Part 7 of 15. Every distribution you fit in practice is an exponential family, and every exponential family comes with two flat coordinate systems linked by a Legendre transform. This is why the scaffolding of modern statistics works.
Play: Drag the parameter point in either natural coordinates θ (left) or expectation coordinates η (right). Observe how the Legendre transform perfectly syncs the two representations. Notice that dragging a straight line in one space results in a curved path in the other.
An exponential family has the canonical form:
Every exponential family is dually flat, meaning it comes with two distinct, flat coordinate systems linked by a Legendre transform:
The gradient of the log-partition function (a strictly convex function) maps natural parameters to expectation parameters. Its Legendre dual (negative entropy) maps them back.
The same structure applies to every exponential family. Table 1 lists a handful of the most common ones with their sufficient statistics, natural parameters, log-partition functions, and the resulting expectation parameters. Each row is a self-contained Legendre pair, and in each the Fisher matrix is the Hessian of in the natural coordinates.
| Family | T(x) | θ | ψ(θ) | η = E[T] |
|---|---|---|---|---|
| Bernoulli(p) | ||||
| Poisson(λ) | ||||
| Exponential(λ) | ||||
| Gaussian(μ, σ²) | ||||
| Categorical(p) |
The categorical row is the exponential family behind softmax. Softmax converts natural to expectation parameters via , and cross-entropy is the KL divergence that respects the dually flat geometry. Natural gradient descent on a softmax (Part 10) is gradient descent in the flat expectation coordinates.
What "dually flat" buys you. The natural parameters flatten the e-connection; the expectation parameters flatten the m-connection. The hyperbolic curvature of the Poincaré half-plane is a property of Levi-Civita, not of the e- or m-connections.
One payoff we can already extract. KL divergence on an exponential family has a closed-form expression in terms of the two potentials:
This is the Bregman divergence of (Part 9 generalises). The Legendre dual:
Same number, different coordinates. The duality is what makes the Part 8 Pythagorean theorem possible.
Part 8 proves the generalised Pythagorean theorem: if lie on a dually flat manifold with the e-geodesic from to Fisher-orthogonal to the m-geodesic from to , then . KL decomposes additively under orthogonal projection — the engine of maximum likelihood, EM, and variational inference.