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Short description: Fourth standardized moment in statistics

In probability theory and statistics, kurtosis (from Greek: κυρτός, kyrtos or kurtos, meaning "curved, arching") is a measure of the "tailedness" of the probability distribution of a real-valued random variable. Like skewness, kurtosis describes a particular aspect of a probability distribution. There are different ways to quantify kurtosis for a theoretical distribution, and there are corresponding ways of estimating it using a sample from a population. Different measures of kurtosis may have different interpretations.

The standard measure of a distribution's kurtosis, originating with Karl Pearson,[1] is a scaled version of the fourth moment of the distribution. This number is related to the tails of the distribution, not its peak;[2] 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.

It is common to compare the excess kurtosis (defined below) of a distribution to 0. This value 0 is the excess kurtosis of any univariate normal distribution. Distributions with negative excess kurtosis are said to be platykurtic, although this does not imply the distribution is "flat-topped" as is sometimes stated. Rather, it means the distribution produces fewer and/or less extreme outliers than the normal distribution. An example of a platykurtic distribution is the uniform distribution, which does not produce outliers. Distributions with a positive excess kurtosis are said to be leptokurtic. An example of a leptokurtic distribution is the Laplace distribution, which has tails that asymptotically approach zero more slowly than a Gaussian, and therefore produces more outliers than the normal distribution. It is common practice to use excess kurtosis, which is defined as Pearson's kurtosis minus 3, to provide a simple comparison to the normal distribution. Some authors and software packages use "kurtosis" by itself to refer to the excess kurtosis. For clarity and generality, however, this article explicitly indicates where non-excess kurtosis is meant.

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.[3] These are analogous to the alternative measures of skewness that are not based on ordinary moments.[3]

Pearson moments

The kurtosis is the fourth standardized moment, defined as

[math]\displaystyle{ \operatorname{Kurt}[X] = \operatorname{E}\left[\left(\frac{X - \mu}{\sigma}\right)^4\right] = \frac{\operatorname{E}\left[(X - \mu)^4\right]}{\left(\operatorname{E}\left[(X - \mu)^2\right]\right)^2} = \frac{\mu_4}{\sigma^4}, }[/math]

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.

The kurtosis is bounded below by the squared skewness plus 1:[4]:432

[math]\displaystyle{ \frac{\mu_4}{\sigma^4} \geq \left(\frac{\mu_3}{\sigma^3}\right)^2 + 1, }[/math]

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 is

[math]\displaystyle{ \operatorname{Kurt}[Y] - 3 = \frac{1}{\left( \sum_{j=1}^n \sigma_j^{\,2}\right)^2} \sum_{i=1}^n \sigma_i^{\,4} \cdot \left(\operatorname{Kurt}\left[X_i\right] - 3\right), }[/math]

where [math]\displaystyle{ \sigma_i }[/math] is the standard deviation of [math]\displaystyle{ X_i }[/math]. In particular if all of the Xi have the same variance, then this simplifies to

[math]\displaystyle{ \operatorname{Kurt}[Y] - 3 = {1 \over n^2} \sum_{i=1}^n \left(\operatorname{Kurt}\left[X_i\right] - 3\right). }[/math]

The reason not to subtract 3 is that the bare fourth 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

[math]\displaystyle{ \begin{align} \operatorname{Kurt}[X+Y] = {1 \over \sigma_{X+Y}^4} \big( & \sigma_X^4\operatorname{Kurt}[X] + 4\sigma_X^3\sigma_Y\operatorname{Cokurt}[X,X,X,Y] \\ & {} + 6\sigma_X^2\sigma_Y^2\operatorname{Cokurt}[X,X,Y,Y] \\[6pt] & {} + 4\sigma_X\sigma_Y^3\operatorname{Cokurt}[X,Y,Y,Y] + \sigma_Y^4\operatorname{Kurt}[Y] \big). \end{align} }[/math]

Note that the fourth-power binomial coefficients (1, 4, 6, 4, 1) appear in the above equation.


