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The persistent current of ballistic chaotic billiards is considered with the help of the Gutzwiller trace formula. We derive the semiclassical formula of a typical persistent current $I^{typ}$ for a single billiard and an average persistent…

Mesoscale and Nanoscale Physics · Physics 2016-08-31 Shiro Kawabata

We investigate symmetry breaking in a time-dependent billiard that undergoes a continuous phase transition when dissipation is introduced. The system presents unlimited velocity, and thus energy growth for the conservative dynamics. When…

Chaotic Dynamics · Physics 2025-08-18 Anne Kétri Pasquinelli da Fonseca , Edson Denis Leonel

The emergence of power laws that govern the large-time dynamics of a one-dimensional billiard of $N$ point particles is analysed. In the initial state, the resting particles are placed in the positive half-line $x\geqslant 0$ at equal…

Statistical Mechanics · Physics 2025-06-26 T. Holovatch , Yu. Kozitsky , K. Pilorz , Yu. Holovatch

In this work, we perform a statistical study on Dirac Billiards in the extreme quantum limit (a single open channel on the leads). Our numerical analysis uses a large ensemble of random matrices and demonstrates the preponderant role of…

Mesoscale and Nanoscale Physics · Physics 2016-09-22 A. J. Nascimento Júnior , M. S. M. Barros , J. G. G. S. Ramos , A. L. R. Barbosa

We investigate the dependence of the escape rate on the position of a hole placed in uniformly hyperbolic systems admitting a finite Markov partition. We derive an exact periodic orbit formula for finite size Markov holes which differs from…

Chaotic Dynamics · Physics 2013-04-09 Orestis Georgiou , Carl P. Dettmann , Eduardo G. Altmann

We study the statistics of the experimental eigenfunctions of chaotic and disordered microwave billiards in terms of the moments of their spatial distributions, such as the Inverse Participation Ratio (IPR) and density-density…

Mesoscale and Nanoscale Physics · Physics 2009-11-07 Prabhakar Pradhan , S. Sridhar

We consider the motion of a particle subjected to the constant gravitational field and scattered inelasticaly by hard boundaries which possess the shape of parabola, wedge, and hyperbola. The billiard itself performs oscillations. The…

Chaotic Dynamics · Physics 2007-05-23 A. Z. Gorski , T. Srokowski

We present a computational scheme based on classical molecular dynamics to study chaotic billiards in static external magnetic fields. The method allows to treat arbitrary geometries and several interacting particles. We test the scheme for…

Mesoscale and Nanoscale Physics · Physics 2010-01-15 M. Aichinger , S. Janecek , E. Rasanen

We extend the application of the concept of structural invariance to bounded time independent systems. This concept, previously introduced by two of us to argue that the connection between random matrix theory and quantum systems with a…

chao-dyn · Physics 2009-10-31 F. Leyvraz , R. A. Mendez-Sanchez , T. H. Seligman

Systems of pinned billiard balls serve as simplified models of collisions, where all particles remain fixed in their positions while their (pseudo-)velocities evolve in accordance with the laws of conservation of energy and momentum. For…

We use an effective Hamiltonian to characterize particle dynamics and find escape rates in a periodically kicked Hamiltonian. We study a model of particles in storage rings that is described by a chaotic symplectic map. Ignoring the…

Statistical Mechanics · Physics 2017-07-31 Archishman Raju , Sayan Choudhury , David L. Rubin , Amie Wilkinson , James P. Sethna

There are numerous physical situations in which a hole or leak is introduced in an otherwise closed chaotic system. The leak can have a natural origin, it can mimic measurement devices, and it can also be used to reveal dynamical properties…

Chaotic Dynamics · Physics 2013-06-07 Eduardo G. Altmann , Jefferson S. E. Portela , Tamás Tél

A "drivebelt" stadium billiard with boundary consisting of circular arcs of differing radius connected by their common tangents shares many properties with the conventional "straight" stadium, including hyperbolicity and mixing, as well as…

Chaotic Dynamics · Physics 2015-06-03 Carl P. Dettmann , Orestis Georgiou

In order to simulate observational and experimental situations, we consider a leak in the phase space of a chaotic dynamical system. We obtain an expression for the escape rate of the survival probability applying the theory of transient…

Chaotic Dynamics · Physics 2009-02-02 Eduardo G. Altmann , Tamas Tel

The changeover from normal to super diffusion in time dependent billiards is explained analytically. The unlimited energy growth for an ensemble of bouncing particles in time dependent billiards is obtained by means of a two dimensional…

Chaotic Dynamics · Physics 2018-06-13 Matheus Hansen , David Ciro , Iberê L. Caldas , Edson D. Leonel

In this paper, we define a variant of billiards in which the ball bounces around a square grid erasing walls as it goes. We prove that there exist periodic tunnels with arbitrarily large period from any possible starting point, that there…

Dynamical Systems · Mathematics 2016-01-26 Edward Newkirk

We prove some partial results on the periodicity of billiard systems on graphs. The results specialize to the case of $n$ billiards with equal mass on the unit interval or circle traveling at the same speed.

Dynamical Systems · Mathematics 2013-12-11 Stephen Michael Miller , Thomas Silverman

We describe conditions under which higher-dimensional billiard models in bounded, convex regions are fully chaotic, generalizing the Bunimovich stadium to dimensions above two. An example is a three-dimensional stadium bounded by a cylinder…

Chaotic Dynamics · Physics 2013-02-07 Thomas Gilbert , David P. Sanders

We study a particle moving at unit speed in a self-similar Lorentz billiard channel; the latter consists of an infinite sequence of cells which are identical in shape but growing exponentially in size, from left to right. We present…

Chaotic Dynamics · Physics 2009-08-29 Felipe Barra , Nikolai Chernov , Thomas Gilbert

We report a dynamical phase transition from integrability to non-integrability in a simple oval-like billiard with boundary $R(\theta)=1+\epsilon\cos(p\theta)$. For $\epsilon=0$, the phase space is {\it foliated} by invariant curves…

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