The dynamic behavior of a multiagent system in which the agent size si is variable it is studied along a Lotka–Volterra approach. The agent size has hereby the meaning of the fraction of a given market that an agent is able to capture (market share). A Lotka–Volterra system of equations for...

Invariants of motion are constructed departing from the Gibbs entropy. The method we applied also allows us to find the subspace of a real vector space to which the system is confined to during its temporal evolution. We also find that the Uncertainty Principle is itself an invariant of motion...

The dynamical problem posed by the coupling of quantal to classical degrees of freedom is tackled, within the framework of the quantum friction phenomenon, by recourse to statistical methods embedded within Jaynes' maximum entropy principle.

We demonstrate that when the Gibbs entropy is an invariant of motion, following Information Theory procedures it is possible to define a generalized metric phase space for the temporal evolution of the mean values of a given Hamiltonian. The metric is positive definite and this fact leads to a...

Using the generalized Ehrenfest theorem the dynamics of the mean values of a complete set of non-commuting observables (CSNCO) associated to a given Hamiltonian is expressed. We found refined time-dependent invariants of motion (TDIM) for the CSNCO, and associated them with different Lie...

We present a general method to study the dynamics of quantum-classical systems. The emergency of chaotic motion in the classical limit together with the transition between regimes are also described.

Invariants of the Lewis kind are introduced within the context of Statistical Mechanics via information theory concepts. Several invariants of the Liouville equation are in this way built-up. Both the classical and the quantal cases are studied. Some applications are discussed. It is shown that...

The Maximum Entropy Principle (MEP) procedure is connected with the usual quantum techniques making clear the advantages of the former approach, especially when a set of non-compatible operators is used.