359{
360 outFile
361 << "The GEANT4 precompound model is considered as an extension of the\n"
362 << "hadron kinetic model. It gives a possibility to extend the low energy range\n"
363 << "of the hadron kinetic model for nucleon-nucleus inelastic collision and it \n"
364 << "provides a ”smooth” transition from kinetic stage of reaction described by the\n"
365 << "hadron kinetic model to the equilibrium stage of reaction described by the\n"
366 << "equilibrium deexcitation models.\n"
367 << "The initial information for calculation of pre-compound nuclear stage\n"
368 << "consists of the atomic mass number A, charge Z of residual nucleus, its\n"
369 << "four momentum P0, excitation energy U and number of excitons n, which equals\n"
370 << "the sum of the number of particles p (from them p_Z are charged) and the number of\n"
371 << "holes h.\n"
372 << "At the preequilibrium stage of reaction, we follow the exciton model approach in ref. [1],\n"
373 << "taking into account the competition among all possible nuclear transitions\n"
374 << "with ∆n = +2, −2, 0 (which are defined by their associated transition probabilities) and\n"
375 << "the emission of neutrons, protons, deuterons, thritium and helium nuclei (also defined by\n"
376 << "their associated emission probabilities according to exciton model)\n"
377 << "\n"
378 << "[1] K.K. Gudima, S.G. Mashnik, V.D. Toneev, Nucl. Phys. A401 329 (1983)\n"
379 << "\n";
380}