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2014EU01      Phys.Rev. C 90, 034609 (2014)

P.Eudes, Z.Basrak, F.Sebille, V.de la Mota, G.Royer

Comprehensive analysis of fusion data well above the barrier

NUCLEAR REACTIONS ¹²C(¹⁴N, X)²⁶Al*, E=3.14, 3.80, 4.29, 6.16, 7.59, 10.39, 11.29, 11.94, 12.72, 17.71 MeV/nucleon; ¹⁶O(²⁰Ne, X)³⁶Ar*, E=3.40, 5.74, 6.10, 6.85, 7.80 MeV/nucleon; ¹²C(²⁴Mg, X)³⁶Ar*, E=25.0, 35.0, 45.0 MeV/nucleon; ²⁷Al(¹²C, X)³⁹K*, E=5.32, 6.75, 7.14, 8.04, 8.13, 15.00 MeV/nucleon; ²⁴Mg(¹⁶O, X)⁴⁰Ca*, E=3.00, 3.25, 3.50, 3.81, 4.13, 4.50, 5.06 MeV/nucleon; ²⁰Ne(²⁰Ne, X)⁴⁰Ca*, E=3.40, 5.85, 6.30, 7.00, 7.80 MeV/nucleon; ¹²C(²⁸Si, X)⁴⁰Ca*, E=3.57, 4.46, 5.36, 5.71, 6.36, 6.43, 11.04, 14.18, 16.14 MeV/nucleon; ²⁷Al(¹⁴N, X)⁴¹Ca*, E=11.21, 18.7 MeV/nucleon; ²⁶Mg(¹⁶O, X)⁴²Ca*, E=3.11, 3.36, 3.67, 3.85, 4.04, 4.49, 5.06 MeV/nucleon; ²⁴Mg(¹⁸O, X)⁴²Ca*, E=3.05, 3.33, 3.50, 3.72, 4.00 MeV/nucleon; ²⁷Al(¹⁶O, X)⁴³Sc*, E=3.13, 3.75, 4.06, 4.38, 4.69, 5.00, 5.06, 6.56, 7.88, 10.50, 13.44 MeV/nucleon; ¹²C(³²S, X)⁴⁴Ti*, E=3.21, 3.40, 4.10, 4.53, 5.00, 19.50 MeV/nucleon; ²⁶Mg(²⁰Ne, X)⁴⁶Ti*, E=3.00, 4.20, 4.65, 5.25, 6.00, 7.50, 10.10, 14.50, 19.75 MeV/nucleon; ²⁷Al(²⁰Ne, X)⁴⁷V*, E=3.00, 4.05, 4.25, 4.65, 5.25, 6.00, 6.90, 7.50, 9.00, 10.50, 14.50, 19.75 MeV/nucleon; ¹²C(³⁵Cl, X)⁴⁷V*, E=3.57, 4.00, 4.40, 5.14, 5.71, 7.94 MeV/nucleon; ³²S(¹⁶O, X)⁴⁸Cr*, E=10.50 MeV/nucleon; ⁴⁰Ca(¹⁶O, X)⁵⁶Ni*, E=3.11, 3.47, 3.92, 4.65, 6.47, 8.73, 13.38 MeV/nucleon; ²⁸Si(²⁸Si, X)⁵⁶Ni*, E=3.21, 3.57, 3.93, 4.29, 5.00, 6.21, 7.68, 8.57, 11.04, 12.04, 14.18, 16.14, 19.70, 20.00, 22.00, 26.00, 30.00, 35.00 MeV/nucleon; ²⁴Mg(³²S, X)⁵⁶Ni*, E=3.95, 4.40, 5.00, 5.75, 6.06, 6.25, 7.47, 8.69 MeV/nucleon; ⁴⁰Ca(¹⁹F, X)⁵⁹Cu*, E=3.45, 4.13, 5.03, 5.42, 6.00, 9.00, 11.37 MeV/nucleon; ²⁷Al(³²S, X)⁵⁹Cu*, E=4.43, 4.77, 5.47, 5.86, 7.09, 7.94, 10.00, 10.50, 11.44, 12.28 MeV/nucleon; ²⁴Mg(³⁵Cl, X)⁵⁹Cu*, E=7.86, 8.07 MeV/nucleon; ⁴⁸Ti(¹²C, X)⁶⁰Ni*, E=6.75, 8.13, 15.00 MeV/nucleon; ⁴⁰Ca(²³Na, X)⁶³Ga*, E=11.30, 12.48 MeV/nucleon; Ti(¹⁶O, X), E=14.19, 19.38 MeV/nucleon; ⁵²Cr(¹⁴N, X)⁶⁶Ga*, E=11.21, 18.71 MeV/nucleon; ²⁷Al(⁴⁰Ar, X)⁶⁷Ga*, E=55.00 MeV/nucleon; ⁴⁰Ca(²⁸Si, X)⁶⁸Se*, E=10.64, 11.04, 11.68, 14.18, 16.14 MeV/nucleon; ⁵⁸Ni(¹²C, X)⁷⁰Se*, E=5.32, 6.75, 8.04, 8.13, 15.00 MeV/nucleon; ⁵⁸Ni(¹⁴N, X)⁷²Br*, E=11.21, 18.71 MeV/nucleon; K, Cl(³⁶Ar, X), E=31.58, 40.03, 51.78 MeV/nucleon; ⁶³Cu(¹²C, X)⁷⁵Br*, E=5.32, 6.75, 8.04, 8.13 MeV/nucleon; ⁴⁰Ca(⁴⁰Ar, X)⁸⁰Sr*, E=4.02, 4.75, 5.90, 6.83, 15.00, 20.00, 30.00 MeV/nucleon; ⁴⁰Ca(⁴⁰Ca, X)⁸⁰Zr*, E=3.55, 3.67, 3.85, 4.05, 4.25, 4.38, 4.55, 4.88, 7.50 MeV/nucleon; ²⁷Al(⁵⁸Ni, X)⁸⁵Nb*, E=28.00 MeV/nucleon; ⁶³Cu(²⁴Mg, X)⁸⁷Nb*, E=6.71, 9.38, 11.71, 14.21 MeV/nucleon; ⁴⁵Sc(⁴⁸Ti, X)⁹³Tc*, E=15.98 MeV/nucleon; ⁵⁸Ni(³⁶Ar, X)⁹⁴Pd*, E=31.58, 40.03, 