The exact interpretation of the Pearson measure of kurtosis (or excess kurtosis) used to be disputed, but is now settled. As Westfall notes in 2014[2], "...its only unambiguous interpretation is in terms of tail extremity; i.e., either existing outliers (for the sample kurtosis) or propensity to produce outliers (for the kurtosis of a probability distribution)." The logic is simple: Kurtosis is the average (or expected value) of the standardized data raised to the fourth power. Standardized values that are less than 1 (i.e., data within one standard deviation of the mean, where the "peak" would be) contribute virtually nothing to kurtosis, since raising a number that is less than 1 to the fourth power makes it closer to zero. The only data values (observed or observable) that contribute to kurtosis in any meaningful way are those outside the region of the peak; i.e., the outliers. Therefore, kurtosis measures outliers only; it measures nothing about the "peak".

Many incorrect interpretations of kurtosis that involve notions of peakedness have been given. One is that kurtosis measures both the "peakedness" of the distribution and the heaviness of its tail.[5] Various other incorrect interpretations have been suggested, such as "lack of shoulders" (where the "shoulder" is defined vaguely as the area between the peak and the tail, or more specifically as the area about one standard deviation from the mean) or "bimodality".[6] Balanda and MacGillivray assert that the standard definition of kurtosis "is a poor measure of the kurtosis, peakedness, or tail weight of a distribution"[5]:114 and instead propose to "define kurtosis vaguely as the location- and scale-free movement of probability mass from the shoulders of a distribution into its center and tails".[5]

Moors' interpretation

In 1986 Moors gave an interpretation of kurtosis.[7] Let

[math]\displaystyle{ Z = \frac{ X - \mu } \sigma, }[/math]

where X is a random variable, μ is the mean and σ is the standard deviation.

Now by definition of the kurtosis [math]\displaystyle{ \kappa }[/math], and by the well-known identity [math]\displaystyle{ E\left[V^2\right] = \operatorname{var}[V] + [E[V]]^2, }[/math]

[math]\displaystyle{ \kappa = E\left[ Z^4 \right] = \operatorname{var}\left[ Z^2 \right] + \left[E\left[Z^2\right]\right]^2 = \operatorname{var}\left[ Z^2 \right] + [\operatorname{var}[Z]]^2 = \operatorname{var}\left[ Z^2 \right] + 1. }[/math]

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 in two circumstances:

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

Maximal entropy

The entropy of a distribution is [math]\displaystyle{ \int p(x) \ln p(x) \, dx }[/math].

For any [math]\displaystyle{ \mu \in \R^n, \Sigma \in \R^{n\times n} }[/math] with [math]\displaystyle{ \Sigma }[/math] positive definite, among all probability distributions on [math]\displaystyle{ \R^n }[/math] with mean [math]\displaystyle{ \mu }[/math] and covariance [math]\displaystyle{ \Sigma }[/math], the normal distribution [math]\displaystyle{ \mathcal N(\mu, \Sigma) }[/math] has the largest entropy.

Since mean [math]\displaystyle{ \mu }[/math] and covariance [math]\displaystyle{ \Sigma }[/math] 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 [math]\displaystyle{ p(x) \propto e^{\sum_i a_i x_i + \sum_{ij}b_{ij}x_ix_j + \cdots + \sum_{i_1\cdots i_n} x_{i_1}\cdots x_{i_n}} }[/math] that has the prescribed moments (if it is feasible), then it is the maximal entropy distribution under the given constraints.[8][9]

By serial expansion, [math]\displaystyle{ \int \frac{1}{\sqrt{2\pi}} e^{-\frac 12 x^2 - \frac 14 gx^4} x^{2n} \, dx = \frac{1}{\sqrt{2\pi}} \int e^{-\frac 12 x^2 - \frac 14 gx^4} x^{2n} \, dx = \sum_k \frac{1}{k!} (-g/4)^k (2n+4k-1)!! = (2n-1)!! - \frac 14 g (2n+3)!! + O(g^2) }[/math]so if a random variable has probability distribution [math]\displaystyle{ p(x) = e^{-\frac 12 x^2 - \frac 14 gx^4}/Z }[/math], where [math]\displaystyle{ Z }[/math] is a normalization constant, then its kurtosis is [math]\displaystyle{ 3 - 6g + O(g^2) }[/math].[10]

Excess kurtosis

The excess kurtosis is defined as kurtosis minus 3. There are 3 distinct regimes as described below.


