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  • Independence of fragment ch...
    Rivet, M.F.; Bacri, Ch.O.; Borderie, B.; Frankland, J.D.; Assenard, M.; Auger, G.; Bocage, F.; Bougault, R.; Brou, R.; Buchet, Ph; Chbihi, A.; Colin, J.; Dayras, R.; Demeyer, A.; Doré, D.; Durand, D.; Eudes, P.; Galichet, E.; Genouin-Duhamel, E.; Gerlic, E.; Germain, M.; Guinet, D.; Lautesse, P.; Laville, J.L.; Lecolley, J.F.; Le Fèvre, A.; Lefort, T.; Legrain, R.; Le Neindre, N.; Lopez, O.; Louvel, M.; Nalpas, L.; Nguyen, A.D.; Parlog, M.; Péter, J.; Plagnol, E.; Rahmani, A.; Reposeur, T.; Rosato, E.; Saint-Laurent, F.; Salou, S.; Squalli, M.; Steckmeyer, J.C.; Stern, M.; Tabacaru, G.; Tamain, B.; Tassan-Got, L.; Tirel, O.; Vintache, D.; Volant, C.; Wieleczko, J.P.; Guarnera, A.; Colonna, M.; Chomaz, P.

    Physics letters. B, 07/1998, Letnik: 430, Številka: 3
    Journal Article

    Charged product multiplicities and Z distributions were measured for single multifragmenting sources produced in collisions between 129 Xe+ nat Sn and 155 Gd+ 238 U at the same available energy per nucleon. Z distributions are found identical for both reactions while fragment multiplicities scale as the charge of the total systems. A complete dynamical simulation, in which multifragmentation originates in the spinodal decomposition of a finite piece of nuclear matter resulting from an incomplete fusion of projectile and target, well accounts for this experimental observation.