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Kurtosis

Fourth standardized moment in statistics

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The standard measure of a distribution's kurtosis, originating with Karl Pearson, is a scaled version of the fourth moment of the distribution. This number is related to the tails of the distribution, not its peak; hence, the sometimes-seen characterization of kurtosis as peakedness is incorrect. For this measure, higher kurtosis corresponds to greater extremity of deviations (or outliers), and not the configuration of data near the mean. The widespread misunderstanding of kurtosis may derive from Pearson's own description of kurtosis, as quoted by Westfall, as a departure from normality, a : 'degree of flat-toppedness which is greater or less than that of the normal curve'.

Excess kurtosis, typically compared to a value of 0, characterizes the tailedness of a distribution. A univariate normal distribution has an excess kurtosis of 0. Negative excess kurtosis indicates a platykurtic distribution, which does not necessarily have a flat top but produces fewer or less extreme outliers than the normal distribution. For instance, the uniform distribution (i.e., one that is uniformly finite over some bound and zero elsewhere) is platykurtic. On the other hand, positive excess kurtosis signifies a leptokurtic distribution. The Laplace distribution for example, has tails that decay more slowly than a normal one, resulting in more outliers. To simplify comparison with the normal distribution, excess kurtosis is calculated as Pearson's kurtosis minus 3. Some authors and software packages use kurtosis to refer specifically to excess kurtosis, but this article distinguishes between the two for clarity.

Alternative measures of kurtosis are: the L-kurtosis, which is a scaled version of the fourth L-moment; measures based on four population or sample quantiles. These are analogous to the alternative measures of skewness that are not based on ordinary moments.

Pearson moments

The kurtosis is the fourth standardized moment, defined as Kurt⁡[X]:=μ~4≡μ4σ4=E⁡[(X−μσ)4]=E⁡[(X−μ)4](E⁡[(X−μ)2])2

where μ4 is the fourth central moment and σ is the standard deviation. Several letters are used in the literature to denote the kurtosis. A very common choice is κ, which is fine as long as it is clear that it does not refer to a cumulant. Other choices include γ2, to be similar to the notation for skewness, although sometimes this is instead reserved for the excess kurtosis. Pearson is systematically using β2.

The kurtosis is bounded below by the squared skewness plus 1: μ4σ4≥(μ3σ3)2+1, where μ3 is the third central moment. The lower bound is realized by the Bernoulli distribution. There is no upper limit to the kurtosis of a general probability distribution, and it may be infinite.

A reason why some authors favor the excess kurtosis is that cumulants are extensive. Formulas related to the extensive property are more naturally expressed in terms of the excess kurtosis. For example, let X1, ..., Xn be independent random variables for which the fourth moment exists, and let Y be the random variable defined by the sum of the Xi. The excess kurtosis of Y isKurt⁡[Y]−3=∑i=1nσi4⋅(Kurt⁡[Xi]−3)(∑j=1nσj2)2,where σi is the standard deviation of Xi. In particular if all of the Xi have the same variance, then this simplifies toKurt⁡[Y]−3=1n2∑i=1n(Kurt⁡[Xi]−3).

The reason not to subtract 3 is that the bare moment better generalizes to multivariate distributions, especially when independence is not assumed. The cokurtosis between pairs of variables is an order four tensor. For a bivariate normal distribution, the cokurtosis tensor has off-diagonal terms that are neither 0 nor 3 in general, so attempting to "correct" for an excess becomes confusing. It is true, however, that the joint cumulants of degree greater than two for any multivariate normal distribution are zero.

For two random variables, X and Y, not necessarily independent, the kurtosis of the sum, X + Y, is Kurt⁡[X+Y]=1σX+Y4(σX4Kurt⁡[X]+4σX3σYCokurt⁡[X,X,X,Y]+6σX2σY2Cokurt⁡[X,X,Y,Y]+4σXσY3Cokurt⁡[X,Y,Y,Y]+σY4Kurt⁡[Y]). Note that the fourth-power binomial coefficients (1, 4, 6, 4, 1) appear in the above equation.

Interpretation

The interpretation of the Pearson measure of kurtosis (or excess kurtosis) was once debated, but it is now well-established. As noted by Westfall in 2014, "... its unambiguous interpretation relates to tail extremity". Specifically, it reflects either the presence of existing outliers (for sample kurtosis) or the tendency to produce outliers (for the kurtosis of a probability distribution). The underlying logic is straightforward: kurtosis represents the average (or expected value) of standardized data raised to the fourth power. Standardized values less than 1—corresponding to data within one standard deviation of the mean (where the peak occurs)—contribute minimally to kurtosis. This is because raising a number less than 1 to the fourth power brings it closer to zero. The meaningful contributors to kurtosis are data values outside the peak region, i.e., the outliers. Therefore, kurtosis primarily measures outliers and provides no information about the central peak.

Numerous misconceptions about kurtosis relate to notions of peakedness. One such misconception is that kurtosis measures both the peakedness of a distribution and the heaviness of its tail. Other incorrect interpretations include notions like lack of shoulders (where the shoulder refers vaguely to the area between the peak and the tail, or more specifically, the region about one standard deviation from the mean) or bimodality. Balanda and MacGillivray argue that the standard definition of kurtosis "poorly captures the kurtosis, peakedness, or tail weight of a distribution." Instead, they propose a vague definition of kurtosis as the location- and scale-free movement of probability mass from the distribution's shoulders into its center and tails.

Moors' interpretation

In 1986, Moors gave an interpretation of kurtosis. Let Z=X−μσ, where X is a random variable, μ is the mean and σ is the standard deviation.

Now by definition of the kurtosis κ, and by the well-known identity E⁡[V2]=var⁡[V]+E⁡[V]2, κ=E⁡[Z4]=var⁡[Z2]+E⁡[Z2]2=var⁡[Z2]+var⁡[Z]2=var⁡[Z2]+1.

The kurtosis can now be seen as a measure of the dispersion of Z2 around its expectation. Alternatively it can be seen to be a measure of the dispersion of Z around +1 and −1. κ attains its minimal value in a symmetric two-point distribution. In terms of the original variable X, the kurtosis is a measure of the dispersion of X around the two values μ ± σ.

High values of κ arise where the probability mass is concentrated around the mean and the data-generating process produces occasional values far from the mean, or where the probability mass is concentrated in the tails of the distribution.

Maximal entropy

The entropy of a distribution is −∫p(x)ln⁡p(x)dx.

For any μ∈Rn,Σ∈Rn×n with Σ positive definite, among all probability distributions on Rn with mean μ and covariance Σ, the normal distribution N(μ,Σ) has the largest entropy.

Since mean μ and covariance Σ are the first two moments, it is natural to consider extension to higher moments. In fact, by Lagrange multiplier method, for any prescribed first n moments, if there exists some probability distribution of form p(x)∝e∑iaixi+∑ijbijxixj+⋯+∑i1⋯inxi1⋯xin that has the prescribed moments (if it is feasible), then it is the maximal entropy distribution under the given constraints.

By serial expansion, ∫12πe−12x2−14gx4x2ndx=12π∫e−12x2−14gx4x2ndx=∑k1k!(−g4)k(2n+4k−1)!!=(2n−1)!!−14g(2n+3)!!+O(g2) so if a random variable has probability distribution p(x)=e−12x2−14gx4/Z, where Z is a normalization constant, then its kurtosis is 3−6g+O(g2).

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