Distributions with zero excess kurtosis are called mesokurtic, or mesokurtotic. The most prominent example of a mesokurtic distribution is the normal distribution family, regardless of the values of its parameters. A few other well-known distributions can be mesokurtic, depending on parameter values: for example, the binomial distribution is mesokurtic for [math]\displaystyle{ p = 1/2 \pm \sqrt{1/12} }[/math].


A distribution with positive excess kurtosis is called leptokurtic, or leptokurtotic. "Lepto-" means "slender".[11] In terms of shape, a leptokurtic distribution has fatter tails. Examples of leptokurtic distributions include the Student's t-distribution, Rayleigh distribution, Laplace distribution, exponential distribution, Poisson distribution and the logistic distribution. Such distributions are sometimes termed super-Gaussian.[12]


The coin toss is the most platykurtic distribution

A distribution with negative excess kurtosis is called platykurtic, or platykurtotic. "Platy-" means "broad".[13] In terms of shape, a platykurtic distribution has thinner tails. Examples of platykurtic distributions include the continuous and discrete uniform distributions, and the raised cosine distribution. The most platykurtic distribution of all is the Bernoulli distribution with p = 1/2 (for example the number of times one obtains "heads" when flipping a coin once, a coin toss), for which the excess kurtosis is −2.

Graphical examples

The Pearson type VII family

pdf for the Pearson type VII distribution with excess kurtosis of infinity (red); 2 (blue); and 0 (black)
log-pdf for the Pearson type VII distribution with excess kurtosis of infinity (red); 2 (blue); 1, 1/2, 1/4, 1/8, and 1/16 (gray); and 0 (black)

The effects of kurtosis are illustrated using a parametric family of distributions whose kurtosis can be adjusted while their lower-order moments and cumulants remain constant. Consider the Pearson type VII family, which is a special case of the Pearson type IV family restricted to symmetric densities. The probability density function is given by

[math]\displaystyle{ f(x; a, m) = \frac{\Gamma(m)}{a\,\sqrt{\pi}\,\Gamma(m-1/2)} \left[1+\left(\frac{x}{a}\right)^2 \right]^{-m}, \! }[/math]

where a is a scale parameter and m is a shape parameter.

All densities in this family are symmetric. The kth moment exists provided m > (k + 1)/2. For the kurtosis to exist, we require m > 5/2. Then the mean and skewness exist and are both identically zero. Setting a2 = 2m − 3 makes the variance equal to unity. Then the only free parameter is m, which controls the fourth moment (and cumulant) and hence the kurtosis. One can reparameterize with [math]\displaystyle{ m = 5/2 + 3/\gamma_2 }[/math], where [math]\displaystyle{ \gamma_2 }[/math] is the excess kurtosis as defined above. This yields a one-parameter leptokurtic family with zero mean, unit variance, zero skewness, and arbitrary non-negative excess kurtosis. The reparameterized density is

[math]\displaystyle{ g(x; \gamma_2) = f\left(x;\; a = \sqrt{2 + \frac{6}{\gamma_2}},\; m = \frac{5}{2} + \frac{3}{\gamma_2}\right). \! }[/math]

In the limit as [math]\displaystyle{ \gamma_2 \to \infty }[/math] one obtains the density

[math]\displaystyle{ g(x) = 3\left(2 + x^2\right)^{-\frac{5}{2}}, \! }[/math]

which is shown as the red curve in the images on the right.

