NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.Barranco Found 38 matches. 1996BA41 Z.Phys. A355, 23 (1996) M.Barranco, E.S.Hernandez, J.Navarro Two Quasiparticle Scattering and Pairing in Neutron Matter with Skyrme Interactions
doi: 10.1007/s002180050073
1993CE01 Phys.Rev. C47, 1091 (1993) M.Centelles, X.Vinas, M.Barranco, N.Ohtsuka, A.Faessler, D.T.Khoa, H.Muther Relativistic Extended Thomas-Fermi Calculations of Finite Nuclei with Realistic Nucleon-Nucleon Interactions NUCLEAR STRUCTURE 12C, 16O, 40,48Ca, 56Ni, 90Zr, 114,118Sn, 140Ce, 208Pb; calculated binding energy, charge radius. 52Fe, 118Sn, 152Dy, 186Os, 207Bi, 240Pu; calculated fission barrier, saddle point quadrupole moment, critical angular momentum, equidensity lines. Relativistic extended Thomas-Fermi calculations, realistic interactions. NUCLEAR REACTIONS 12C(12C, 12C), E=2.4 GeV; 28Si, 12C(16O, 16O), E=1.503 GeV; calculated σ(θ). Relativistic extended Thomas-Fermi calculations, realistic interactions.
doi: 10.1103/PhysRevC.47.1091
1992CE01 Nucl.Phys. A537, 486 (1992) M.Centelles, X.Vinas, M.Barranco, S.Marcos, R.J.Lombard Semiclassical Approximations in Non-Linear σ(omega) Models NUCLEAR STRUCTURE 40Ca, 208Pb; calculated total energy, proton, neutron rms radii, nucleon densities. Nonlinear (sigma-omega) models, semi-classical approximations.
doi: 10.1016/0375-9474(92)90365-Q
1991BA28 Phys.Rev. C44, 178 (1991) M.Barranco, R.J.Lombard, S.Marcos, S.A.Moszkowski Multi-Lambda Matter in a Derivative Coupling Model NUCLEAR STRUCTURE 40Ca; calculated baryon density, spin orbit potential, scalar, vector fields. Mean field approximation.
doi: 10.1103/PhysRevC.44.178
1991CE09 J.Phys.(London) G17, L193 (1991) M.Centelles, X.Vinas, M.Barranco, N.Ohtsuka, A.Faessler, D.T.Khoa, H.Muther Relativistic Extended Thomas-Fermi Calculations of Finite Nuclei NUCLEAR STRUCTURE 12C, 16O, 40,48Ca, 56Ni, 90Zr, 114,118Sn, 140Ce, 208Pb; calculated binding energy, charge radii. 240Pu; calculated fission barrier angular momentum dependence vs quadrupole moment. Relativistic extended Thomas-Fermi model. NUCLEAR REACTIONS 12C(12C, 12C), E=1.016 GeV; calculated σ(θ). Microscopic optical potential. Relativistic extended Thomas-Fermi model.
doi: 10.1088/0954-3899/17/11/005
1990CE03 Nucl.Phys. A510, 397 (1990) M.Centelles, M.Pi, X.Vinas, F.Garcias, M.Barranco Self-Consistent Extended Thomas-Fermi Calculations in Nuclei NUCLEAR STRUCTURE 40Ca, 90Zr, 208Pb; calculated total energies. Extended Thomas-Fermi model, Skyrme type forces.
doi: 10.1016/0375-9474(90)90058-T
1990GA12 Z.Phys. A336, 31 (1990) F.Garcias, M.Barranco, A.Faessler, N.Ohtsuka Angular Momentum and Temperature Dependence of Fission Barriers with a Realistic Force NUCLEAR STRUCTURE 132Ce, 152Dy; calculated fission barrier thermal evolution. Bethe-Goldstone equation, realistic forces.
1990GA25 Z.Phys. A337, 261 (1990) F.Garcias, M.Barranco, J.Navarro, E.Suraud High Temperature Giant Dipole and Isoscalar Resonances NUCLEAR STRUCTURE 63Cu, 90Zr, 114Sn, 140Ce, 160Er, 208Pb; calculated GDR energy vs temperature. Semi-classical approximation, RPA sum rules.
