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Heavy-tailed distributions

In the engineering point of view, the self-similarity means that the traffic had similar statistical properties at a range of timescales: milliseconds, seconds, minutes, hours, even days and weeks. The merging of traffic streams, as in a statistical multiplexer, does not result in smoothing of traffic, in other words, burst data streams that are multiplexed tend to produce a bursty aggregate stream. Correspondingly, this traffic property can be described in the mathematical terms that the traffic has a long range dependence, which can be characterized that the correlation function of the traffic process is a heavy-tailed distribution.

A distribution is heavy-tailed if

\begin{displaymath}
P [X \gt x] \sim x ^{-\alpha} \end{displaymath}

as $x\rightarrow \infty$, where $0<\alpha <2$. One of the simplest heavy-tailed distributions is the Pareto distribution. The Pareto distribution is power-law over its entire range; its probability density function is given by

\begin{displaymath}
p(x) = \alpha{}k^{\alpha}x^{-\alpha-1} \end{displaymath}

where $\alpha\gt$, k>0, and $x\geq{}k$. Its distribution function has the form

\begin{displaymath}
F (x) = P [X \leq{}x] = 1-{(k/x)}^{\alpha} \end{displaymath}

The parameter k represents the smallest possible value of the random variable.

1.
if $\alpha{}\leq{}2$, the distribution has infinite variance.
2.
if $\alpha{}\leq{}1$, then the distribution has also infinite mean.

Thus, as depicted in Figure 1, with $\alpha{}$ decreases, a large portion of the probability mass is present in the tail of the distribution. In practical terms, a random variable that follows a heavy-tailed distribution can be extremely large with non negligible probability.

The strict mathematics indicates that there are self-similar process that are not long-range dependent, and vice versa. However, by the restriction $1<\alpha{}<2$ in the definition, self-similarity implies long-range dependence, and vice versa.


  
Figure 1: Pareto and Exponential Probability Density Functions
\begin{figure}


\center{
\psfig {file=figure/pareto.eps,width=8cm}
}
\end{figure}


next up previous
Next: Previous research Up: Mathematical Background Previous: Self-Similarity
Hei Xiao Jun
5/2/2001