The family of all normal distributions, parametrized by the expected valueμ and the varianceσ2 ≥ 0, with the Riemannian metric given by the Fisher information matrix, is a statistical manifold. Its geometry is modeled on hyperbolic space. A simple example of a statistical manifold, taken from physics, would be the canonical ensemble: it is a one-dimensional manifold, with the temperatureT serving as the coordinate on the manifold. For any fixed temperature T, one has a probability space: so, for a gas of atoms, it would be the probability distribution of the velocities of the atoms. As one varies the temperature T, the probability distribution varies. Another simple example, taken from medicine, would be the probability distribution of patientoutcomes, in response to the quantity of medicine administered. That is, for a fixed dose, some patients improve, and some do not: this is the baseprobability space. If the dosage is varied, then the probability of outcomes changes. Thus, the dosage is the coordinate on the manifold. To be a smooth manifold, one would have to measure outcomes in response to arbitrarily small changes in dosage; this is not a practically realizable example, unless one has a pre-existing mathematical model of dose-response where the dose can be arbitrarily varied.
Definition
Let X be an orientable manifold, and let be a measure on X. Equivalently, let be a probability space on, with sigma algebra and probability. The statistical manifold S of X is defined as the space of all measures on X. Note that this space is infinite-dimensional; it is commonly taken to be a Fréchet space. The points of S are measures. Rather than dealing with an infinite-dimensional spaceS, it is common to work with a finite-dimensional submanifold, defined by considering a set of probability distributions parameterized by some smooth, continuously-varying parameter. That is, one considers only those measures that are selected by the parameter. If the parameter is n-dimensional, then, in general, the submanifold will be as well. All finite-dimensional statistical manifolds can be understood in this way.