1989GA10 Nucl.Phys. A495, 169c (1989) F.Garcias, M.Barranco, J.Nemeth, C.Ngo, X.Vinas The Fission of Hot Rotating Nuclei: A selfconsistent Thomas-Fermi calculation NUCLEAR STRUCTURE 109Cd, 118Sn, 164Ho, 186Os, 207Bi, 240Pu; calculated fission barrier thermal evolution. Axially deformed Thomas-Fermi model.
doi: 10.1016/0375-9474(89)90316-3
1989GA13 Phys.Rev. C40, 1522 (1989) F.Garcias, M.Barranco, H.S.Wio, C.Ngo, J.Nemeth Fission Stability Diagram of 240Pu NUCLEAR STRUCTURE 240Pu; calculated fission barrier vs quadrupole moment. Axially symmetric deformed Thomas-Fermi model.
doi: 10.1103/PhysRevC.40.1522
1989GR25 Yad.Fiz. 50, 990 (1989) K.A.Gridnev, P.B.Danilov, V.B.Subbotin, M.Barranko, K.Binyas Building of Ion-Ion Potential by the Energy-Density-Functional Method NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 238U; calculated nucleon density profiles. Euler-Lagrange equations, exact solution.
1989NA22 Nucl.Phys. A505, 173 (1989) The Dipole Isovector M3 Sum Rule in the Random Phase Approximation NUCLEAR STRUCTURE 16O, 40Ca, 60Ni, 90Zr, 114Sn, 140Ce, 208Pb; calculated M3 dipole isovector sum rule contributions. RPA, Skyrme interactions.
doi: 10.1016/0375-9474(89)90369-2
1989VI03 Nucl.Phys. A495, 201c (1989) X.Vinas, M.Pi, F.Garcias, Ll.Serra, M.Barranco (h-bar)4-Order Thomas-Fermi Variational Calculations of Finite Nuclei NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 208Pb; calculated giant resonance energies. Semi-classical density matrix expansion method.
doi: 10.1016/0375-9474(89)90319-9
1988GA07 Phys.Lett. 206B, 177 (1988) F.Garcias, M.Barranco, J.Nemeth, C.Ngo Thomas-Fermi Calculations of the Level Density Parameter of Deformed Nuclei NUCLEAR STRUCTURE 164Ho, 63Cu; calculated fission barrier vs quadrupole moment. 63Cu, 164Ho, 205At, 240Pu; calculated level density parameter vs quadrupole moment. Constrained Thomas-Fermi model.
doi: 10.1016/0370-2693(88)91487-6
1988MI12 Z.Phys. A330, 5 (1988) A.Milian, M.Barranco, D.Mas, R.J.Lombard Nuclear Collective States at Finite Temperature NUCLEAR STRUCTURE A=80-205; calculated isoscalar monopole, octupole giant resonance energy vs particle number. 90Zr, 40Ca, 208Pb; calculated levels, reduced transition probabilities. Energy density method.
1988PI11 Phys.Lett. 215B, 5 (1988) M.Pi, X.Vinas, F.Garcias, M.Barranco (h-bar)4-Order Variational Thomas-Fermi Calculations of Finite Nuclei: The local case NUCLEAR STRUCTURE A=72-292; calculated total energies, chemical potentials. A=204; calculated Woods-Saxon densities. A=224; calculated harmonic oscillator densities.
doi: 10.1016/0370-2693(88)91058-1
1988SU03 Nucl.Phys. A480, 29 (1988) E.Suraud, M.Barranco, J.Treiner A Semi-Classical Model for Isoscalar Giant Resonances at Finite Temperatures NUCLEAR STRUCTURE 56Fe, 208Pb; calculated neutron, proton rms radii. 90Zr, 40Ca, 120Sn, 208Pb; calculated isoscalar giant resonances. Semi-classical model, finite temperatures.
doi: 10.1016/0375-9474(88)90382-X
1987BA08 Nucl.Phys. A464, 29 (1987) M.Barranco, M.Pi, J.Nemeth, C.Ngo, E.Tomasi Spurious Continuum Effects on Excited Giant Resonances NUCLEAR STRUCTURE 40Ca; calculated giant monopole isoscalar strength function. 208Pb; calculated sum rules, average energies; deduced spurious continuum effects role. Time-dependent Thomas-Fermi model.
doi: 10.1016/0375-9474(87)90420-9
1987NG04 J.Phys.(Paris), Colloq.C-2, 157 (1987) C.Ngo, R.Boisgard, J.Desbois, J.Nemeth, M.Barranco Multifragmentation of Nuclei NUCLEAR STRUCTURE 208Pb; calculated multi-fragmentation instability, per nucleon excitation energy/binding energy, density vs radius. Irrotational hydrodynamical model.
1987SU19 J.Phys.(Paris), Colloq.C-2, 11 (1987) E.Suraud, M.Barranco, J.Treiner A Semi-Classical Description of Giant Resonances at Finite Temperature NUCLEAR STRUCTURE 90Zr, 120Sn, 208Pb; calculated giant resonance energies vs temperature. Semi-classical model.