In the other direction as [math]\displaystyle{ \gamma_2 \to 0 }[/math] one obtains the standard normal density as the limiting distribution, shown as the black curve.

In the images on the right, the blue curve represents the density [math]\displaystyle{ x \mapsto g(x; 2) }[/math] with excess kurtosis of 2. The top image shows that leptokurtic densities in this family have a higher peak than the mesokurtic normal density, although this conclusion is only valid for this select family of distributions. The comparatively fatter tails of the leptokurtic densities are illustrated in the second image, which plots the natural logarithm of the Pearson type VII densities: the black curve is the logarithm of the standard normal density, which is a parabola. One can see that the normal density allocates little probability mass to the regions far from the mean ("has thin tails"), compared with the blue curve of the leptokurtic Pearson type VII density with excess kurtosis of 2. Between the blue curve and the black are other Pearson type VII densities with γ2 = 1, 1/2, 1/4, 1/8, and 1/16. The red curve again shows the upper limit of the Pearson type VII family, with [math]\displaystyle{ \gamma_2 = \infty }[/math] (which, strictly speaking, means that the fourth moment does not exist). The red curve decreases the slowest as one moves outward from the origin ("has fat tails").

Other well-known distributions

Probability density functions for selected distributions with mean 0, variance 1 and different excess kurtosis
Logarithms of probability density functions for selected distributions with mean 0, variance 1 and different excess kurtosis

Several well-known, unimodal, and symmetric distributions from different parametric families are compared here. Each has a mean and skewness of zero. The parameters have been chosen to result in a variance equal to 1 in each case. The images on the right show curves for the following seven densities, on a linear scale and logarithmic scale:

Note that in these cases the platykurtic densities have bounded support, whereas the densities with positive or zero excess kurtosis are supported on the whole real line.

One cannot infer that high or low kurtosis distributions have the characteristics indicated by these examples. There exist platykurtic densities with infinite support,

  • e.g., exponential power distributions with sufficiently large shape parameter b

and there exist leptokurtic densities with finite support.

  • e.g., a distribution that is uniform between −3 and −0.3, between −0.3 and 0.3, and between 0.3 and 3, with the same density in the (−3, −0.3) and (0.3, 3) intervals, but with 20 times more density in the (−0.3, 0.3) interval

Also, there exist platykurtic densities with infinite peakedness,

  • e.g., an equal mixture of the beta distribution with parameters 0.5 and 1 with its reflection about 0.0

and there exist leptokurtic densities that appear flat-topped,

  • e.g., a mixture of distribution that is uniform between −1 and 1 with a T(4.0000001) Student's t-distribution, with mixing probabilities 0.999 and 0.001.

Sample kurtosis


A natural but biased estimator

For a sample of n values, a method of moments estimator of the population excess kurtosis can be defined as

[math]\displaystyle{ g_2 = \frac{m_4}{m_2^2} -3 = \frac{\tfrac{1}{n} \sum_{i=1}^n (x_i - \overline{x})^4}{\left[\tfrac{1}{n} \sum_{i=1}^n (x_i - \overline{x})^2\right]^2} - 3 }[/math]

where m4 is the fourth sample moment about the mean, m2 is the second sample moment about the mean (that is, the sample variance), xi is the ith value, and [math]\displaystyle{ \overline{x} }[/math] is the sample mean.

This formula has the simpler representation,

[math]\displaystyle{ g_2 = \frac{1}{n} \sum_{i=1}^n z_i^4 - 3 }[/math]

where the [math]\displaystyle{ z_i }[/math] values are the standardized data values using the standard deviation defined using n rather than n − 1 in the denominator.

For example, suppose the data values are 0, 3, 4, 1, 2, 3, 0, 2, 1, 3, 2, 0, 2, 2, 3, 2, 5, 2, 3, 999.

