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NSR database version of May 20, 2024.

Search: Author = M.S.Hussein

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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
Citations: PlumX Metrics


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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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0905.


2017BA17      Eur.Phys.J. A 53, 126 (2017)

J.F.Babb, R.Higa, M.S.Hussein

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
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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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2017HU06      Eur.Phys.J. A 53, 110 (2017)

M.S.Hussein

Two-step nuclear reactions: The Surrogate Method, the Trojan Horse Method and their common foundations

doi: 10.1140/epja/i2017-12321-7
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2017HU16      Acta Phys.Pol. B48, 1837 (2017)

M.S.Hussein, J.F.Babb, R.Higa

The Casimir-Polder Interaction Between Two Neutrons and Possible Relevance to Tetraneutron States

doi: 10.5506/APhysPolB.48.1837
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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
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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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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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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, 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
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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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2013DE26      Phys.Rev.Lett. 111, 082701 (2013)

P.Descouvemont, M.S.Hussein

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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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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2009AN15      Phys.Rev. C 80, 034610 (2009)

D.M.Andrade, M.S.Hussein

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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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2008HU06      Phys.Rev. C 77, 054609 (2008)

M.S.Hussein, R.Lichtenthaler

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0440.


2007BE58      Phys.Rev. C 76, 051602 (2007)

C.A.Bertulani, M.S.Hussein

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
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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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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
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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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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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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
Citations: PlumX Metrics


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
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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
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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
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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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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0348.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0348.


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
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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
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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
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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
Citations: PlumX Metrics


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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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0348.


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
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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
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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
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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
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2004TA31      Phys.Rev. C 70, 034603 (2004)

T.Tarutina, M.S.Hussein

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
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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
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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
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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
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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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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
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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
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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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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
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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
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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
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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
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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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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
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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.


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
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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
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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
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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
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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
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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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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
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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
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2000HU07      Phys.Rev.Lett. 84, 3783 (2000)

M.S.Hussein, M.P.Pato

Matrix Elements of Random Operators and Discrete Symmetry Breaking in Nuclei

doi: 10.1103/PhysRevLett.84.3783
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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
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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
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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
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1999CA13      Phys.Rev. C59, R2343 (1999)

B.V.Carlson, M.S.Hussein

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
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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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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
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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
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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
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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
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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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