.M.Nunes, I.J.Thompson Scaling and interference in the dissociation of halo nuclei NUCLEAR REACTIONS 12C, 40Ca, 120Sn, 208Pb(8B, X), E=44, 70 MeV/nucleon; 12C, 40Ca, 120Sn, 208Pb(11Be, X), E=44, 70, 200 MeV/nucleon; 12C, 40Ca, 120Sn, 208Pb(7Be, X), E=100 MeV/nucleon; calculated elastic nuclear breakup σ; deduced target mass dependence, Coulomb-nuclear interference. Continuum discretized coupled channels calculations, other targets also considered.
doi: 10.1016/j.physletb.2006.07.046
2006TA28 Braz.J.Phys. 36, 1349 (2006) T.Tarutina, A.R.Samana, F.Krmpotic, M.S.Hussein Quasiparticle-Rotor Model Description of Carbon Isotopes NUCLEAR STRUCTURE 12,13,14,15,16,17,18,19C;calculated level energies, J, π, configurations, deformation using quasiparticle-rotor coupling model withing the usual BCS and projected BCS.
doi: 10.1590/S0103-97332006000800003
2005AL18 Nucl.Phys. A753, 83 (2005) M.A.G.Alvarez, N.Alamanos, L.C.Chamon, M.S.Hussein Study of the effects of Pauli blocking and Pauli nonlocality on the optical potential NUCLEAR REACTIONS 12C(α, α), E=43 MeV; 12C(6He, 6He), E=38 MeV; 12C(6Li, 6Li), E=53 MeV; 12C, 28Si(7Li, 7Li), E=50 MeV; 12C, 16O, 90Zr, 208Pb(12C, 12C), E=25-120 MeV; 90Zr, 208Pb(16O, 16O), E=94 MeV; 208Pb(40Ar, 40Ar), E=44 MeV; analyzed σ(θ); deduced optical model parameters, Pauli effects.
doi: 10.1016/j.nuclphysa.2005.01.031
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
2005GO09 Phys.Rev. C 71, 034608 (2005) P.R.S.Gomes, M.D.Rodriguez, G.V.Marti, I.Padron, L.C.Chamon, J.O.Fernandez Niello, O.A.Capurro, A.J.Pacheco, J.E.Testoni, A.Arazi, M.Ramirez, R.M.Anjos, J.Lubian, R.Veiga, R.Liguori Neto, E.Crema, N.Added, C.Tenreiro, M.S.Hussein Effect of the breakup on the fusion and elastic scattering of weakly bound projectiles on 64Zn NUCLEAR REACTIONS 64Zn(6Li, X), (7Li, X), (9Be, X), (16O, X), E ≈ 16-69 MeV; measured fusion and reaction σ; deduced reaction mechanism features. 64Zn(9Be, 9Be), E=17-28 MeV; 64Zn(16O, 16O), E=40-64 MeV; measured elastic σ(θ). Coupled channels analysis.
doi: 10.1103/PhysRevC.71.034608
2005GO35 J.Phys.(London) G31, S1669 (2005) P.R.S.Gomes, I.Padron, J.O.Fernandez Niello, G.V.Marti, M.D.Rodriguez, O.A.Capurro, A.J.Pacheco, J.E.Testoni, A.Arazi, J.Lubian, R.M.Anjos, L.C.Chamon, E.Crema, M.S.Hussein Fusion, break-up and elastic scattering of weakly bound nuclei NUCLEAR REACTIONS 27Al, 64Zn(9Be, X), E(cm) ≈ 14-25 MeV; 64Zn(6Li, X), E(cm) ≈ 15-40 MeV; measured reaction, break-up, and fusion σ; deduced optical potential features.
doi: 10.1088/0954-3899/31/10/051
2005LI56 Eur.Phys.J. A 25, Supplement 1, 733 (2005) R.Lichtenthaler, A.Lepine-Szily, V.Guimaraes, C.Perego, V.Placco, O.Camargo, Jr., R.Denke, P.N.de Faria, E.A.Benjamin, N.Added, G.F.Lima, M.S.Hussein, J.Kolata, A.Arazi Radioactive Ion beams in Brazil (RIBRAS)
doi: 10.1140/epjad/i2005-06-043-y
2005WI04 Phys.Rev. C 71, 034319 (2005) A.N.Wilson, A.J.Sargeant, P.M.Davidson, M.S.Hussein How large is the spreading width of a superdeformed band? NUCLEAR STRUCTURE 192,194Hg, 192,194Pb, 152Dy; calculated superdeformed levels spreading widths, decay-out features. Two models compared.