Then the [math]\displaystyle{ z_i }[/math] values are −0.239, −0.225, −0.221, −0.234, −0.230, −0.225, −0.239, −0.230, −0.234, −0.225, −0.230, −0.239, −0.230, −0.230, −0.225, −0.230, −0.216, −0.230, −0.225, 4.359

and the [math]\displaystyle{ z_i^4 }[/math] values are 0.003, 0.003, 0.002, 0.003, 0.003, 0.003, 0.003, 0.003, 0.003, 0.003, 0.003, 0.003, 0.003, 0.003, 0.003, 0.003, 0.002, 0.003, 0.003, 360.976.

The average of these values is 18.05 and the excess kurtosis is thus 18.05 − 3 = 15.05. This example makes it clear that data near the "middle" or "peak" of the distribution do not contribute to the kurtosis statistic, hence kurtosis does not measure "peakedness". It is simply a measure of the outlier, 999 in this example.

Standard unbiased estimator

Given a sub-set of samples from a population, the sample excess kurtosis [math]\displaystyle{ g_2 }[/math] above is a biased estimator of the population excess kurtosis. An alternative estimator of the population excess kurtosis, which is unbiased in random samples of a normal distribution, is defined as follows:[3]

[math]\displaystyle{ \begin{align} G_2 & = \frac{k_4}{k_2^2} \\[6pt] & = \frac{n^2\,[(n+1)\,m_4 - 3\,(n-1)\,m_{2}^2]}{(n-1)\,(n-2)\,(n-3)} \; \frac{(n-1)^2}{n^2\,m_2^2} \\[6pt] & = \frac{n-1}{(n-2)\,(n-3)} \left[(n+1)\,\frac{m_4}{m_{2}^2} - 3\,(n-1) \right] \\[6pt] & = \frac{n-1}{(n-2)\,(n-3)} \left[(n+1)\,g_2 + 6 \right] \\[6pt] & = \frac{(n+1)\,n\,(n-1)}{(n-2)\,(n-3)} \; \frac{\sum_{i=1}^n (x_i - \bar{x})^4}{\left(\sum_{i=1}^n (x_i - \bar{x})^2\right)^2} - 3\,\frac{(n-1)^2}{(n-2)\,(n-3)} \\[6pt] & = \frac{(n+1)\,n}{(n-1)\,(n-2)\,(n-3)} \; \frac{\sum_{i=1}^n (x_i - \bar{x})^4}{k_2^2} - 3\,\frac{(n-1)^2}{(n-2) (n-3)} \end{align} }[/math]

where k4 is the unique symmetric unbiased estimator of the fourth cumulant, k2 is the unbiased estimate of the second cumulant (identical to the unbiased estimate of the sample variance), m4 is the fourth sample moment about the mean, m2 is the second sample moment about the mean, xi is the ith value, and [math]\displaystyle{ \bar{x} }[/math] is the sample mean. This adjusted Fisher–Pearson standardized moment coefficient [math]\displaystyle{ G_2 }[/math] is the version found in Excel and several statistical packages including Minitab, SAS, and SPSS.[14]

Unfortunately, in nonnormal samples [math]\displaystyle{ G_2 }[/math] is itself generally biased.

Upper bound

An upper bound for the sample kurtosis of n (n > 2) real numbers is[15]

[math]\displaystyle{ g_2 \le \frac{1}{2} \frac{n-3}{n-2} g_1^2 + \frac{n}{2} - 3. }[/math]

where [math]\displaystyle{ g_1=m_3/m_2^{3/2} }[/math] is the corresponding sample skewness.

Variance under normality

The variance of the sample kurtosis of a sample of size n from the normal distribution is[16]

[math]\displaystyle{ \operatorname{var}(g_2) = \frac{24n(n-1)^2}{(n-3)(n-2)(n+3)(n+5)} }[/math]

Stated differently, under the assumption that the underlying random variable [math]\displaystyle{ X }[/math] is normally distributed, it can be shown that [math]\displaystyle{ \sqrt{n} g_2 \,\xrightarrow{d}\, \mathcal{N}(0, 24) }[/math].[17]:Page number needed


The sample kurtosis is a useful measure of whether there is a problem with outliers in a data set. Larger kurtosis indicates a more serious outlier problem, and may lead the researcher to choose alternative statistical methods.

