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NSR database version of April 29, 2024.

Search: Author = M.Pi

Found 15 matches.

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1996VE03      Int.J.Mod.Phys. E5, 353 (1996)

J.Ventura, A.Polls, X.Vinas, M.Pi

Cold Neutron and Nuclear Matter with Effective and Realistic Interactions

doi: 10.1142/S0218301396000177
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1991PI04      Nucl.Phys. A524, 537 (1991)

M.Pi, E.Suraud, P.Schuck

Quasi-Fusion of ¹³⁹La + ¹²C at Intermediate Energies ( Question ) A study within the Landau-Vlasov approach

NUCLEAR REACTIONS ¹²C(¹³⁹La, X), E=50-170 MeV/nucleon; analyzed data; deduced fusion threshold beam energy dependence.

doi: 10.1016/0375-9474(91)90284-D
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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
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1989SU05      Nucl.Phys. A492, 294 (1989)

E.Suraud, M.Pi, P.Schuck

Giant Dipole Modes in Heavy-Ion Reactions

NUCLEAR REACTIONS ¹²C(¹²Be, ¹²Be'), ⁴⁰Ca(¹⁶O, ¹⁶O'), E=5 MeV/nucleon; calculated dipole mode time evolution.

doi: 10.1016/0375-9474(89)90088-2
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1989SU10      Nucl.Phys. A495, 73c (1989)

E.Suraud, D.Cussol, Ch.Gregoire, D.Boilley, M.Pi, P.Schuck, B.Remaud, F.Sebille

Explosions in Landau Vlasov Dynamics

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, X), E=20-100 MeV/nucleon; ⁵⁰Ti(⁴⁰Ar, X), E=20, 44 MeV/nucleon; ¹⁹⁷Au(⁴⁰Ar, X), E=60 MeV/nucleon; calculated average density time evolution. Landau-Vlasov simulations.

doi: 10.1016/0375-9474(89)90309-6
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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
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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
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1988SU05      Nucl.Phys. A482, 187c (1988)

E.Suraud, M.Pi, P.Schuck

Excitation of Giant Dipole Modes in Heavy-Ion Reactions

NUCLEAR REACTIONS ¹²C(¹²Be, X), E=5 MeV/nucleon; calculated GDR excitation strength function. Nonlinearized Vlasov equation.

doi: 10.1016/0375-9474(88)90584-2
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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
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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
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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
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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
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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
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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
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1982PI05      Phys.Rev. C26, 733 (1982)

M.Pi, X.Vinas, M.Barranco

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
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