The Fréchet distribution, also known as inverse Weibull distribution,[2][3] is a special case of the generalized extreme value distribution. It has the cumulative distribution function
where α > 0 is a shape parameter. It can be generalised to include a location parameter m (the minimum) and a scale parameter s > 0 with the cumulative distribution function
Named for Maurice Fréchet who wrote a related paper in 1927,[4] further work was done by Fisher and Tippett in 1928 and by Gumbel in 1958.[5][6]
The single parameter Fréchet, with parameter α , {\displaystyle \ \alpha \ ,} has standardized moment
(with t = x − α {\displaystyle \ t=x^{-\alpha }\ } ) defined only for k < α : {\displaystyle \ k<\alpha \ :}
where Γ ( z ) {\displaystyle \ \Gamma \left(z\right)\ } is the Gamma function.
In particular:
The quantile q y {\displaystyle q_{y}} of order y {\displaystyle y} can be expressed through the inverse of the distribution,
In particular the median is:
The mode of the distribution is ( α α + 1 ) 1 α . {\displaystyle \left({\frac {\alpha }{\alpha +1}}\right)^{\frac {1}{\alpha }}.}
Especially for the 3-parameter Fréchet, the first quartile is q 1 = m + s log ( 4 ) α {\displaystyle q_{1}=m+{\frac {s}{\sqrt[{\alpha }]{\log(4)}}}} and the third quartile q 3 = m + s log ( 4 3 ) α . {\displaystyle q_{3}=m+{\frac {s}{\sqrt[{\alpha }]{\log({\frac {4}{3}})}}}.}
Also the quantiles for the mean and mode are:
However, in most hydrological applications, the distribution fitting is via the generalized extreme value distribution as this avoids imposing the assumption that the distribution does not have a lower bound (as required by the Frechet distribution). [citation needed]