51.78 MeV/nucleon; ⁹²Mo(¹⁶O, X)¹⁰⁸Sn*, E=11.70 MeV/nucleon; ⁷⁶Ge(³²S, X)¹⁰⁸Cd*, E=4.94, 5.56, 6.19, 6.81, 7.03 MeV/nucleon; ⁶⁸Zn(⁴⁰Ar, X)¹⁰⁸Cd*, E=14.60, 19.60, 27.55, 35.00 MeV/nucleon; ⁵⁶Fe(⁵²Cr, X)¹⁰⁸Sn*, E=5.10 MeV/nucleon; ⁹³Nb(¹⁹F, X)¹¹²Sn*, E=3.84, 5.00 MeV/nucleon; ⁴⁸Ti(⁶⁴Zn, X)¹¹²Te*, E=35.00, 50.00 MeV/nucleon; ⁵⁸Ni(⁵⁸Ni, X)¹¹⁶Ba*, E=32.00, 40.50, 51.50, 63.50 MeV/nucleon; ¹⁰⁰Mo(¹⁸O, X)¹¹⁸Sn*, E=5.56, 8.33, 9.39, 10.28, 12.06 MeV/nucleon; ⁴⁰Ca(⁷⁸Kr, X)¹¹⁸Ba*, E=5.50 MeV/nucleon; ⁴⁰Ca(⁸²Kr, X)¹²²Ba*, E=5.50 MeV/nucleon; ¹²⁴Sn(¹²C, X)¹³⁶Ba*, E=30.00, 49.00, 84.00 MeV/nucleon; ¹²⁴Sn(¹⁴N, X)¹³⁸La*, E=10.00, 20.00, 30.00 MeV/nucleon; ¹²⁴Sn(²⁰Ne, X)¹⁴⁴Nd*, E=20.00, 30.00 MeV/nucleon; ¹⁰⁸Ag(⁴⁰Ar, X)¹⁴⁸Tb*, E=4.22, 4.93, 5.90, 7.20, 8.40, 8.43, 27.40 MeV/nucleon; ⁶⁵Cu(⁸⁴Kr, X)¹⁴⁹Ho*, E=5.88, 7.19 MeV/nucleon; ¹¹⁶Sn(⁴⁰Ar, X)¹⁵⁶Er*, E=4.63, 5.50, 6.78, 8.48 MeV/nucleon; ¹²¹Sb(⁴⁰Ar, X)¹⁶¹Tm*, E=4.97, 5.65, 7.05, 7.50 MeV/nucleon; ¹⁴⁶Nd(¹⁶O, X)¹⁶²Er*, E=10.06 MeV/nucleon; ³⁰Si(¹³²Xe, X)¹⁶²Er*, E=5.40, 5.90, 6.60, 7.50, 8.20 MeV/nucleon; ¹²⁴Sn(⁴⁰Ar, X)¹⁶⁴Er*, E=24.00, 27.00 MeV/nucleon; ¹⁵⁴Sm(¹⁴N, X)¹⁶⁸Tm*, E=35.00, 100.00, 130.00, 135.00 MeV/nucleon; ¹⁵⁹Tb(¹⁴N, X)¹⁷³Hf*, E=22.07, 35.00, 100.00 MeV/nucleon; ¹⁵⁹Tb(¹⁶O, X)¹⁷⁵Ta*, E=14.00, 25.00 MeV/nucleon; ¹⁵⁹Tb(²⁰Ne, X)¹⁷⁹Re*, E=8.00, 10.00, 13.00, 16.00 MeV/nucleon; ¹²⁴Sn(⁵⁸Ni, X)¹⁸²Pt*, E=3.96, 4.12.4.28.4.66.5.00 MeV/nucleon; ¹⁶⁵Ho(²⁰Ne, X)¹⁸⁵Ir*, E=30.00 MeV/nucleon; ¹⁶⁹Tm(²⁰Ne, X)¹⁸⁹Au*, E=8.00, 10.00, 13.00, 16.00 MeV/nucleon; ¹⁸²W(¹²C, X)¹⁹⁴Hg*, E=10.08, 13.92 MeV/nucleon; ¹⁷⁵Lu(¹⁹F, X)¹⁹⁴Hg*, E=7.11, 9.68 MeV/nucleon; ¹⁵⁴Sm(⁴⁰Ar, X)¹⁹⁴Hg*, E=5.53, 6.80, 8.50 MeV/nucleon; ¹⁸¹Ta(¹⁴N, X)¹⁹⁵Hg*, E=35.00 MeV/nucleon; ¹⁸¹Ta(¹⁶O, X)¹⁹⁷Tl*, E=14.00, 25.00 MeV/nucleon; ¹⁶⁴Dy(⁴⁰Ar, X)²⁰⁴Po*, E=5.53, 6.80, 8.48 MeV/nucleon; ¹⁸¹Ta(²⁴Mg, X)²⁰⁵At*, E=11.25, 13.96, 14.17 MeV/nucleon; ¹⁶⁵Ho(⁴⁰Ar, X)²⁰⁵At*, E=5.65, 7.00, 7.50, 7.88, 8.50, 9.77 MeV/nucleon; ¹⁹⁷Au(¹²C, X)²⁰⁹At*, E=86.00 MeV/nucleon; ¹⁹⁷Au(¹⁴N, X)²¹¹Rn*, E=35.00, 100.00, 130.00, 155.00 MeV/nucleon; ¹⁹⁷Au(¹⁶O, X)²¹³Fr*, E=14.00, 107.00 MeV/nucleon; ¹⁹⁷Au(²⁰Ne, X)²¹⁷Ac*, E=7.50, 11.00, 14.50, 20.00, 30.00 MeV/nucleon; ¹⁹⁷Au(⁴⁰Ar, X)²³⁷Bk*, E=5.47, 5.68, 6.20, 6.75, 8.40, 8.48, 8.57 MeV/nucleon; ²⁰⁹Bi(²⁰Ne, X)²²⁹Np*, E=30.00 MeV/nucleon; ²³²Th(¹⁴N, X)²⁴⁶Bk*, E=30.00 MeV/nucleon; ²³⁸U(⁴⁰Ar, X)²⁷⁸Ds*, E=6.25, 7.50, 8.50, 10.40 MeV/nucleon; Analyzed 382 complete and incomplete fusion σ data relative to 81 systems, A=26-278, E ≈ 3-155 MeV/nucleon; distinguished evaporation and fusion-fission mechanisms; deduced universal homographic law of fusion from properly normalized and scaled fusion σ(E) data, threshold for incomplete fusion, energy of vanishing of complete and incomplete fusion; proposed a reaction mechanism for fusion disappearance.