doi: 10.1103/PhysRevC.71.034319
2004BA18 Braz.J.Phys. 34, 773 (2004) E.Baldini-Neto, B.V.Carlson, R.A.Rego, M.S.Hussein p+6, 8He Elastic Scattering at Intermediate Energies NUCLEAR REACTIONS 6,8He(p, p), E ≈ 0.7 GeV; calculated σ(θ), analyzing power. Relativistic optical potential. NUCLEAR STRUCTURE 4,6,8He; calculated radii.
doi: 10.1590/s0103-97332004000500017
2004BB18 Braz.J.Phys. 34, 773 (2004) E.Baldini-Neto, B.V.Carlson, R.A.Rego, M.S.Hussein p+6, 8He Elastic Scattering at Intermediate Energies NUCLEAR REACTIONS 6,8He(p, p), E ≈ 0.7 GeV; calculated σ(θ), analyzing power. Relativistic optical potential. NUCLEAR STRUCTURE 4,6,8He; calculated radii.
doi: 10.1590/S0103-97332004000500017
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
2004GO47 Phys.Lett. B 601, 20 (2004) P.R.S.Gomes, I.Padron, M.D.Rodriguez, G.V.Marti, R.M.Anjos, J.Lubian, R.Veiga, R.Liguori Neto, E.Crema, N.Added, L.C.Chamon, J.O.Fernandez Niello, O.A.Capurro, A.J.Pacheco, J.E.Testoni, D.Abriola, A.Arazi, M.Ramirez, M.S.Hussein Fusion, reaction and break-up cross sections of weakly bound projectiles on 64Zn NUCLEAR REACTIONS 64Zn(16O, X), E(cm) ≈ 32-55 MeV; 64Zn(9Be, X), E(cm) ≈ 14-25 MeV; 64Zn(6Li, X), (7Li, X), E(cm) ≈ 14-40 MeV; 64Zn(6He, X), E(cm) ≈ 7-13 MeV; measured fusion, reaction, and breakup σ. Comparison with previous results.
doi: 10.1016/j.physletb.2004.09.029
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
2004HU06 Nucl.Phys. A734, 445 (2004) M.S.Hussein, A.J.Sargeant, M.P.Pato, M.Ueda Variance of the decay intensity of superdeformed bands
doi: 10.1016/j.nuclphysa.2004.01.082
2004HU10 Nucl.Phys. A734, E61 (2004) M.S.Hussein, M.Ueda, A.J.Sargeant, M.P.Pato Resonances and the thermonuclear reaction rate NUCLEAR REACTIONS 12C(n, γ), E=low; calculated astrophysical reaction rate, resonance effects.
doi: 10.1016/j.nuclphysa.2004.03.020
2004HU12 Nucl.Phys. A738, 367 (2004) M.S.Hussein, B.V.Carlson, T.Frederico, T.Tarutina Three-body model for the complete fusion of a two-cluster composite projectile with a heavy target
doi: 10.1016/j.nuclphysa.2004.04.063
2004HU14 Prog.Theor.Phys.(Kyoto), Suppl. 154, 146 (2004) M.S.Hussein, A.J.Sargeant, M.P.Pato, N.Takigawa, M.Ueda Energy Averages over Regular and Chaotic States in the Decay Out of Superdeformed Bands
doi: 10.1143/PTPS.154.146
2004LI78 Braz.J.Phys. 34, 753 (2004) V.P.Likhachev, J.D.T.Arruda-Neto, M.T.F.da Cruz, H.Dias, S.B.Duarte, W.R.Carvalho, Jr., M.S.Hussein, A.C.S.Lima, L.F.R.Macedo, J.Mesa, S.A.Pashchuk, T.E.Rodrigues, G.Silva, H.R.Schelin, O.A.P.Tavares Residual Nucleus Excitation Energy in (e, e'p)- Reaction
doi: 10.1590/S0103-97332004000500012
2004SA30 Phys.Rev. C 69, 067301 (2004) A.J.Sargeant, M.S.Hussein, M.P.Pato, N.Takigawa, M.Ueda Addendum: Attenuation of the intensity within a superdeformed band
doi: 10.1103/PhysRevC.69.067301
2004TA31 Phys.Rev. C 70, 034603 (2004) Interference effects in the Coulomb dissociation of 15, 17, 19C NUCLEAR REACTIONS 208Pb(19C, X), E=67 MeV/nucleon; 208Pb(17C, X), E=495 MeV/nucleon; 208Pb(15C, X), E=605 MeV/nucleon; calculated Coulomb dissociation σ(E), interference effects. Comparison with data. NUCLEAR STRUCTURE 15,17,19C; calculated dipole strength functions. Particle-rotor model.
