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Multifractality of US Dollar/Deutsche Mark Exchange Rates - Studies2

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• α0 denotes the value <strong>of</strong> α for which f(α0) = 1. This is the maximum value <strong>of</strong> the multifractal<br />

spectrum. By strict concavity, α0 is unique. This is also the most frequently occurring value<br />

<strong>of</strong> α, occupying a set <strong>of</strong> Lebesgue measure one (or T if the sample span is not renormalized<br />

to a value <strong>of</strong> one.)<br />

• α1 denotes the value <strong>of</strong> α that carries most <strong>of</strong> the mass <strong>of</strong> a multifractal measure, or most<br />

<strong>of</strong> the variation <strong>of</strong> a multifractal process. Multifractal measures satisfy f(α1) =α1. The<br />

spectrum <strong>of</strong> a multifractal process generated by the MMAR thus satisfies fP (α1) =1/H.<br />

• αmin denotes the smallest manifest α, i.e. αmin =<br />

• αmax denotes the largest manifest α.<br />

<br />

<br />

min : f(α) ≥ 0 .<br />

α<br />

Each <strong>of</strong> these points is depicted in the multifractal diagram shown in Figure 8.<br />

4.4 Unifractal Examples<br />

While the Legendre transform (8) can be worked out mechanically, a graphical representation is<br />

more instructive. This is obtained by plotting, for each q, a line <strong>of</strong> slope q and vertical intercept<br />

−τ(q). Placing all <strong>of</strong> these lines upon the same graph, the lower envelope gives the estimated<br />

multifractal spectrum.<br />

For each <strong>of</strong> the Fractional Gaussian Noises in Figure 4, the simulated partition functions follow<br />

lines <strong>of</strong> approximate slope τ(q) =Hq − 1. Figure 9 shows Legendre transforms <strong>of</strong> scaling functions<br />

for FGN’s with self–affinity indices .4, .53, .6, .8. Only the left side <strong>of</strong> each spectrum is shown.<br />

The right side <strong>of</strong> the multifractal spectrum comes from negative moments <strong>of</strong> the partition function,<br />

which are not used in the empirical work in this paper. Each <strong>of</strong> the lines drawn passes through the<br />

same point at {α, f(α)} = {H, 1} . The lower envelope is thus degenerate:<br />

⎧<br />

⎪⎨ 1, α = H<br />

f(α) =<br />

⎪⎩ −∞, α = H<br />

By inspection <strong>of</strong> equation (8), this form derives from the linearity <strong>of</strong> τ(q). The multifractal spectrum<br />

is defined only for values <strong>of</strong> α that are tangency slopes for some value <strong>of</strong> the scaling function.<br />

A single valued multifractal spectrum is an alternative way <strong>of</strong> saying that each <strong>of</strong> these processes<br />

contains only a single Hölder exponent. Thus α0, which carries all <strong>of</strong> the Lebesgue measure <strong>of</strong> the<br />

17

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