doi: 10.1103/PhysRevC.90.034609
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2013EU01      Europhys.Lett. 104, 22001 (2013)

P.Eudes, Z.Basrak, F.Sebille, V.de la Mota, G.Royer

Towards a unified description of evaporation-residue fusion cross-sections above the barrier

NUCLEAR REACTIONS ¹²⁴Sn(¹²C, X), ²⁸Si(²⁸Si, X), ⁹⁶Zr(³⁶Ar, X), E<20 MeV/nucleon; analyzed available data for 300 fusion evaporation σ; deduced a universal homographic law. DYWAN microscopic transport model.

doi: 10.1209/0295-5075/104/22001
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2011SE11      Phys.Rev. C 84, 055801 (2011)

F.Sebille, V.de la Mota, S.Figerou

Probing the microscopic nuclear matter self-organization processes in the neutron star crust

doi: 10.1103/PhysRevC.84.055801
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2009SE04      Nucl.Phys. A822, 51 (2009)

F.Sebille, S.Figerou, V.de la Mota

Self-consistent dynamical mean-field investigation of exotic structures in isospin-asymmetric nuclear matter

doi: 10.1016/j.nuclphysa.2009.02.013
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2007SE09      Phys.Rev. C 76, 024603 (2007)

F.Sebille, V.de la Mota, I.C.Sagrado Garcia, J.F.Lecolley, V.Blideanu

Probing the nuclear matter isospin asymmetry by nucleon-induced reactions at Fermi energies

