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NSR database version of May 3, 2024.

Search: Author = G.Madurga

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1987ES06      J.Phys.(London) G13, 1261 (1987)

J.I.Escudero, F.Barranco, G.Madurga

Consistent Description of the Experimental Root Mean Square Charge Radii

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ⁹⁰Zr, ²⁰⁸Pb; calculated rms charge radii; deduced long-range residual interaction role.

doi: 10.1088/0305-4616/13/10/014
Citations: PlumX Metrics

1985AN16      Nucl.Phys. A443, 380 (1985)

M.V.Andres, J.M.Quesada, M.Lozano, G.Madurga

A Level-Density-Dependent Imaginary Potential for Heavy Ions

NUCLEAR REACTIONS ²⁸Si, ⁴⁰Ca(⁹Be, ⁹Be), E=14-26 MeV; ²⁴Mg(¹²C, ¹²C), E=21, 24 MeV; ²⁴Mg(¹⁶O, ¹⁶O), E=28-33 MeV; ⁴⁰Ca(²⁰Ne, ²⁰Ne), E=44.1-70.4 MeV; ⁴⁰Ca(³²S, ³²S), E=100-151.5 MeV; calculated real folding potential renormalization constants, σ(θ). Level density dependent heavy ion potential component.

NUCLEAR STRUCTURE ⁹Be, ¹²C, ¹⁶O, ²⁰Ne, ²⁴Mg, ²⁸Si, ³²S, ⁴⁰Ca; calculated neutron, proton, charge density distributions. Woods-Saxon potential.

doi: 10.1016/0375-9474(85)90269-6
Citations: PlumX Metrics

1984LO06      J.Phys.(London) G10, 1071 (1984)

M.Lozano, A.Mandly, G.Madurga

Fusion Barriers for Heavy Systems with 1000 < Z₁Z₂ < 3000

NUCLEAR REACTIONS ⁶⁵Cu(⁸⁶Kr, X), E(cm)=157.4-308.2 MeV; ¹⁶⁵Ho(⁴⁰Ar, X), E(cm)=181, 240.9 MeV; ⁵⁶Fe(¹³⁶Xe, X), E(cm)=225 MeV; ¹³⁹La(⁸⁶Kr, X), E(cm)=312, 376.8, 438.6 MeV; ¹⁶⁵Ho(⁸⁴Kr, X), E=298.2, 326 MeV; ²⁰⁹Bi(⁸⁴Kr, X), E(cm)=356.7, 374.5; calculated fusion σ. ¹⁴¹Pr(³⁵Cl, X), E(cm)=120-135 MeV; ^144,148,154Sm(⁴⁰Ar, X), E(cm)=125-145 MeV; calculated fusion σ(E), barriers. Shell model nuclear density, effective interaction generated folding optical potential.

NUCLEAR STRUCTURE ³⁵Cl, ⁴⁰Ar, ⁵⁶Fe, ⁶⁵Cu, ^84,86Kr, ⁹⁰Zr, ¹⁰⁹Ag, ¹³²Xe, ¹³⁹La, ¹⁴¹Pr, ^144,148,154Sm, ¹⁶⁵Ho, ²⁰⁹Bi, ²³⁸U; calculated nuclear density distribution rms radii.

doi: 10.1088/0305-4616/10/8/012
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1983BR05      J.Phys.(London) G9, 423 (1983)

B.A.Brown, S.E.Massen, J.I.Escudero, P.E.Hodgson, G.Madurga, J.Vinas

The Charge and Matter Distributions of ²⁰⁸Pb

NUCLEAR STRUCTURE ²⁰⁸Pb; analyzed charge, matter distribution, single particle energies, valence orbital rms radii; deduced best potential.

doi: 10.1088/0305-4616/9/4/009
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1983QU01      Phys.Lett. 125B, 14 (1983)

J.M.Quesada, M.Lozano, G.Madurga

A Phenomenological Imaginary Part of the Optical Potential for Heavy Ions

NUCLEAR REACTIONS ²⁸Si(¹⁶O, ¹⁶O), E=33-81 MeV; calculated σ(θ). Optical potential, phenomenological imaginary part.

doi: 10.1016/0370-2693(83)91224-8
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1982LO13      J.Phys.(London) G8, 1259 (1982)

M.Lozano, J.I.Escudero, G.Madurga

Nuclear Structure Effects in Frictionless Formula for Heavy-Ion Fusion

NUCLEAR REACTIONS, ICPND ¹⁴N(¹²C, X), E=10-80 MeV; ^12,13C(¹²C, X), E=10-35 MeV; ¹⁰B, ¹⁴N(¹⁴N, X), E=sub-Coulomb; ¹⁴N(¹⁴N, X), ^14,15N(¹⁶O, X), E=near fusion; ^24,26Mg, ¹⁶O, ²⁷Al, ⁴⁰Ca(¹⁶O, X), ²⁷Al(¹⁷O, X), ²⁸Si, ²⁴Mg, ²⁷Al(¹⁸O, X), ²⁴Mg, ²⁷Al(²⁰Ne, X), (³²S, X), ²⁸Si(²⁸Si, X), ⁴⁰Ca, ⁵⁸Ni(³²S, X), ^58,64,62Ni, ²⁷Al, ^54,56Fe, ^{112,116,120,124}Sn, ⁹⁰Zr, ¹⁴¹Pr(³⁵Cl, X), ¹¹⁰Pd, ¹⁰⁹Ag, ¹²¹Sb, ¹⁶⁵Ho, ¹⁹⁷Au, ²³⁸U(⁴⁰Ar, X), ¹³²Xe, ¹⁶⁵Ho(⁵⁶Fe, X), (⁸⁴Kr, X), E=high; calculated fusion σ vs E. Semi-empirical formalism, final state, entrance channel effects.