1986AN18 Nucl.Phys. A455, 561 (1986) M.V.Andres, M.Lozano, M.Barranco, M.Pi, X.Vinas, K.A.Gridnev Nuclear Transfer Contribution to the Imaginary Nucleus-Nucleus Potential NUCLEAR REACTIONS 40Ca(16O, 16O), E=40-139.6 MeV; 40Ca(40Ca, 40Ca), E=129.6-240 MeV; 208Pb(16O, 16O), E=192-1295 MeV; calculated σ(θ). Nucleon transfer role in nucleus-nucleus potential imaginary term.
doi: 10.1016/0375-9474(86)90322-2
1986NE02 Z.Phys. A323, 419 (1986) J.Nemeth, M.Barranco, C.Ngo, E.Tomasi Model for the Evolution of Hot and Compressed Spherical Nuclei NUCLEAR STRUCTURE 40Ca; calculated rms radius time evolution. 208Pb, 16O calculated density profile vs radius evolution. Hydrodynamical approach.
1986NE04 Z.Phys. A325, 347 (1986) J.Nemeth, M.Barranco, J.Desbois, C.Ngo Multifragmentation of Hot and Compressed Nuclei within a Time Dependent Thomas Fermi and Percolation Model NUCLEAR STRUCTURE 208Pb; calculated dynamical evolution, density profile, primary, secondary mass distribution, multifragmentation, normal de-excitation regions, maximum thermal excitation energy per nucleon; deduced hot compressed nuclei multifragmentation. Time dependent Thomas-Fermi, percolation models.
1986PI02 Phys.Lett. 166B, 1 (1986) M.Pi, M.Barranco, J.Nemeth, C.Ngo, E.Tomasi Time-Dependent Thomas-Fermi Approach to Nuclear Monopole Oscillations NUCLEAR STRUCTURE 16O, 40Ca; calculated isoscalar strength function. Time-dependent Thomas-Fermi approach.
doi: 10.1016/0370-2693(86)91143-3
1985BA15 Phys.Lett. 154B, 96 (1985) M.Barranco, A.Polls, S.Marcos, J.Navarro, J.Treiner The Excited Dipole Resonance: A finite-temperature sum rule approach NUCLEAR STRUCTURE 40Ca, 78Kr, 127Cs, 144Gd, 208Pb; calculated GDR energy, width evolution vs excitation energy. Finite temperature sum rule approach.
doi: 10.1016/0370-2693(85)90565-9
1985BA55 Nucl.Phys. A444, 445 (1985) M.Barranco, A.Polls, J.Martorell RPA Sum Rules for Giant Resonances at Finite Temperature NUCLEAR STRUCTURE 40Ca, 90Zr, 120Sn, 208Pb; calculated giant multipole resonances. Finite temperature, RPA.
doi: 10.1016/0375-9474(85)90462-2
1985LE02 Z.Phys. A320, 383 (1985) S.Leray, G.La Rana, C.Ngo, M.Barranco, M.Pi, X.Vinas Emission of Prompt Nucleons in Heavy Ion Collisions NUCLEAR REACTIONS 165Ho(20Ne, xn), E=220, 402, 700 MeV; calculated prompt neutron multiplicity. Incomplete fusion, dynamical model.
doi: 10.1007/BF01415714
1985NE03 Z.Phys. A320, 691 (1985) J.Nemeth, M.Barranco, C.Ngo, E.Tomasi Spherical Time Dependent Thomas-Fermi Calculation of the Dynamical Evolution of Hot and Compressed Nuclei NUCLEAR STRUCTURE 40Ca; calculated density profile vs temperature. Self consistent time-dependent Thomas-Fermi model.
doi: 10.1007/BF01411873
1984BA45 Phys.Lett. 143B, 314 (1984) M.Barranco, S.Marcos, J.Treiner The Warm Breath NUCLEAR STRUCTURE 208Pb, 90Zr; calculated isoscalar giant monopole resonance, width. 208Pb; calculated isothermal compressibility, giant monopole resonance transition density. Hot modified Thomas-Fermi method.
doi: 10.1016/0370-2693(84)91472-2
1984BA66 Nucl.Phys. A428, 239c (1984) M.Barranco, M.Pi, X.Vinas, G.La Rana, S.Leray, C.Ngo, E.Tomasi Friction, Imaginary Potential and Nucleon Jetting Calculated from Nucleon Currents in Semi-Infinite Nuclear Matter NUCLEAR REACTIONS 40Ca(40Ca, X), E(cm)=64.8-120 MeV; calculated reaction σ. 165Ho(20Ne, X), E=402 MeV; calculated promptly emitted σ(θn), σ(En). Heavy ion collisions, nucleon jetting model.
