1997
DOI: 10.1103/physreve.55.r6319
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Dynamics of two interacting particles in classical billiards

Abstract: The problem of two interacting particles moving in a ddimensional billiard is considered here. A suitable coordinate transformation leads to the problem of a particle in an unconventional hyperbilliard. A dynamical map can be readily constructed for this general system, which greatly simplifies calculations. As a particular example, we consider two identical particles interacting through a screened Coulomb potential in a one-dimensional billiard. We find that the screening plays an important role in the dynami… Show more

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Cited by 19 publications
(12 citation statements)
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“…A Yukawa interaction between particles is assumed. Such a system has been considered classically [6] and quantum mechanically [7] for the case of equal masses. In order to calculate the spectrum of Lyapunov Exponents (LEs), the dynamics in tangent space is determined explicitly.…”
Section: Introductionmentioning
confidence: 99%
“…A Yukawa interaction between particles is assumed. Such a system has been considered classically [6] and quantum mechanically [7] for the case of equal masses. In order to calculate the spectrum of Lyapunov Exponents (LEs), the dynamics in tangent space is determined explicitly.…”
Section: Introductionmentioning
confidence: 99%
“…Electron transport experiments performed on semiconductor quantum dots in the Coulomb blockade (CB) regime [4] provide a further possibility to check RMT predictions. The classical motion of electrons in these structures can be assumed to be chaotic due to an irregular potential landscape produced by impurities, an asymmetric confinement potential [5], and/or electron-electron interactions [6]. The transport properties of quantum dots are inherently related to their energy spectra and electronic wavefunctions and thus the connection with RMT is readily made [5,7].…”
mentioning
confidence: 99%
“…As perhaps one of the simplest examples (see Ref. [16] for a description of the general case), consider two particles of equal masses moving in a 1D box defined in the interval q : (− 1 2 , 1 2 ) (we measure all lengths in terms of the box size). The particles are assumed to interact via a screened potential V (q 1 , q 2 ) = exp(−λ|q 1 − q 2 |)/|q 1 − q 2 | , where λ is the inverse screening length.…”
Section: A Classical Dotmentioning
confidence: 99%