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Search: Author = V.de la Mota

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2020BE11      Phys.Rev. C 101, 054608 (2020)

G.Besse, V.de la Mota, E.Bonnet, P.Eudes, P.Napolitani, Z.Basrak

Reexamining an extended-mean-field approach in heavy-ion collisions near the Fermi energy

NUCLEAR REACTIONS ⁵⁸Ni(⁵⁸Ni, X), ¹²⁹Xe(¹²⁰Sn, X), ⁴⁰Ar(⁶³Cu, X), (¹⁰⁷Ag, X), (¹⁹⁷Au, X), ¹⁹⁷Au(¹⁹⁷Au, X), E=20-120 MeV/nucleon; calculated stopping observables, energy isotropy ratio, large fluctuations, and linear momentum transfer using extended time-dependent Hartree-Fock (ETDHF) mean-field approach. Comparison with experimental data. Modeling of heavy-ion reactions at intermediate energies, and static and dynamical aspects of nuclear systems. ⁴⁰Ar, ⁵⁸Ni, ⁶³Cu, ¹⁰⁷Ag, ¹²⁰Sn, ¹²⁹Xe, ¹⁹⁷Au; calculated binding energies and mean-square radii using Hartree-Fock equations, and compared with experimental data.

doi: 10.1103/PhysRevC.101.054608
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2016BA24      Phys.Rev. C 93, 054609 (2016)

Z.Basrak, P.Eudes, V.de la Mota

Aspects of the momentum dependence of the equation of state and of the residual NN cross section, and their effects on nuclear stopping

NUCLEAR REACTIONS ¹²⁹Xe(¹²⁰Sn, X), E=12-100 MeV/nucleon; calculated nuclear stopping, energy-based isotropy ratio as stopping observable; investigated nuclear equation of state, effects of zero-range and non-local nuclear mean field, role of nucleon-nucleon residual interaction, isospin, energy and angular dependence of nucleon-nucleon cross section, in-medium modifications of nucleon-nucleon cross section, simplified parametrization of angular dependence of neutron-proton and proton-proton cross section; deduced fixed set of model parameters for energies below Fermi energy, for energies above Fermi energy model reproduces experimental data by parameters of in-medium modification of nucleon-nucleon cross section that smoothly evolve with energy, strong reduction of free nucleon-nucleon cross section around Fermi energy, effects of reaction centrality. Through Heavy-Ion Phase-Space Event generator (HIPSE) deduced that high multiplicity events are spread over a broad impact parameter range. Semiclassical Landau-Vlasov transport model (BUU type).

doi: 10.1103/PhysRevC.93.054609
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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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2014EU02      Nucl.Phys. A930, 131 (2014)

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

Is there incomplete fusion mechanism beyond 100A MeV?

doi: 10.1016/j.nuclphysa.2014.07.035
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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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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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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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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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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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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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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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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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1984DE29      Phys.Lett. 143B, 279 (1984)

V.de la Mota, C.O.Dorso, E.S.Hernandez

Damping of Quantal Collective Motion in Spherical Nuclei: Dissipation versus diffusion

NUCLEAR STRUCTURE ²⁰⁸Pb; calculated diffusive, dissipative isovector GDR evolution relative weight. Quantal collective vibration model.

doi: 10.1016/0370-2693(84)91465-5
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