D'Agostino's K-squared test is a goodness-of-fit normality test based on a combination of the sample skewness and sample kurtosis, as is the Jarque–Bera test for normality.

For non-normal samples, the variance of the sample variance depends on the kurtosis; for details, please see variance.

Pearson's definition of kurtosis is used as an indicator of intermittency in turbulence.[18] It is also used in magnetic resonance imaging to quantify non-Gaussian diffusion.[19]

A concrete example is the following lemma by He, Zhang, and Zhang:[20] Assume a random variable [math]\displaystyle{ X }[/math] has expectation [math]\displaystyle{ E[X] = \mu }[/math], variance [math]\displaystyle{ E\left[(X - \mu)^2\right] = \sigma^2 }[/math] and kurtosis [math]\displaystyle{ \kappa = \tfrac{1}{\sigma^4}E\left[(X - \mu)^4\right]. }[/math] Assume we sample [math]\displaystyle{ n = \tfrac{2\sqrt{3} + 3}{3}\kappa\log\tfrac{1}{\delta} }[/math] many independent copies. Then

[math]\displaystyle{ \Pr\left[\max_{i=1}^n X_i \le \mu\right] \le \delta \quad\text{and}\quad \Pr\left[\min_{i=1}^n X_i \ge \mu\right] \le \delta. }[/math]

This shows that with [math]\displaystyle{ \Theta(\kappa\log\tfrac{1}\delta) }[/math] many samples, we will see one that is above the expectation with probability at least [math]\displaystyle{ 1-\delta }[/math]. In other words: If the kurtosis is large, we might see a lot values either all below or above the mean.

Kurtosis convergence

Applying band-pass filters to digital images, kurtosis values tend to be uniform, independent of the range of the filter. This behavior, termed kurtosis convergence, can be used to detect image splicing in forensic analysis.[21]

Other measures

A different measure of "kurtosis" is provided by using L-moments instead of the ordinary moments.[22][23]

