In measure and probability theory in mathematics, a convex measure is a probability measure that - loosely put - does not assign more mass to any intermediate set "between" two measurable sets A and B than it does to A or B individually. There are multiple ways in which the comparison between the probabilities of A and B and the intermediate set can be made, leading to multiple definitions of convexity, such as log-concavity, harmonic convexity, and so on. The mathematician Christer Borell was a pioneer of the detailed study of convex measures on locally convex spaces in the 1970s.[1] [2]
Let X be a locally convex Hausdorff vector space, and consider a probability measure μ on the Borel σ-algebra of X. Fix -∞ ≤ s ≤ 0, and define, for u, v ≥ 0 and 0 ≤ λ ≤ 1,
Ms,(u,v)=\begin{cases}(λus+(1-λ)vs)1/s&if-infty<s<0,\ min(u,v)&ifs=-infty,\ uλv1-&ifs=0.\end{cases}
λA+(1-λ)B=\{λx+(1-λ)y\midx\inA,y\inB\}
\mu(λA+(1-λ)B)\geqMs,(\mu(A),\mu(B)).
The special case s = 0 is the inequality
\mu(λA+(1-λ)B)\geq\mu(A)λ\mu(B)1,
log\mu(λA+(1-λ)B)\geqλlog\mu(A)+(1-λ)log\mu(B).
The classes of s-convex measures form a nested increasing family as s decreases to -∞"
s\leqtand\muist-convex\implies\muiss-convex
s\leqt\implies\{s-convexmeasures\}\supseteq\{t-convexmeasures\}.
The convexity of a measure μ on n-dimensional Euclidean space Rn in the sense above is closely related to the convexity of its probability density function.[2] Indeed, μ is s-convex if and only if there is an absolutely continuous measure ν with probability density function ρ on some Rk so that μ is the push-forward on ν under a linear or affine map and
es,\circ\rho\colonRk\toR
es,(t)=\begin{cases}ts&if-infty<s<0\ t-1/k&ifs=-infty,\ -logt&ifs=0.\end{cases}
Convex measures also satisfy a zero-one law: if G is a measurable additive subgroup of the vector space X (i.e. a measurable linear subspace), then the inner measure of G under μ,
\mu\ast(G)=\sup\{\mu(K)\midK\subseteqGandKiscompact\},