NUCLEAR REACTIONS ²⁰⁸Pb(n, pX), E=96 MeV; ²⁰⁸Bi(n, pX), (p, pX), E=63 MeV; analyzed σ.

doi: 10.1103/PhysRevC.76.024603
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2007SE13      Nucl.Phys. A791, 313 (2007)

F.Sebille, V.de la Mota, I.C.Sagrado Garcia, J.F.Lecolley, V.Blideanu

Analysis of emission mechanisms in nucleon-induced reactions around the Fermi energy

NUCLEAR REACTIONS ²⁰⁸Pb(p, nX), E=62 MeV; ²⁰⁸Pb(n, pX), E=96 MeV; ²⁰⁸Pb(p, pX), E=62 MeV; ²⁰⁸Pb(n, nX), E=96 MeV; calculated σ and angular distributions in the framework of the microscopic DYWAN model.

doi: 10.1016/j.nuclphysa.2007.04.024
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2005SE12      Nucl.Phys. A756, 229 (2005)

F.Sebille, C.Bonilla, V.Blideanu, J.F.Lecolley

Investigation of nucleon-induced reactions in the Fermi energy domain within the microscopic DYWAN model

NUCLEAR REACTIONS ²⁰⁸Pb(n, pX), (n, dX), (n, tX), (n, αX), E=96 MeV; Fe, Sn, Bi(p, pX), (p, dX), (p, tX), (p, αX), E ≈ 62 MeV; calculated light charged particle spectra, σ(E). Dynamical wavelet model, comparison with data.

doi: 10.1016/j.nuclphysa.2005.03.010
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2004DE58      Braz.J.Phys. 34, 781 (2004)

V.de la Mota, F.Sebille, C.Bonilla

Dissipative and Fluctuating Dynamical Description of Nuclear Reactions

NUCLEAR REACTIONS Ag(Ar, X), E=27, 44 MeV/nucleon; calculated heavy fragments recoil velocities vs angle. ²⁰⁸Pb(n, pX), E=96 MeV; calculated proton spectra, σ(E, θ). Dynamical model, comparison with data.

doi: 10.1590/s0103-97332004000500019
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2002DE69      Acta Phys.Hung.N.S. 16, 203 (2002)

V.de la Mota, F.Sebille

Nuclear Dynamics with a Wavelet Representation

NUCLEAR REACTIONS ¹⁰⁷Ag(⁴⁰Ar, X), E=27, 44 MeV/nucleon; ¹⁰⁰Mo(¹⁰⁰Mo, X), E=18.7 MeV/nucleon; calculated fragment energy and angular distributions. ⁵⁸Ni(³⁶Ar, X), E=95 MeV/nucleon; calculated fragment multiplicities and rapidity spectra. Pb(n, pX), E=62.7 MeV; calculated Ep, σ(E, θ). Dynamical wavelet approach.

doi: 10.1556/APH.16.2002.1-4.23
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2001DE57      Eur.Phys.J. A 12, 479 (2001)

V.de la Mota, F.Sebille

Dissipative and Fluctuating Effects in Nuclear Dynamics with a Wavelet Representation

NUCLEAR REACTIONS ¹⁰⁷Ag(⁴⁰Ar, X), E=27, 44 MeV/nucleon; ¹⁰⁰Mo(¹⁰⁰Mo, X), E=18.7 MeV/nucleon; calculated fragments velocity and angular distributions; deduced fluctuation and dissipation effects. Wavelet representation, comparisons with data and other models.

doi: 10.1007/s10050-001-8670-4
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1999HA45      Phys.Rev. C60, 031603 (1999)

F.Haddad, Ph.Eudes, Z.Basrak, F.Sebille

Signature of Geometrical Effects in Heavy-Ion Reactions below 100 MeV/Nucleon

NUCLEAR REACTIONS ²⁷Al, ¹⁰⁷Ag(⁴⁰Ar, X), ⁴⁰Ar(¹⁰⁷Ag, X), ⁵⁸Ni(³⁶Ar, X), ¹²⁹Sn(¹²⁰Xe, X), E=41-100 MeV/nucleon; calculated charged particle dynamical emission percentage vs energy, impact parameter. Landau-Vlasov model, comparison with data.

doi: 10.1103/PhysRevC.60.031603
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1998DE54      Nuovo Cim. 111A, 881 (1998)

V.de la Mota, B.Jouault, F.Sebille, S.Priault

The DYWAN Model and the Description of Transport Phenomena in Nuclei

NUCLEAR REACTIONS Ca(Ca, X), E=30, 50, 90 MeV/nucleon; calculated density vs time. Dynamical model.

