The probability density function can be written
$$f(y;b,d,k) = d b^{-d k} y^{d k-1} \exp[-(y/b)^d] / \Gamma(k)$$
for scale parameter \(b > 0\),
and Weibull-type shape parameter \(d > 0\),
gamma-type shape parameter \(k > 0\),
and \(y > 0\).
The mean of \(Y\)
is \(b \times \Gamma(k+1/d) / \Gamma(k)\)
(returned as the fitted values),
which equals \(bk\) if \(d=1\).
There are many special cases, as given in Table 1 of Stacey and Mihram (1965).
In the following, the parameters are in the order \(b,d,k\).
The special cases are:
Exponential \(f(y;b,1,1)\),
Gamma \(f(y;b,1,k)\),
Weibull \(f(y;b,d,1)\),
Chi Squared \(f(y;2,1,a/2)\) with \(a\) degrees of freedom,
Chi \(f(y;\sqrt{2},2,a/2)\) with \(a\) degrees of freedom,
Half-normal \(f(y;\sqrt{2},2,1/2)\),
Circular normal \(f(y;\sqrt{2},2,1)\),
Spherical normal \(f(y;\sqrt{2},2,3/2)\),
Rayleigh \(f(y;c\sqrt{2},2,1)\) where \(c>0\).
Also the log-normal distribution corresponds to when k = Inf.