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We introduce a modified version of the disordered Klein-Gordon lattice model, having two parameters for controlling the disorder strength: $D$, which determines the range of the coefficients of the on-site potentials, and $W$, which defines the strength of the nearest-neighbor interactions. We fix $W=4$ and investigate how the properties of the systems normal modes change as we approach its ordered version, i.e. $Drightarrow 0$. We show that the probability density distribution of the normal modes frequencies takes a `U-shaped profile as $D$ decreases. Furthermore, we use two quantities for estimating the modes spatial extent, the so-called localization volume $V$ (which is related to the modes second moment) and the modes participation number $P$. We show that both quantities scale as $propto D^{-2}$ when $D$ approaches zero and we numerically verify a proportionality relation between them as $V/P approx 2.6$.
We implement several symplectic integrators, which are based on two part splitting, for studying the chaotic behavior of one- and two-dimensional disordered Klein-Gordon lattices with many degrees of freedom and investigate their numerical performanc
We consider paradigmatic quenched disordered quantum spin models, viz., the XY spin glass and random-field XY models, and show that quenched averaged quantum correlations can exhibit the order-from-disorder phenomenon for finite-size systems as well
We study the ladder operator on scalar fields, mapping a solution of the Klein-Gordon equation onto another solution with a different mass, when the operator is at most first order in derivatives. Imposing the commutation relation between the dAlembe
We study the chaotic behavior of multidimensional Hamiltonian systems in the presence of nonlinearity and disorder. It is known that any localized initial excitation in a large enough linear disordered system spreads for a finite amount of time and t
We study equilibrium properties of catalytically-activated $A + A to oslash$ reactions taking place on a lattice of adsorption sites. The particles undergo continuous exchanges with a reservoir maintained at a constant chemical potential $mu$ and rea