doi: 10.1103/PhysRevC.70.034603
2004UE05 Phys.Rev. C 70, 025802 (2004) M.Ueda, A.J.Sargeant, M.P.Pato, M.S.Hussein Resonances and thermonuclear reaction rates for charged particle collisions NUCLEAR REACTIONS 12C(p, γ), E=low; calculated astrophysical reaction rate, resonance contribution. Analytic expression.
doi: 10.1103/PhysRevC.70.025802
2003AL17 Nucl.Phys. A723, 93 (2003) M.A.G.Alvarez, L.C.Chamon, M.S.Hussein, D.Pereira, L.R.Gasques, E.S.Rossi, Jr., C.P.Silva A parameter-free optical potential for the heavy-ion elastic scattering process NUCLEAR REACTIONS 12C, 16O, 40Ca, 90Zr, 208Pb(12C, 12C), 208Pb(16O, 16O), (40Ar, 40Ar), E ≈ 16-2400 MeV; analyzed σ(θ); deduced optical potential features.
doi: 10.1016/S0375-9474(03)01158-8
2003BA65 Nucl.Phys. A724, 345 (2003) E.Baldini-Neto, B.V.Carlson, R.A.Rego, M.S.Hussein p + 4, 6, 8He elastic scattering at intermediate energies NUCLEAR REACTIONS 4He(p, p), E=0.561, 0.8, 1.029 GeV; 6He(p, p), E=0.717 GeV; 8He(p, p), E=0.671 GeV; calculated σ(θ), analyzing power. Relativistic optical model, comparison with data and other models.
doi: 10.1016/S0375-9474(03)01540-9
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
2003CH85 Braz.J.Phys. 33, 238 (2003) L.C.Chamon, B.V.Carlson, L.R.Gasques, D.Pereira, C.De Conti, M.A.G.Alvarez, M.S.Hussein, M.A.Candido Ribeiro, E.S.Rossi, Jr., C.P.Silva Nonlocal Description of the Nuclear Interaction
doi: 10.1590/s0103-97332003000200012
2003HA35 Phys.Rev. C 68, 048801 (2003) K.Hagino, M.S.Hussein, A.B.Balantekin Role of virtual break-up of projectile in astrophysical fusion reactions NUCLEAR REACTIONS 3He(d, p), 7Li(p, α), E(cm)=0-100 keV; calculated virtual Coulomb breakup contribution.
doi: 10.1103/PhysRevC.68.048801
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
2003LI01 Nucl.Phys. A713, 24 (2003) V.P.Likhachev, J.Mesa, J.D.T.Arruda-Neto, B.V.Carlson, W.R.Carvalho, Jr., L.C.Chamon, A.Deppman, H.Dias, M.S.Hussein Quasi-free 238U(e, e'f) cross section in macroscopic-microscopic approach NUCLEAR REACTIONS 238U(e, e'X), E=720 MeV; calculated quasifree electrofission σ(E, θ). Comparison with data. NUCLEAR STRUCTURE 238U; calculated single-particle level energies. 237,238U, 237Pa; calculated fissility vs excitation energy.
doi: 10.1016/S0375-9474(02)01302-7
2003LI25 Phys.Rev. C 68, 014615 (2003) V.P.Likhachev, J.D.T.Arruda-Neto, W.R.Carvalho, Jr., A.Deppman, I.G.Evseev, F.Garcia, M.S.Hussein, L.F.R.Macedo, A.Margaryan, J.Mesa, V.O.Nesterenko, O.Rodriguez, S.A.Pashchuk, H.R.Schelin, M.S.Vaudeluci Inclusive quasifree electrofission cross section for 238U NUCLEAR STRUCTURE 237,238U, 237Pa; calculated fissility vs excitation energy. NUCLEAR REACTIONS 238U(e, e'p), (e, e'), E=300 MeV; calculated σ(E, θ). 238U(e, F), E=100-250 MeV; measured fission σ; deduced reaction mechanism features.