NUCLEAR STRUCTURE Ca, Pb; calculated binding energies, radii. Dynamical model.

doi: 10.1007/BF03035973
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1998JO02      Nucl.Phys. A628, 119 (1998)

B.Jouault, F.Sebille, V.de la Mota

Wavelet Representation of the Nuclear Dynamics

NUCLEAR REACTIONS C(C, X), E=84 MeV/nucleon; Ca(Ca, X), E=30, 50, 90 MeV/nucleon; calculated particle density vs time. Dynamical-wavelet-in-nuclei model.

doi: 10.1016/S0375-9474(97)00610-6
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1997BA79      Nucl.Phys. A624, 472 (1997)

Z.Basrak, P.Eudes, P.Abgrall, F.Haddad, F.Sebille

Effects of the Mean-Field Dynamics and the Phase-Space Geometry on the Cluster Formation

NUCLEAR REACTIONS ²⁷Al(⁴⁰Ar, X), E=65 MeV/nucleon; calculated density vs time, charge, rapidity, multiplicity distributions. Dynamically generated one-body phase space, Landau-Vlasov model.

doi: 10.1016/S0375-9474(97)00393-X
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1997EU01      Phys.Rev. C56, 2003 (1997)

Ph.Eudes, Z.Basrak, F.Sebille

Dynamical Aspects of Particle Emission in Binary Dissipative Collisions: Effects on hot-nuclei formation

NUCLEAR REACTIONS ²⁷Al(⁴⁰Ar, X), E=65 MeV/nucleon; analyzed light charged particle rapidity distributions, multiplicity, invariant σ; deduced dynamical effects. Landau-Vlasov model.

doi: 10.1103/PhysRevC.56.2003
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1997JO05      Nucl.Phys. A615, 82 (1997)

B.Jouault, G.Royer, J.F.Lecolley, F.Sebille, F.Haddad

Comparison between the Fragmentation Processes in Central Pb + Ag and Pb + Au Collisions

NUCLEAR REACTIONS Ag(Pb, X), E=29 MeV/nucleon; ¹⁹⁷Au(Pb, X), E=29 MeV/nucleon; calculated densities, Coulomb, surface energies time evolution, fragment velocities, kinetic energies. Landau-Vlasov model, medium mass fragmentation process.

doi: 10.1016/S0375-9474(96)00477-0
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1997LU02      Phys.Rev. C55, 1906 (1997)

J.Lukasik, J.Benlliure, V.Metivier, E.Plagnol, B.Tamain, M.Assenard, G.Auger, Ch.O.Bacri, E.Bisquer, B.Borderie, R.Bougault, R.Brou, Ph.Buchet, J.L.Charvet, A.Chbihi, J.Colin, D.Cussol, R.Dayras, A.Demeyer, D.Dore, D.Durand, E.Gerlic, S.Germain, D.Gourio, D.Guinet, P.Lautesse, J.L.Laville, J.F.Lecolley, A.Le Fevre, T.Lefort, R.Legrain, O.Lopez, M.Louvel, N.Marie, L.Nalpas, M.Parlog, J.Peter, O.Politi, A.Rahmani, T.Reposeur, M.F.Rivet, E.Rosato, F.Saint-Laurent, M.Squalli, J.C.Steckmeyer, M.Stern, L.Tassan-Got, E.Vient, C.Volant, J.P.Wieleczko, M.Colonna, F.Haddad, Ph.Eudes, T.Sami, F.Sebille

Dynamical Effects and Intermediate Mass Fragment Production in Peripheral and Semicentral Collisions of Xe + Sn at 50 MeV/nucleon

NUCLEAR REACTIONS Sn(Xe, X), E=50 MeV/nucleon; measured invariant cm velocity, mean multiplicity of p, d, t, ³He, α, Z ≤ 15 fragments; deduced dynamically influenced emission relative to isotropic statistical evaporation, possible reaction mechanism. Dynamical models.

doi: 10.1103/PhysRevC.55.1906
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1997RE03      Z.Phys. A357, 79 (1997)

T.Reposeur, V.de la Mota, F.Sebille, C.O.Dorso

Signals of Fragment Structures from a Semiclassical Transport Equation in Heavy-Ion Collisions

NUCLEAR REACTIONS ⁵⁸Ni(³⁶Ar, X), E=32-95 MeV/nucleon; analyzed charged product, intermediate mass fragment multiplicity data. Semi-classical transport equation.

doi: 10.1007/s002180050217
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1996HA07      Phys.Rev. C53, 1437 (1996)

F.Haddad, J.B.Natowitz, B.Jouault, V.de la Mota, G.Royer, F.Sebille

Compressibility Probed by Linear Momentum Transfer

NUCLEAR REACTIONS ²³⁸U(¹⁶O, X), E=20-70 MeV/nucleon; ¹⁵⁴Sm, ²³⁸U(¹⁴N, X), ²³²Th(α, X), ⁵⁸Ni, ²³⁸U(¹²C, X), ⁶⁸Zn, ²³²Th, ¹⁹⁷Au(⁴⁰Ar, X), E not given; analyzed linear momentum transfer related features, compressibility characteristics for these, other reactions. Landau-Vlasov model.

doi: 10.1103/PhysRevC.53.1437
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1996HA21      Z.Phys. A354, 321 (1996)

