Nuclear Science References (NSR)

NUCLEAR REACTIONS ⁹⁰Zr(α, α), E=40-200 MeV; calculated σ(θ), forward scattering features; deduced rainbow scattering shadow effect. Semiclassical interpretation. Sum-of-differences approach.

doi: 10.1016/S0375-9474(99)00021-4
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1998UE02 Phys.Rev.Lett. 81, 1809 (1998)

M.Ueda, M.P.Pato, M.S.Hussein

Forward Glory Phenomenon in the Dark-Side of Heavy-Ion Nuclear Rainbow Scattering

NUCLEAR REACTIONS ⁹⁰Zr(α, α), E=40 MeV; calculated scattering amplitude vs θ; deduced rainbow scattering components, absorption role. Comparison of quantum, semiclassical approaches.

doi: 10.1103/PhysRevLett.81.1809
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1995HU02 Phys.Rev. C51, 846 (1995)

M.S.Hussein, M.P.Pato, A.F.R.de Toledo Piza

Influence of Resonant Channels on Subbarrier Heavy-Ion Fusion

NUCLEAR REACTIONS ²⁰⁸Pb(¹¹Li, X), E(cm)=10-40 MeV; calculated fusion σ(E); deduced resonant channels role. Schematic model.

doi: 10.1103/PhysRevC.51.846
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1995HU08 Phys.Rev. C51, 2681 (1995)

M.S.Hussein, M.P.Pato

Analytical Treatment of Heavy-Ion Elastic Scattering at Intermediate Energies

NUCLEAR REACTIONS ¹²C(¹¹C, ¹¹C), (¹¹Li, ¹¹Li), E not given; calculated σ(θ). Eikonal approximation, complex Woods-Saxon interaction based phase shift, deflection functions.

doi: 10.1103/PhysRevC.51.2681
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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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1994PA10 Phys.Rev. C49, 2919 (1994)

M.P.Pato, C.A.Nunes, C.L.Lima, M.S.Hussein, Y.Alhassid

Deformed Gaussian Orthogonal Ensemble Analysis of the Interacting Boson Model

doi: 10.1103/PhysRevC.49.2919
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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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1993HU03 Phys.Rev. C47, 2401 (1993)

M.S.Hussein, M.P.Pato

Deformed Gaussian Orthogonal Ensemble Description of Isospin Mixing and Spectral Fluctuation Properties

NUCLEAR STRUCTURE ²⁶Al; analyzed T=0, 1 levels spacing distributions Gaussian orthogonal ensemble.

doi: 10.1103/PhysRevC.47.2401
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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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1991HU03 Phys.Rev. C44, 2219 (1991)

M.S.Hussein, M.P.Pato, C.A.Bertulani

Low Energy Behavior of ¹¹Li Dissocation Cross Section

NUCLEAR REACTIONS ¹⁹⁷Au(¹¹Li, X), E=0.005-1 GeV/nucleon; calculated Coulomb dissociation σ. Different model dependent dipole resonance strengths.

doi: 10.1103/PhysRevC.44.2219
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1990HU06 Phys.Rev.Lett. 65, 839 (1990)

M.S.Hussein, C.L.Lima, M.P.Pato, C.A.Bertulani

Color van der Waals Force Acting in Heavy-Ion Scattering at Low Energies

NUCLEAR REACTIONS ²⁰⁸Pb(²⁰⁸Pb, ²⁰⁸Pb), E(cm)=500 MeV; calculated σ(θ); deduced color van der Waals force role.

doi: 10.1103/PhysRevLett.65.839
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1988PA03 Z.Phys. A329, 189 (1988)

M.P.Pato, E.C.Oliveira, L.C.Gomes

A Comparison of the Gaussian Approximation and Langevin's Simulation in DIC

NUCLEAR REACTIONS ²³²Th(⁴⁰Ar, X), E=279 MeV; calculated Gaussian approximation first, second moments; deduced sources of discrepancy. Fokker-Planck equation.

1988PA07 Phys.Lett. 207B, 121 (1988)

M.P.Pato, M.S.Hussein

Refraction-Diffraction Interference in Heavy-Ion Elastic Angular Distributions

NUCLEAR REACTIONS ¹²C(¹³C, ¹³C), E=260 MeV; calculated σ(θ) related quantities. Refraction-diffraction interference.

doi: 10.1016/0370-2693(88)91401-3
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1982HU04 Phys.Rev. C25, 1896 (1982)

M.S.Hussein, M.P.Pato

Back-Angle Scattering of ¹²C on ²⁸Si

NUCLEAR REACTIONS ²⁸Si(¹²C, ¹²C), E(cm) ≈ 16-35 MeV; calculated σ(θ) vs E; deduced structure, reaction mechanism, α-transfer. Complex l-window model.

doi: 10.1103/PhysRevC.25.1896
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