{Red-Horse}
Two types of uncertainty:
Inherent uncertainty is uncertainty that cannot be reduced by gathering more information. The origins of this class of uncertainty typically occur at scales that are smaller than either the model or the observations in a given study. Other names for this uncertainty are irreducible uncertainty, aleatoric uncertainty, and variability.
Ignorance is typically associated with limitations in models or available experimental data.
Two approaches to probability:
For a probability space $(\Omega, \Sigma, P)$ and an arbitrary measurable space $(H, \mathcal{H})$, random variable $X: \Omega \to H$ is a $(\Sigma, \mathcal{H})$-measuralbe function. It has induced distribution
$$\eta_X (X \in A) = P(X^{-1}(A)), \quad A \in \mathcal{H}$$
$H$ be a metric space.
Topological dual: the space of continuous linear functionals defined on a topological linear space.
Weak topology: the topological dual of a topological linear space induce a topology in the original space where neighborhoods are defined in terms of their images under the duality pairing. It is a subset of the original topology, i.e. a weaker topology.
duality pairing
Reproducing kernel Hilbert spaces (RKHS): The operator $S_X^{-1}$ is a reproducing kernel in $H_X$
A countably-normed space is a topological vector space over $C$ with topology given by a countable family of norms (i.e. intersection of all norm-induce neighborhoods). A countably-Hilbert space is a countably-normed space complete with respect to its topology, and each norm is induced from an inner product.
The compatibility requirement on the norms associated with a countably-Hilbert spaceimplies an ordering in these norms.
Nuclear operator
Both the covariance operator and the characteristic functional of a stochastic process are nuclear operators.
Nuclear space
canonical embedding
Kolmogorov consistency requirements
When $H$ is a Hilbert space, the covariance opertator $S_X$ is Hilbert–Schmidt, self-adjoint, positive, and completely continuous, and therefore has a finite or countable set of eigenvalues and corresponding orthonormal eigenfunctions ${ (\lambda_n, \phi_n) }$.
The RKHS structure ensures that the evaluation functional in this space is continuous.
Thus we have Karhunen–Loeve expansion for such defined RVs.