F.Haddad, B.Borderie, V.de la Mota, M.F.Rivet, F.Sebille, B.Jouault

Dynamical Analysis of Dissipative Collisions between Ar and Ag Nuclei in the Fermi Energy Domain

NUCLEAR REACTIONS ¹⁰⁷Ag(⁴⁰Ar, X), E=27, 44 MeV/nucleon; calculated binary collisions primary partners main characteristics; deduced temperature parameter estimates. Landau Vlasov microscopic transport model.

doi: 10.1007/s002180050052
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1996JO04      Nucl.Phys. A597, 136 (1996)

B.Jouault, V.de la Mota, F.Sebille, G.Royer, J.F.Lecolley

Dynamical Analysis of Isospin and Angular Momentum Effects in Peripheral Heavy-Ion Reactions

NUCLEAR REACTIONS ¹⁹⁷Au(Pb, X), E=29 MeV/nucleon; analyzed data; deduced dynamical, out-of-equilibrium effects role.

doi: 10.1016/0375-9474(95)00428-9
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1995HA27      Phys.Rev. C52, 2013 (1995)

F.Haddad, F.Sebille, M.Farine, V.de la Mota, P.Schuck, B.Jouault

Effects of Gogny-Type Interactions on the Nuclear Flow

NUCLEAR REACTIONS ⁹³Nb(⁹³Nb, X), E ≤ 400 MeV/nucleon; calculated flow parameter vs E, mean density vs time. ¹⁹⁷Au(¹⁹⁷Au, X), Pb(Ar, X), E=400 MeV/nucleon; calculated flow parameter vs impact parameter; deduced incompressibility modulus. Semi-classical Landau-Vlasov approach.

doi: 10.1103/PhysRevC.52.2013
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1995JO19      Nucl.Phys. A591, 497 (1995)

B.Jouault, F.Sebille, G.Royer, V.de la Mota

Fragmentation in Central Pb + Au Collisions within a Microscopic Dynamic Approach

NUCLEAR REACTIONS ¹⁹⁷Au(²⁰⁸Pb, X), E=29 MeV/nucleon; analyzed mean density, surface, Coulomb, collective energies time evolution. Microscopic dynamic approach.

doi: 10.1016/0375-9474(95)00174-Y
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1995RE05      Nucl.Phys. A583, 323c (1995)

B.Remaud, B.Benhassine, M.Farine, D.Idier, F.Sebille

Dynamics of Fluctuations in Heavy-Ion Reactions

doi: 10.1016/0375-9474(94)00679-H
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1994AB01      Phys.Rev. C49, 1040 (1994)

P.Abgrall, F.Haddad, V.de la Mota, F.Sebille

Study of Energy Deposition in Heavy-Ion Reactions

NUCLEAR REACTIONS Ca(Ca, X), E=40, 60 MeV/nucleon; calculated energy distribution, residue excitation vs time. Ca(Ca, X), Pb(Pb, X), E ≈ 25-100 MeV/nucleon; calculated relaxation time vs E. Semi-classical Landau-Vlasov model.

doi: 10.1103/PhysRevC.49.1040
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1994HA10      Nucl.Phys. A572, 459 (1994)

F.Haddad, G.Royer, F.Sebille, B.Remaud

From Fission to Scattering in the ¹⁰⁰Mo (18.7 MeV/u) + ¹⁰⁰Mo Reaction within a Microscopic Dynamic Approach

NUCLEAR REACTIONS ¹⁰⁰Mo(¹⁰⁰Mo, F), E=18.7 MeV/nucleon; calculated symmetric fission, fragmentation barriers. ¹⁰⁰Mo(¹⁰⁰Mo, X), E=18.7 MeV/nucleon; calculated per nucleon collective energy vs time from equilibration, other reaction dynamics. Landau-Vlasov transport equation.

doi: 10.1016/0375-9474(94)90184-8
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1994ID03      Ann.Phys.(Paris) 19, 159 (1994)

D.Idier, M.Farine, B.Remaud, F.Sebille

Modelling an Infinite Nucleonic System. Static and Dynamical Properties. Study of Density Fluctuations

1993BO04      Phys.Lett. 302B, 15 (1993)

B.Borderie, B.Remaud, M.F.Rivet, F.Sebille

Coulomb Instability in Collisions between Very Heavy Nuclei Around 30 MeV per Nucleon

NUCLEAR REACTIONS ¹⁵⁵Gd(²³⁸U, X), E=35 MeV/nucleon; calculated Coulomb instability; deduced unstable bubbles formation.

doi: 10.1016/0370-2693(93)90628-U
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1992DE25      Z.Phys. A343, 417 (1992)

V.de la Mota, F.Sebille, B.Remaud, P.Schuck

On the Competing Role of Mean-Field and Residual Interactions in Flow Observables