doi: 10.1016/0375-9474(84)90254-9
1984LA04 Nucl.Phys. A414, 309 (1984) G.La Rana, C.Ngo, A.Faessler, L.Rikus, R.Sartor, M.Barranco, X.Vinas Heavy-Ion Optical Potentials at Finite Temperature Calculated using a Complex Effective Interaction Derived from a Realistic Force NUCLEAR REACTIONS 40Ca(40Ca, 40Ca), E=400, 800 MeV; 208Pb(40Ca, 40Ca), E=1 GeV; calculated optical potential parameters vs separation distance, temperature. Double folding method.
doi: 10.1016/0375-9474(84)90647-X
1984PI13 Nucl.Phys. A426, 163 (1984) M.Pi, X.Vinas, M.Barranco, G.La Rana, S.Leray, C.Ngo, E.Tomasi Nucleon Currents between Highly Excited Nuclei (II). Influence of the Relative Motion NUCLEAR REACTIONS 40Ca(16O, X), E=40-204.1 MeV; 88Sr(16O, X), E=48-59 MeV; 28Si(16O, X), E=81, 141 MeV; 208Pb(16O, X), E=129.5-312.6 MeV; 40Ca(20Ne, X), E=151 MeV; 32S(32S, X), E=90.9 MeV; 40Ca(40Ca, X), E=143.6-240 MeV; 58Ni(16O, X), E=142 MeV; 209Bi(136Xe, X), E=940, 1130 MeV; calculated optical potential imaginary part for nucleon transfer at strong absorption radius. Finite temperature Thomas-Fermi method.
doi: 10.1016/0375-9474(84)90071-X
1983CH16 Nucl.Phys. A401, 143 (1983) X.S.Chen, C.Ngo, E.Tomasi, M.Barranco, X.Vinas, H.Ngo Real Part of the Nuclear Interaction Potential between α or p and Excited Heavy Nuclei NUCLEAR REACTIONS 56Fe, 208Pb(p, p), (α, α), E not given; calculated interaction potentials. 40Ca, 51V, 56Fe, 59Co, 60,62Ni, 63Cu, 90Zr, 116Sn, 181Ta, 197Au, 208Pb, 233,238U(α, X), (p, p), E not given; calculated fusion barrier, proton potential barrier vs temperature. Double folding model.
doi: 10.1016/0375-9474(83)90341-X
1982PI05 Phys.Rev. C26, 733 (1982) Estimation of Temperature Effects on Fission Barriers NUCLEAR STRUCTURE 232Th, 238U, 242Pu, 246Cm; calculated fission barrier, deformation, deformation energy. Accurate mass formula, finite temperature, liquid drop model.
doi: 10.1103/PhysRevC.26.733
1982TO13 Nucl.Phys. A389, 69 (1982) E.Tomasi, X.S.Chen, S.Leray, C.Ngo, M.Barranco, X.Vinas, H.Ngo Calculation of Interaction Potentials between Two Heavy Ions at Finite Temperature NUCLEAR REACTIONS 40Ca(40Ca, X), 63Cu(24Mg, X), 109Ag(40Ar, X), E(cm) ≈ 66-200 MeV; calculated σ(fusion) vs E. Thomas-Fermi model, finite temperature nuclear densities.
doi: 10.1016/0375-9474(82)90291-3
1981BA03 Nucl.Phys. A351, 269 (1981) Self-Consistent Description of Nuclear Level Densities NUCLEAR STRUCTURE A=25-225; calculated level density vs mass; deduced effective mass role on level density parameter. Self-consistent, modified Thomas-Fermi method.
doi: 10.1016/0375-9474(81)90444-9
1980BA13 Phys.Lett. 91B, 321 (1980) M.Barranco, R.J.Lombard, D.Mas Coupling of Two-Quasi-Particle 2+ States to the T = 0 Giant Quadrupole Resonance in the Even Pb-Isotopes NUCLEAR STRUCTURE 190,192,194,196,198,200,202,204,206,210,212,214Pb; calculated energy of 2+ levels. Two quasiparticle plus T=0, GQR coupling.
doi: 10.1016/0370-2693(80)90986-7
1978BA49 Phys.Lett. 78B, 542 (1978) Excitation Energy of the Lowest 2+ and 3- Levels in 32Mg and 146Gd NUCLEAR STRUCTURE 32Mg, 146Gd; calculated levels.
doi: 10.1016/0370-2693(78)90635-4
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