See also


  1. Pearson, Karl (1905), "Das Fehlergesetz und seine Verallgemeinerungen durch Fechner und Pearson. A Rejoinder" (in en), Biometrika 4 (1–2): 169–212, doi:10.1093/biomet/4.1-2.169 
  2. 2.0 2.1 Westfall, Peter H. (2014), "Kurtosis as Peakedness, 1905 - 2014. R.I.P.", The American Statistician 68 (3): 191–195, doi:10.1080/00031305.2014.917055, PMID 25678714 
  3. 3.0 3.1 3.2 Joanes, Derrick N.; Gill, Christine A. (1998), "Comparing measures of sample skewness and kurtosis", Journal of the Royal Statistical Society, Series D 47 (1): 183–189, doi:10.1111/1467-9884.00122 
  4. Pearson, Karl (1916), "Mathematical Contributions to the Theory of Evolution. — XIX. Second Supplement to a Memoir on Skew Variation.", Philosophical Transactions of the Royal Society of London A 216 (546): 429–457, doi:10.1098/rsta.1916.0009, Bibcode1916RSPTA.216..429P 
  5. 5.0 5.1 5.2 Balanda, Kevin P. (1988), "Kurtosis: A Critical Review", The American Statistician 42 (2): 111–119, doi:10.2307/2684482 
  6. Darlington, Richard B. (1970), "Is Kurtosis Really 'Peakedness'?", The American Statistician 24 (2): 19–22, doi:10.1080/00031305.1970.10478885 
  7. Moors, J. J. A. (1986), "The meaning of kurtosis: Darlington reexamined", The American Statistician 40 (4): 283–284, doi:10.1080/00031305.1986.10475415 
  8. Tagliani, A. (1990-12-01). "On the existence of maximum entropy distributions with four and more assigned moments". Probabilistic Engineering Mechanics 5 (4): 167–170. doi:10.1016/0266-8920(90)90017-E. ISSN 0266-8920. https://dx.doi.org/10.1016/0266-8920%2890%2990017-E. 
  9. Rockinger, Michael; Jondeau, Eric (2002-01-01). "Entropy densities with an application to autoregressive conditional skewness and kurtosis". Journal of Econometrics 106 (1): 119–142. doi:10.1016/S0304-4076(01)00092-6. ISSN 0304-4076. https://www.sciencedirect.com/science/article/pii/S0304407601000926. 
  10. Bradde, Serena; Bialek, William (2017-05-01). "PCA Meets RG" (in en). Journal of Statistical Physics 167 (3): 462–475. doi:10.1007/s10955-017-1770-6. ISSN 1572-9613. PMID 30034029. PMC 6054449. Bibcode2017JSP...167..462B. https://doi.org/10.1007/s10955-017-1770-6. 
  11. "Lepto-". http://medical-dictionary.thefreedictionary.com/lepto-. 
  12. Benveniste, Albert; Goursat, Maurice; Ruget, Gabriel (1980), "Robust identification of a nonminimum phase system: Blind adjustment of a linear equalizer in data communications", IEEE Transactions on Automatic Control 25 (3): 385–399, doi:10.1109/tac.1980.1102343 
  13. "platy-: definition, usage and pronunciation - YourDictionary.com". http://www.yourdictionary.com/platy-prefix. 
  14. Doane DP, Seward LE (2011) J Stat Educ 19 (2)
  15. Sharma, Rajesh; Bhandari, Rajeev K. (2015), "Skewness, kurtosis and Newton's inequality", Rocky Mountain Journal of Mathematics 45 (5): 1639–1643, doi:10.1216/RMJ-2015-45-5-1639, http://projecteuclid.org/euclid.rmjm/1453817258 
  16. "The Moments of the Distribution for Normal Samples of Measures of Departure from Normality", Proceedings of the Royal Society A 130 (812): 16–28, 1930, doi:10.1098/rspa.1930.0185, Bibcode1930RSPSA.130...16F 
  17. Kendall, Maurice G.; Stuart, Alan (1969), The Advanced Theory of Statistics, Volume 1: Distribution Theory (3rd ed.), London, UK: Charles Griffin & Company Limited, ISBN 0-85264-141-9, https://archive.org/details/advancedtheoryof0001kend 
  18. Sandborn, Virgil A. (1959), "Measurements of Intermittency of Turbulent Motion in a Boundary Layer", Journal of Fluid Mechanics 6 (2): 221–240, doi:10.1017/S0022112059000581, Bibcode1959JFM.....6..221S 
  19. Jensen, J.; Helpern, J.; Ramani, A.; Lu, H.; Kaczynski, K. (19 May 2005). "Diffusional kurtosis imaging: The quantification of non-Gaussian water diffusion by means of magnetic resonance imaging". Magn Reson Med 53 (6): 1432–1440. doi:10.1002/mrm.20508. PMID 15906300. https://onlinelibrary.wiley.com/doi/full/10.1002/mrm.20508. 
  20. He, Simai; Zhang, Jiawei; Zhang, Shuzhong (2010). "Bounding probability of small deviation: A fourth moment approach". Mathematics of Operations Research 35 (1): 208–232. doi:10.1287/moor.1090.0438. 
  21. Pan, Xunyu; Zhang, Xing; Lyu, Siwei (2012), "Exposing Image Splicing with Inconsistent Local Noise Variances", 2012 IEEE International Conference on Computational Photography (ICCP), 28-29 April 2012; Seattle, WA, USA: IEEE, doi:10.1109/ICCPhot.2012.6215223 
  22. Hosking, Jonathan R. M. (1992), "Moments or L moments? An example comparing two measures of distributional shape", The American Statistician 46 (3): 186–189, doi:10.1080/00031305.1992.10475880 
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Further reading

External links