Abstract. We find a normal form which describes the high energy dynamics of a class of piecewise smooth Fermi-Ulam ping pong models; depending on the value of a single real parameter, the dynamics can be either hyperbolic or elliptic. In the first case we prove that the set of orbits undergoing Fermi acceleration has zero measure but full Hausdorff dimension. We also show that for almost every orbit the energy eventually falls below a fixed threshold. In the second case we prove that, generically, we have stable periodic orbits for arbitrarily high energies, and that the set of Fermi accelerating orbits may have infinite measure. 1. History and introduction In this paper we study the dynamics of piecewise smooth Fermi-Ulam ping pongs; Fermi...
We investigate with numerical methods the celebrated Fermi--Pasta--Ulam model, a chain of non--linea...
We investigate with numerical methods the scaling of the relaxation time to equipartion in the celeb...
The problem of a classical particle confined to bounce between two rigid walls, where one of them is...
In the thesis we describe the dynamics of two variations of the Fermi acceleration models. The firs...
In this paper we show an infinite measure set of exponentially escaping orbits for a resonant Fermi ...
Billiard maps are one of the most common types of dynamical systems. In recent years, billiards with...
Fermi acceleration in a Fermi-Ulam model, consisting of an ensemble of particles bouncing between tw...
The phenomenon of Fermi acceleration is addressed for the problem of a classical and dissipative bou...
Some phase space transport properties for a conservative bouncer model are studied. The dynamics of ...
The chaotic low energy region of the Fermi-Ulam simplified accelerator model is characterized by the...
Billiards with time dependent boundaries are a natural generalization of the one dimensional Fermi a...
The unlimited energy growth ( Fermi acceleration) of a classical particle moving in a billiard with ...
Abstract. We consider a dynamical system on the semi-infinite cylin-der which models the high energy...
Analytical arguments are used to describe the behavior of the average velocity in the problem of an ...
The phenomenon of Fermi acceleration is addressed for a dissipative bouncing ball model with externa...
We investigate with numerical methods the celebrated Fermi--Pasta--Ulam model, a chain of non--linea...
We investigate with numerical methods the scaling of the relaxation time to equipartion in the celeb...
The problem of a classical particle confined to bounce between two rigid walls, where one of them is...
In the thesis we describe the dynamics of two variations of the Fermi acceleration models. The firs...
In this paper we show an infinite measure set of exponentially escaping orbits for a resonant Fermi ...
Billiard maps are one of the most common types of dynamical systems. In recent years, billiards with...
Fermi acceleration in a Fermi-Ulam model, consisting of an ensemble of particles bouncing between tw...
The phenomenon of Fermi acceleration is addressed for the problem of a classical and dissipative bou...
Some phase space transport properties for a conservative bouncer model are studied. The dynamics of ...
The chaotic low energy region of the Fermi-Ulam simplified accelerator model is characterized by the...
Billiards with time dependent boundaries are a natural generalization of the one dimensional Fermi a...
The unlimited energy growth ( Fermi acceleration) of a classical particle moving in a billiard with ...
Abstract. We consider a dynamical system on the semi-infinite cylin-der which models the high energy...
Analytical arguments are used to describe the behavior of the average velocity in the problem of an ...
The phenomenon of Fermi acceleration is addressed for a dissipative bouncing ball model with externa...
We investigate with numerical methods the celebrated Fermi--Pasta--Ulam model, a chain of non--linea...
We investigate with numerical methods the scaling of the relaxation time to equipartion in the celeb...
The problem of a classical particle confined to bounce between two rigid walls, where one of them is...