NUCLEAR REACTIONS ⁹³Nb(⁹³Nb, X), E=150 MeV/nucleon; calculated flow observables; deduced mean field, residual interactions role. Semi-classical Landau-Vlasov approach.

doi: 10.1007/BF01289818
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1992DE34      Phys.Rev. C46, 677 (1992)

V.de la Mota, F.Sebille, M.Farine, B.Remaud, P.Schuck

Analysis of the Transverse Momentum Collective Motion in Heavy-Ion Collisions below 100 MeV/Nucleon

NUCLEAR REACTIONS ⁹³Nb(⁹³Nb, X), Ca(Ca, X), C(C, X), E=50-100 MeV/nucleon; calculated collective sideward flow vs E. ²⁷Al(Ar, X), E=45, 65 MeV/nucleon; calculated mean transverse momentum vs longitudinal rapidity. Gogny type forces.

doi: 10.1103/PhysRevC.46.677
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1991FA08      Z.Phys. A339, 363 (1991)

M.Farine, T.Sami, B.Remaud, F.Sebille

Isospin Effects on Dynamics of Heavy-Ion Collisions

NUCLEAR REACTIONS ⁴⁸Ca(⁴⁸Ca, X), E=40 MeV/nucleon; calculated nucleon emission number vs model parameter; deduced isospin role on reaction dynamics. Landau-Valasov formalism, effective force.

doi: 10.1007/BF01560638
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1991GA04      Phys.Lett. 255B, 311 (1991)

F.Garcias, V.De La Mota, B.Remaud, G.Royer, F.Sebille

Dynamics of Hot Rotating Nuclei

NUCLEAR STRUCTURE ⁴⁰Ca; calculated binding energy per nucleon, rms radius, deexcitation channels phase diagram; deduced fission disappearance at high excitation. Hot rotating nuclei, microscopic semi-classical transport formalism.

doi: 10.1016/0370-2693(91)90771-H
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1991JO12      Z.Phys. A340, 63 (1991)

D.Jouan, B.Borderie, M.F.Rivet, C.Cabot, H.Fuchs, H.Gauvin, C.Gregoire, F.Hanappe, D.Gardes, M.Montoya, B.Remaud, F.Sebille

Dynamics and Thermalization in Violent Collisions between ⁴⁰Ar and Ag at 27 MeV/nucleon

NUCLEAR REACTIONS Ag(⁴⁰Ar, X), E=27 MeV/nucleon; measured (fragment)(fragment)-coin; deduced reaction mechanism.

doi: 10.1007/BF01284482
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1991RO06      Phys.Rev. C44, 2226 (1991)

G.Royer, B.Remaud, F.Sebille, V.de la Mota

Semiclassical Simulation of Sudden Nucleus Scission with Two-Body Collisions

NUCLEAR STRUCTURE ⁴⁰Ca; calculated fission barrier heights. Semi-classical simulation, two-body collision effects.

doi: 10.1103/PhysRevC.44.2226
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1990AR12      Nucl.Phys. A514, 564 (1990)

D.Ardouin, Z.Basrak, P.Schuck, A.Peghaire, F.Saint-Laurent, H.Delagrange, H.Doubre, C.Gregoire, A.Kyanowski, W.Mittig, J.Peter, Y.P.Viyogi, J.Quebert, C.K.Gelbke, W.G.Lynch, M.Maier, J.Pochodzalla, G.Bizard, F.Lefebvres, B.Tamain, B.Remaud, F.Sebille

Preequilibrium Particles and Mean-Field Effects from Particle-Particle Correlations in Heavy-Ion Collisions

NUCLEAR REACTIONS ¹⁹⁷Au, Ti(⁴⁰Ar, X), E=60 MeV/nucleon; measured (particle)(particle) correlations for X=p, d, α; deduced mean-field, two-body collisions effects. Landau-Vlasov equation analysis.

doi: 10.1016/0375-9474(90)90156-G
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1990DA16      Phys.Lett. 247B, 223 (1990)

H.Dabrowski, D.Goujdami, F.Guilbault, C.Lebrun, D.Ardouin, P.Lautridou, R.Boisgard, J.Quebert, A.Peghaire, P.Eudes, F.Sebille, B.Remaud

Temperature Measurements at Backward Angles in ⁴⁰Ar Induced Reactions on Ag at E/A = 44 MeV

NUCLEAR REACTIONS Ag(⁴⁰Ar, X), E=44 MeV/nucleon; measured pt-, dα-correlation; deduced target-like fragment emission temperature.

doi: 10.1016/0370-2693(90)90886-B
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1989LE15      Nucl.Phys. A495, 283c (1989)

S.Leray, C.Ngo, M.E.Spina, B.Remaud, F.Sebille

Multifragmentation in the Framework of a Restructured Aggregation Model

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=200 MeV/nucleon; calculated fragment yield vs mass, multiplicity distribution. Restructured aggregation model.

doi: 10.1016/0375-9474(89)90326-6
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1989SE10      Nucl.Phys. A501, 137 (1989)