doi: 10.1103/PhysRevC.68.014615
2003LI61 Braz.J.Phys. 33, 294 (2003) R.Lichtenthaler, A.Lepine-Szily, V.Guimaraes, G.F.Lima, M.S.Hussein Radioactive Ion beams in Brasil (RIBRAS)
doi: 10.1590/s0103-97332003000200025
2003TA06 Phys.Rev. C 67, 044605 (2003) T.Tarutina, L.C.Chamon, M.S.Hussein Coulomb excitation of 11Be reexamined NUCLEAR REACTIONS 208Pb(11Be, 11Be'), E=45, 59.7, 64 MeV/nucleon; 197Au(11Be, 11Be'), E=59.7 MeV/nucleon; analyzed Coulomb excitation σ, survival probability. 11Be deduced transition B(E1).
doi: 10.1103/PhysRevC.67.044605
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
2002CH39 Phys.Rev. C66, 014610 (2002) L.C.Chamon, B.V.Carlson, L.R.Gasques, D.Pereira, C.De Conti, M.A.G.Alvarez, M.S.Hussein, M.A.Candido Ribeiro, E.S.Rossi, Jr., C.P.Silva Toward a Global Description of the Nucleus-Nucleus Interaction NUCLEAR STRUCTURE Z=1-82; analyzed charge distribution data, radii. 16O, 56Fe, 120Sn, 208Pb; calculated nucleon density distributions. NUCLEAR REACTIONS 58Ni(16O, X), E not given; 58Ni(α, X), E=139 MeV; calculated folding potential; deduced parameters. Other reaction data analyzed.
doi: 10.1103/PhysRevC.66.014610
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
2002LI23 Phys.Rev. C65, 044611 (2002) V.P.Likhachev, J.Mesa, J.D.T.Arruda-Neto, B.V.Carlson, A.Deppman, M.S.Hussein, V.O.Nesterenko, F.Garcia, O.Rodriguez Quasifree Electrofission of 238U NUCLEAR REACTIONS 238U(e, e'p), E=2 GeV; calculated σ(E, θ), residual nucleus fissility.
doi: 10.1103/PhysRevC.65.044611
2002RO31 Phys.Rev. C66, 024611 (2002) M.O.Roos, H.Dias, O.Rodriguez, N.Teruya, M.S.Hussein Preequilibrium escape widths of giant resonances NUCLEAR STRUCTURE 40Ca, 90Zr, 208Pb; calculated giant resonance preequilibrium escape widths. Statistical multistep compound theory.
doi: 10.1103/PhysRevC.66.024611
2002SA04 Phys.Rev. C65, 024302 (2002); Comment Phys.Rev. C 68, 069801 (2003) A.J.Sargeant, M.S.Hussein, M.P.Pato, N.Takigawa, M.Ueda Attenuation of the Intensity within a Superdeformed Band
doi: 10.1103/PhysRevC.65.024302
2002SA52 Phys.Rev. C 66, 064301 (2002) A.J.Sargeant, M.S.Hussein, M.P.Pato, M.Ueda Energy averages and fluctuations in the decay out of superdeformed bands
doi: 10.1103/PhysRevC.66.064301
2002UE04 Prog.Theor.Phys.(Kyoto), Suppl. 146, 634 (2002) M.Ueda, A.J.Sargeant, M.P.Pato, M.S.Hussein Evaluation of Effective Astrophysical S Factor for Non-Resonant Reactions
doi: 10.1143/PTPS.146.634
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
2001HU06 Nucl.Phys. A686, 163 (2001) M.S.Hussein, A.F.R.de Toledo Piza, O.K.Vorov, A.K.Kerman Estimate of the Anapole Moment of an Exotic Nucleus NUCLEAR STRUCTURE 11Be; analyzed data; deduced anapole moment, halo anomaly.
doi: 10.1016/S0375-9474(00)00519-4
2000DE24 Phys.Rev. C61, 051301 (2000) A.Delfino, T.Frederico, M.S.Hussein, L.Tomio Virtual States of Light Non-Borromean Halo Nuclei NUCLEAR STRUCTURE 12Be, 18,20C; calculated p-wave virtual states energies; deduced scaling properties. Core-plus-two-neutron approach.
doi: 10.1103/PhysRevC.61.051301
2000HU07 Phys.Rev.Lett. 84, 3783 (2000) Matrix Elements of Random Operators and Discrete Symmetry Breaking in Nuclei
doi: 10.1103/PhysRevLett.84.3783
2000HU19 Ann.Phys.(New York) 284, 167 (2000) M.S.Hussein, A.F.R.de Toledo Piza, O.K.Vorov SU(2, 1) Model of Multiple Giant Dipole Resonance Coulomb Excitation NUCLEAR STRUCTURE 208Pb, 197Au, 136Xe; calculated enhancement factor for Coulomb excitation of double GDR. SU(2, 1) algebra, various projectiles, comparison with data.
