An exponential dispersion model adds a second parameter, the dispersion index, to a natural exponential family (here
with mean
Reproductive property
If
are independent with and , then . At a common mean the precisions add. Under addition the index set is a commutative monoid, a convex cone, acting by convolution, and the weighted average is its projectivisation.
Example, continuous index and the Tweedie class
The additive model extends to a continuous index, a Lévy convolution semigroup
, iff is a Lévy exponent, equivalently the generating law is infinitely divisible. Among natural exponential families the reproducible ones are exactly the power-variance Tweedie models, with (Bar-Lev–Enis), obeying the scaling . The index flow’s generator is a genuine transport velocity iff the Lévy measure vanishes, giving Gaussian ; otherwise it is a jump process.