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exponent, -1 - ?, the MSD scales like the MSD of the corresponding normal file, in the power of ?.
* In anomalous files of independent particles, the MSD is very slow and scales like, . Even more exciting, the particles form clusters in such files, defining a dynamical phase transition. This depends on the anomaly power ?: the percentage of particles in clusters ? follows, .
* Other generalizations include: when the particles can bypass each other with a constant probability upon encounter,

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