“…The fundamental problem was that the nuclei that were produced far above the target nucleus were the result of events with high total kinetic energy loss, i.e., high excitation energies and resulting poor survival probabilities. Very recently, Zagrebaev and Greiner [9][10][11][12][13][14][15][16], using a new model [17] for these collisions, have examined the older experiments and some proposed new experiments ( 232 Th + 250 Cf, 238 U + 238 U, and 238 U + 248 Cm). With their new model, which emphasizes the role of shell effects in damped collisions, they are able to correctly describe the previously measured fragment angular, energy, and charge distributions from the 136 Xe + 209 Bi reaction and the isotopic yields of Cf, Es, Fm, and Md from the 238 U + 248 Cm reaction.…”