Abstract

Many-particle effects in escapes of hard disks from a square box via a hole are discussed in a viewpoint of dynamical systems. Starting from NN disks in the box at the initial time, we calculate the probability Pn(t)P_{n}(t) for at least nn disks to remain inside the box at time tt for n=1,2,⋯ ,Nn=1,2,\cdots,N. At early times the probabilities Pn(t)P_{n}(t), n=2,3,⋯ ,N−1n=2,3,\cdots,N-1, are described by superpositions of exponential decay functions. On the other hand, after a long time the probability Pn(t)P_{n}(t) shows a power-law decay ∼t−2n\sim t^{-2n} for n≠1n\neq 1, in contrast to the fact that it decays with a different power law ∼t−n\sim t^{-n} for cases without any disk-disk collision. Chaotic or non-chaotic properties of the escape systems are discussed by the dynamics of a finite time largest Lyapunov exponent, whose decay properties are related with those of the probability Pn(t)P_{n}(t).

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