We present an extensive simulation study of the kinetic behavior of the two-species annihilation reaction of the type A + B → 0, with input of species that takes place immediately after each reaction event. Simulations are performed by using lattices of length L in d = 1 dimension. Two different types of processes are considered: (i) the locally conservative kinetic (LCK) case, which involves the conservation of the densities of both types of particles during the whole reaction, and (ii) the so-called globally conservative kinetic (GCK) case where the total density of particles still remains constant, but after each reaction event, the type of particle to be introduced into the system is selected at random with the same probability. By starting from a random distribution of particles, it is found that the reaction rate, given by the number of reaction events per unit of time and length, decreases as a power law of the time according to Rate ∝ t
–β, with β = 1/2 and β = 1/4 for the GCK and LCK cases, respectively. It is found that the GCK never leads to the occurrence of a steady state, and the fluctuations of the density difference between different types of species in the lattice grow as ⟨γ2(t)⟩ ∝ t
δ, where δ = 1 is an exponent. However, for the LCK case, we observe that after a crossover time of the order of τ ∝ L
z
, where z = 2 is a dynamic exponent, the systems reach stationary regimes, such that Rate
stat ∝ ρ
X
, where ρ is the density of the species, and X = 3 is the (anomalous) reaction order. Our simulation results not only confirm some existing analytical predictions but also, in many kinetic scaling aspects, go beyond the present knowledge addressing new and interesting theoretical challenges.