Abstract
the SA by high-dimensional noise for values of r comparable with the variance of this noise, "breaks" should be observed on the curves in Figs. 4a and b. For r less than the coordinates of these breaks, the slope of in C(r)(m) equals the dimension of the imbedded phase space, i.e., m. Of course, if the intensity of the technical noise is so high that the fractal structure of the SA is "smeared" completely, then the curves of in C(r)(m). versus In do r not have a section with equal slope, and therefore such noise dominates in the laser radiation.
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