F.Sebille, G.Royer, C.Gregoire, B.Remaud, P.Schuck

Nuclear Dynamics with the (Finite-Range) Gogny Force: Flow effects

NUCLEAR REACTIONS ⁹³Nb(⁹³Nb, X), E=150 MeV/nucleon; calculated average density time evolution. Landau-Vlasov equation, Gogny force.

doi: 10.1016/0375-9474(89)90569-1
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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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1988MI23      Nucl.Phys. A489, 461 (1988)

J.Mignen, G.Royer, F.Sebille

Comparison between the Symmetric Fission and Fusion Paths

NUCLEAR STRUCTURE ⁴⁰Ca, ¹⁰⁹Cd, ¹⁶⁰Dy, ²⁴⁰Pu; calculated deformation energy vs fission fragment distance. Liquid drop model, nuclear proximity energy.

doi: 10.1016/0375-9474(88)90007-3
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1987GR04      Phys.Lett. 186B, 14 (1987)

C.Gregoire, B.Remaud, F.Sebille, L.Vinet

Peripheral Reactions at Intermediate Energies in Landau-Vlasov Dynamics

NUCLEAR REACTIONS ²⁷Al(⁴⁰Ar, X), E=44 MeV/nucleon; calculated target fragment average recoil vs projectile-like mass, projectile-like fragment mean energy vs mass, bombarding energy per nucleon vs abraded nucleon number; ⁴⁰Ca(¹⁶O, X), E=25 MeV/nucleon; calculated time evolution; ¹⁰⁸Ag(⁴⁰Ar, X), E=35 MeV/nucleon; calculated projectile-like fragment isospin vs time. Landau-Vlasov dynamics.

doi: 10.1016/0370-2693(87)90504-1
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1987GR09      Nucl.Phys. A465, 317 (1987)

C.Gregoire, B.Remaud, F.Sebille, L.Vinet, Y.Raffray

Semi-Classical Dynamics of Heavy-Ion Reactions

NUCLEAR REACTIONS ²⁷Al(⁴⁰Ar, X), E=27, 35 MeV/nucleon; calculated collision dynamics characteristics. Extended Vlasov equation.

doi: 10.1016/0375-9474(87)90437-4
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1987GR29      J.Phys.(Paris), Colloq.C-2, 203 (1987)

C.Gregoire, B.Remaud, F.Sebille, L.Vinet, D.Jacquet

Low and Intermediate Energy Heavy Ion Collisions in the Semi-Classical Microscopic Description

NUCLEAR REACTIONS ²⁷Al(⁴⁰Ar, X), E=27, 35, 44 MeV/nucleon; ²⁸Si(²⁸Si, X), E=12 MeV/nucleon; ²³⁸U(⁴⁰Ar, X), E=27 MeV/nucleon; ⁴⁰Ca(¹⁶O, X), E=5.5 MeV/nucleon; calculated fragment mass-mass correlations, ejectile energies, σ(θ). Landau-Vlasov dynamics.

1987VI03      Nucl.Phys. A468, 321 (1987)

L.Vinet, C.Gregoire, P.Schuck, B.Remaud, F.Sebille

A Study of the Disintegration of Highly Excited Nuclei with the Vlasov-Uehling-Uhlenbeck Equation

NUCLEAR STRUCTURE ⁴⁰Ca; calculated fragmentation density profile time evolution, anisotropy, monopole Landau parameters, energy per nucleon, density distributions. ⁴⁰Ar; calculated energy, excitation energy per nucleon, mean kinetic energy time evolution in fragmentation.

doi: 10.1016/0375-9474(87)90520-3
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1986VI03      Phys.Lett. 172B, 17 (1986)

L.Vinet, F.Sebille, C.Gregoire, B.Remaud, P.Schuck

Solution of the Vlasov Equation for Compressed and Heated Spherical Nuclei

NUCLEAR STRUCTURE ⁴⁰Ca, ¹⁶O; calculated rms radius, density time evolutions.

doi: 10.1016/0370-2693(86)90208-X
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1985GR07      Nucl.Phys. A436, 365 (1985)

C.Gregoire, B.Remaud, F.Scheuter, F.Sebille

Semiclassical Approaches to Proton Emission in Intermediate-Energy Heavy-Ion Reactions

NUCLEAR REACTIONS ¹²C(¹²C, pX), E=1032 MeV; calculated σ(Ep, θp); deduced one- to two-body process transition. Semi-classical approach.

doi: 10.1016/0375-9474(85)90203-9
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1983SE05      Z.Phys. A310, 99 (1983)

F.Sebille, B.Remaud

Cold Production of Fast Nucleons in Central Heavy-Ion Reactions

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, X), E=10-60 MeV/nucleon; calculated fast nucleon intensities, tunneling multiplicities; deduced reaction mechanism. Semi-classical model.

doi: 10.1007/BF01433617
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