In optimal transport, a branch of mathematics, polar factorization of vector fields is a basic result due to Brenier (1987), with antecedents of Knott-Smith (1984) and Rachev (1985), that generalizes many existing results among which are the polar decomposition of real matrices, and the rearrangement of real-valued functions.
The theorem Notation. Denote ξ # μ {\displaystyle \xi _{\#}\mu } the image measure of μ {\displaystyle \mu } through the map ξ {\displaystyle \xi } . Definition: Measure preserving map. Let ( X , μ ) {\displaystyle (X,\mu )} and ( Y , ν ) {\displaystyle (Y,\nu )} be some probability spaces and σ : X → Y {\displaystyle \sigma :X\rightarrow Y} a measurable map. Then, σ {\displaystyle \sigma } is said to be measure preserving iff σ # μ = ν {\displaystyle \sigma _{\#}\mu =\nu } , where # {\displaystyle \#} is the pushforward measure. Spelled out: for every ν {\displaystyle \nu } -measurable subset Ω {\displaystyle \Omega } of Y {\displaystyle Y} , σ − 1 ( Ω ) {\displaystyle \sigma ^{-1}(\Omega )} is μ {\displaystyle \mu } -measurable, and μ ( σ − 1 ( Ω ) ) = ν ( Ω ) {\displaystyle \mu (\sigma ^{-1}(\Omega ))=\nu (\Omega )} . The latter is equivalent to:
∫ X ( f ∘ σ ) ( x ) μ ( d x ) = ∫ X ( σ ∗ f ) ( x ) μ ( d x ) = ∫ Y f ( y ) ( σ # μ ) ( d y ) = ∫ Y f ( y ) ν ( d y ) {\displaystyle \int _{X}(f\circ \sigma )(x)\mu (dx)=\int _{X}(\sigma ^{*}f)(x)\mu (dx)=\int _{Y}f(y)(\sigma _{\#}\mu )(dy)=\int _{Y}f(y)\nu (dy)}
where f {\displaystyle f} is ν {\displaystyle \nu } -integrable and f ∘ σ {\displaystyle f\circ \sigma } is μ {\displaystyle \mu } -integrable. Theorem. Consider a map ξ : Ω → R d {\displaystyle \xi :\Omega \rightarrow \mathbb {R} ^{d}} where Ω {\displaystyle \Omega } is a convex subset of R d {\displaystyle \mathbb {R} ^{d}} , and μ {\displaystyle \mu } a measure on Ω {\displaystyle \Omega } which is absolutely continuous. Assume that ξ # μ {\displaystyle \xi _{\#}\mu } is absolutely continuous. Then there is a convex function φ : Ω → R {\displaystyle \varphi :\Omega \rightarrow \mathbb {R} } and a map σ : Ω → Ω {\displaystyle \sigma :\Omega \rightarrow \Omega } preserving μ {\displaystyle \mu } such that
ξ = ( ∇ φ ) ∘ σ {\displaystyle \xi =\left(\nabla \varphi \right)\circ \sigma }
In addition, ∇ φ {\displaystyle \nabla \varphi } and σ {\displaystyle \sigma } are uniquely defined almost everywhere.
Applications and connections
Dimension 1 In dimension 1, and when μ {\displaystyle \mu } is the Lebesgue measure over the unit interval, the result specializes to Ryff's theorem. When d = 1 {\displaystyle d=1} and μ {\displaystyle \mu } is the uniform distribution over [ 0 , 1 ] {\displaystyle \left[0,1\right]} , the polar decomposition boils down to
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