Spallation reactions, as well as the standard theoretical tool for their study, namely the intra-nuclear cascade (INC) + evaporation model, are briefly introduced. The theoretical foundations and the domain of validity of the INC model are discussed in some detail.
IntroductionThe name "spallation reactions" refers in general to a high-energy hadron-nucleus reaction in the ∼200 MeV to ∼3 GeV incident energy range. 1 This specification of the energy range makes the definition more oriented towards the results of the reactions, which are sketched below, rather than on a particular reaction mechanism. We will actually argue in this paper that the reaction mechanism which prevails in the above-mentioned energy range does not change really when the incident energy decreases from 200 MeV down to a few tens of MeV. Likewise, the reaction mechanism does not really change either when the incident energy goes over the 3 GeV limit, as discussed in another presentation to this conference [1]. In Sect. 2 we will shortly review the properties of spallation reactions, in particular those that are important for technological applications, which, in turn, have largely contributed to the revived interest in these reactions. In Sect. 3, the standard theoretical tool, namely the intra-nuclear cascade (INC) + evaporation model is briefly introduced. The foundations of this empirical model are discussed in Sect. 4, in connection with transport theories. In Sect. 5, the most important assumptions of both INC and transport theories are examined. Section 6 contains our conclusion.
Properties of the Spallation ReactionsThe main property of the spallation reactions is a copious emission of light particles, mostly neutrons. The neutron multiplicity distribution for a typical case is shown in Fig. 1. On the average, about 15 neutrons are emitted. Light charged particles (protons, deuterons, tritons, etc.) and pions are also produced, at smaller (typically by an order of magnitude) rates. As a result, the target residue may be substantially lighter than the original target nucleus.This main property is enhanced when a high-energy proton beam hits a macroscopic piece of heavy metal, a so-called spallation source. The interaction process can be viewed as an iteration of microscopic spallation Presented at the workshop "30 years of strong interactions", Spa, Belgium, 6-8 April 2011.1 By extension, reactions induced by light nuclei with a kinetic energy per nucleon in the same energy range, are also denoted as "spallation reactions".