NUCLEAR STRUCTURE A=9-238; calculated nuclear density distribution rms radii. Semi-empirical formalism.

doi: 10.1088/0305-4616/8/9/011
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1981VI01      Phys.Rev. C23, 780 (1981)

F.J.Vinas, M.Lozano, G.Madurga

Double Folding with a Density-Dependent Effective Interaction and its Analytical Approximation

NUCLEAR REACTIONS ^72,74,76Ge(¹⁶O, ¹⁶O), (¹⁸O, ¹⁸O), E=56 MeV; ¹⁰⁰Mo, ⁶²Ni(¹²C, ¹²C), E=48 MeV; ⁷⁴Ge(¹²C, ¹²C), E=42 MeV; ²⁰⁸Pb(¹²C, ¹²C), E=96 MeV; ²⁰⁷Pb(¹³C, ¹³C), E=86.1 MeV; ²⁸Si(¹⁶O, ¹⁶O), E=141.5, 215 MeV; ⁵⁹Co, ⁶⁰Ni(¹⁶O, ¹⁶O), E=141.7 MeV; ²⁰⁹Bi(¹¹B, ¹¹B), E=74.6; ²⁰⁸Pb(¹⁶O, ¹⁶O), E=129.5, 192 MeV; ²⁰⁹Bi(⁴⁰Ar, ⁴⁰Ar), E=286 MeV; analyzed σ(θ); deduced real optical potential parameters, renormalizing factor. Double folding model, nucleon-nucleon effective potential.

doi: 10.1103/PhysRevC.23.780
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1980LO01      Nucl.Phys. A334, 349 (1980)

M.Lozano, G.Madurga

Exponential Optical Potentials for Heavy-Ion Elastic Scattering

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁶O, ¹⁶O), E=129.5, 192 MeV; ²⁰⁸Pb(¹²C, ¹²C), E=96 MeV; ²⁰⁹Bi(¹¹B, ¹¹B), E=74.6 MeV; ⁶²Ni, ¹⁰⁰Mo(¹²C, ¹²C), E=48 MeV; ⁷⁴Ge(¹²C, ¹²C), E=42 MeV; ⁶⁰Ni, ⁵⁹Co, ²⁸Si(¹⁶O, ¹⁶O), E=141.7 MeV; ²⁰⁷Pb(¹³C, ¹³C), E=86.1 MeV; ^72,74,76Ge(¹⁶O, ¹⁶O), (¹⁸O, ¹⁸O), E=56 MeV; ⁶⁴Ni(¹⁶O, ¹⁶O), E=56 MeV; ²⁰⁹Bi, ²³⁸U(⁴⁰Ar, ⁴⁰Ar), E=340 MeV; calculated σ(θ). Exponential optical potentials.

doi: 10.1016/0375-9474(80)90074-3
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1980LO02      Phys.Lett. 90B, 50 (1980)

M.Lozano, G.Madurga

Nuclear-Structure Dependence of the Fusion Cross Section for Heavy Ions

NUCLEAR REACTIONS ¹²C(¹⁴N, X), (¹⁸O, X), (¹⁵N, X), (¹⁹F, X), E(cm)=0.01-0.05 GeV; ³²S(²⁴Mg, X), (²⁷Al, X), ²⁷Al, ⁴⁸Ti, ⁵⁶Fe, ⁶²Ni, ^116,124Sn(³⁵Cl, X), E=0.03-0.1 GeV; calculated fusion σ(E). Semiclassical model, nuclear matter density distribution.

doi: 10.1016/0370-2693(80)90048-9
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1980MA34      Phys.Lett. B95, 358 (1980)

G.Madurga, M.Lozano, A.Jadraque

The Role of Rainbow Refraction in Heavy Ion Elastic Scattering

NUCLEAR REACTIONS ⁴⁰Ca(²⁰Ne, ²⁰Ne), (¹³C, ¹³C), (⁶Li, ⁶Li), ²⁸Si(¹⁶O, ¹⁶O), E=30-200 MeV; ²⁰⁸Pb, ⁴⁰Ca(¹⁶O, ¹⁶O), E=100-300 MeV; ⁵⁹Co(¹⁶O, ¹⁶O), ⁴⁰Ca(⁴⁰Ca, ⁴⁰Ca), E=40-200 MeV; analyzed data; deduced strong absorption radius, rainbow distance vs E.

doi: 10.1016/0370-2693(80)90168-9
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1979LO05      Phys.Lett. 82B, 170 (1979)

M.Lozano, G.Madurga, P.E.Hodgson

Critical Radii for Alpha-Particle Elastic Scattering

NUCLEAR STRUCTURE ^{110,112,114,116}Cd, ^{112,114,116,118,120,122,124}Sn, ^{122,124,126,128,130}Te, ^{142,144,146,148,150}Nd, ^{144,146,148,150,152}Sm, ^204,206,208Pb; calculated nuclear density distribution using Saxon-Woods single particle functions; deduced method to obtain α-optical potentials from target nucleus structure.

doi: 10.1016/0370-2693(79)90727-5
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1972MA73      Nuovo Cim. 12A, 451 (1972)

G.Madurga

Asymmetry of Direct Neutron Emission in Polarized-Muon Capture

doi: 10.1007/BF02729557
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