MOS Classification: 34G10; 35B40; 35P05; 47D06; 45K05; 80A30 Fragmentation-coagulation processes, in which aggregates can break up or get together, often occur together with decay processes in which the components can be removed from the aggregates by a chemical reaction, evaporation, dissolution, or death. In this paper, we consider the discrete decay-fragmentation equation and prove the existence and uniqueness of physically meaningful solutions to this equation using the theory of semigroups of operators. In particular, we find conditions under which the solution semigroup is analytic, compact, and has the asynchronous exponential growth property. The theoretical analysis is illustrated by a number of numerical simulations. KEYWORDS asynchronous exponential growth, C 0 semigroups, discrete fragmentation, death process, long-term behaviour, numerical simulations, spectral gap
INTRODUCTIONFragmentation-coagulation processes, in which we observe breaking up of clusters of particles into smaller pieces or, conversely, creation of bigger clusters by an aggregation of smaller pieces, occur in many areas of science and engineering, where they describe polymerization and depolymerization, droplets formation and their breakup, grinding of rocks, formation of animal groups, or phytoplankton aggregates. 1-6 In many cases, fragmentation and coagulation are accompanied by other processes such as growth or decay of clusters due to chemical reactions, surface deposition from the solute or, conversely, dissolution and evaporation, or birth and death of cells forming the cluster. 4,7-10 Another process affecting the concentration of clusters is their sinking or sedimentation. 5,7 There are 2 main ways of modelling fragmentation-coagulation processes: the discrete one, in which we assume that each cluster is composed of a finite number of identical indivisible units called monomers 11 and the continuous one, where it is assumed that the size of the particles constituting the cluster can be an arbitrary positive number x ∈ R. 12 Consequently, the latter case is modelled by an integro-differential equation for the density of size x clusters, while in the former, we deal with an infinite system of ordinary differential equations for the densities of the clusters of size i ∈ N, also called i-mers. Similarly, the growth/decay process is modelled by a first-order (transport) differential 6530