doi: 10.1006/aphy.2000.6066
2000SA01 Phys.Rev. C61, 011302 (2000) A.J.Sargeant, M.S.Hussein, M.P.Pato, M.Ueda Saturation of the Width of the Strength Function
doi: 10.1103/PhysRevC.61.011302
2000UE01 Phys.Rev. C61, 045801 (2000) M.Ueda, A.J.Sargeant, M.P.Pato, M.S.Hussein Effective Astrophysical S Factor for Nonresonant Reactions NUCLEAR REACTIONS 7Be(p, γ), E not given; calculated effective astrophysical S factors. Asymptotic expansion.
doi: 10.1103/PhysRevC.61.045801
1999CA13 Phys.Rev. C59, R2343 (1999) Time Scales of Multiple Giant Dipole Resonance Excitation and Decay NUCLEAR STRUCTURE A=20-250; calculated GDR excitation and decay time scales, related features; deduced contributions to multiple-phonon cross sections, particle emission role. Direct and non-direct paths.
doi: 10.1103/PhysRevC.59.R2343
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
1999GA50 Phys.Rev. C60, 064311 (1999); Erratum Phys.Rev. C 80, 039903 (2009) F.Garcia, O.Rodriguez, F.Guzman, H.Dias, J.D.T.Arruda-Neto, M.S.Hussein, A.K.Kerman Particle-Hole Level Densities in Deformed Nuclei NUCLEAR STRUCTURE 233Th, 239U; calculated potential energy surfaces, particle-hole level densities; deduced deformation effects. Microscopic combinatorial approach.
doi: 10.1103/PhysRevC.60.064311
1999HU02 Phys.Rev. C59, R1242 (1999) M.S.Hussein, A.F.R.de Toledo Piza, O.K.Vorov Nonlinear Enhancement of the Multiphonon Coulomb Excitation in Relativistic Heavy Ion Collisions NUCLEAR REACTIONS 208Pb(208Pb, X), E=70-700 MeV/nucleon; calculated double GDR Coulomb excitation σ; deduced nonlinearity parameter. SU(1, 1) algebra.
doi: 10.1103/PhysRevC.59.R1242
1999HU16 Phys.Rev. C60, 064615 (1999) M.S.Hussein, A.F.R.de Toledo Piza, O.K.Vorov, A.K.Kerman Enhancement of Parity Violating Mixing in Halo Nuclei and the Problem of Neutron Weak Parity Nonconserving Potential Constant NUCLEAR STRUCTURE 11Be; calculated halo density, wave-function; deduced parity-nonconserving effects.
doi: 10.1103/PhysRevC.60.064615
1999LE14 Phys.Rev.Lett. 82, 3972 (1999) A.Lepine-Szily, M.S.Hussein, R.Lichtenthaler, J.Cseh, G.Levai Elastic Transfer: A nondispersive component in the optical potential, and its effect on the 12C + 24Mg elastic scattering NUCLEAR REACTIONS 24Mg(12C, 12C), E(cm)=12, 13, 14 MeV; 28Si(12C, 12C), E(cm)=13.3, 14.7, 16.1 MeV; analyzed σ(θ); deduced dispersive component to optical potential. 24Mg ground state deduced carbon clustering role.
doi: 10.1103/PhysRevLett.82.3972
1999LE38 Acta Phys.Pol. B30, 1451 (1999) A.Lepine-Szily, M.S.Hussein, R.Lichtenthaler, J.Cseh, G.Levai Elastic Transfer: A non-dispersive component in the optical potential and its effect in the 12C + 24Mg elastic scattering NUCLEAR REACTIONS 24Mg(12C, 12C), E=16-40 MeV; 28Si(12C, 12C), E(cm)=13-16 MeV; analyzed σ(θ); deduced relations between the real and imaginary optical model terms. 24Mg deduced cluster features.
1999LI34 Phys.Rev. C60, 041601 (1999) R.Lichtenthaler, A.Lepine-Szily, M.S.Hussein Nuclear Transparency and the Onset of Strong Absorption Regime in the 12C +24Mg System NUCLEAR REACTIONS 24Mg(12C, 12C), E=16-40 MeV; analyzed σ(θ); deduced strong absorption regime, coupling to elastic transfer channel, other reaction mechnanism features.
doi: 10.1103/PhysRevC.60.041601
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