M. Riesz extension theorem

The M. Riesz extension theorem is a theorem in mathematics, proved by Marcel Riesz[1] during his study of the problem of moments.[2]

Formulation

Let E {\displaystyle E} be a real vector space, F E {\displaystyle F\subset E} be a vector subspace, and K E {\displaystyle K\subset E} be a convex cone.

A linear functional ϕ : F R {\displaystyle \phi :F\to \mathbb {R} } is called K {\displaystyle K} -positive, if it takes only non-negative values on the cone K {\displaystyle K} :

ϕ ( x ) 0 for x F K . {\displaystyle \phi (x)\geq 0\quad {\text{for}}\quad x\in F\cap K.}

A linear functional ψ : E R {\displaystyle \psi :E\to \mathbb {R} } is called a K {\displaystyle K} -positive extension of ϕ {\displaystyle \phi } , if it is identical to ϕ {\displaystyle \phi } in the domain of ϕ {\displaystyle \phi } , and also returns a value of at least 0 for all points in the cone K {\displaystyle K} :

ψ | F = ϕ and ψ ( x ) 0 for x K . {\displaystyle \psi |_{F}=\phi \quad {\text{and}}\quad \psi (x)\geq 0\quad {\text{for}}\quad x\in K.}

In general, a K {\displaystyle K} -positive linear functional on F {\displaystyle F} cannot be extended to a K {\displaystyle K} -positive linear functional on E {\displaystyle E} . Already in two dimensions one obtains a counterexample. Let E = R 2 ,   K = { ( x , y ) : y > 0 } { ( x , 0 ) : x > 0 } , {\displaystyle E=\mathbb {R} ^{2},\ K=\{(x,y):y>0\}\cup \{(x,0):x>0\},} and F {\displaystyle F} be the x {\displaystyle x} -axis. The positive functional ϕ ( x , 0 ) = x {\displaystyle \phi (x,0)=x} can not be extended to a positive functional on E {\displaystyle E} .

However, the extension exists under the additional assumption that E K + F , {\displaystyle E\subset K+F,} namely for every y E , {\displaystyle y\in E,} there exists an x F {\displaystyle x\in F} such that y x K . {\displaystyle y-x\in K.}

Proof

The proof is similar to the proof of the Hahn–Banach theorem (see also below).

By transfinite induction or Zorn's lemma it is sufficient to consider the case dim  E / F = 1 {\displaystyle E/F=1} .

Choose any y E F {\displaystyle y\in E\setminus F} . Set

a = sup { ϕ ( x ) x F ,   y x K } ,   b = inf { ϕ ( x ) x F , x y K } . {\displaystyle a=\sup\{\,\phi (x)\mid x\in F,\ y-x\in K\,\},\ b=\inf\{\,\phi (x)\mid x\in F,x-y\in K\,\}.}

We will prove below that < a b {\displaystyle -\infty <a\leq b} . For now, choose any c {\displaystyle c} satisfying a c b {\displaystyle a\leq c\leq b} , and set ψ ( y ) = c {\displaystyle \psi (y)=c} , ψ | F = ϕ {\displaystyle \psi |_{F}=\phi } , and then extend ψ {\displaystyle \psi } to all of E {\displaystyle E} by linearity. We need to show that ψ {\displaystyle \psi } is K {\displaystyle K} -positive. Suppose z K {\displaystyle z\in K} . Then either z = 0 {\displaystyle z=0} , or z = p ( x + y ) {\displaystyle z=p(x+y)} or z = p ( x y ) {\displaystyle z=p(x-y)} for some p > 0 {\displaystyle p>0} and x F {\displaystyle x\in F} . If z = 0 {\displaystyle z=0} , then ψ ( z ) > 0 {\displaystyle \psi (z)>0} . In the first remaining case x + y = y ( x ) K {\displaystyle x+y=y-(-x)\in K} , and so

ψ ( y ) = c a ϕ ( x ) = ψ ( x ) {\displaystyle \psi (y)=c\geq a\geq \phi (-x)=\psi (-x)}

by definition. Thus

ψ ( z ) = p ψ ( x + y ) = p ( ψ ( x ) + ψ ( y ) ) 0. {\displaystyle \psi (z)=p\psi (x+y)=p(\psi (x)+\psi (y))\geq 0.}

In the second case, x y K {\displaystyle x-y\in K} , and so similarly

ψ ( y ) = c b ϕ ( x ) = ψ ( x ) {\displaystyle \psi (y)=c\leq b\leq \phi (x)=\psi (x)}

by definition and so

ψ ( z ) = p ψ ( x y ) = p ( ψ ( x ) ψ ( y ) ) 0. {\displaystyle \psi (z)=p\psi (x-y)=p(\psi (x)-\psi (y))\geq 0.}

In all cases, ψ ( z ) > 0 {\displaystyle \psi (z)>0} , and so ψ {\displaystyle \psi } is K {\displaystyle K} -positive.

We now prove that < a b {\displaystyle -\infty <a\leq b} . Notice by assumption there exists at least one x F {\displaystyle x\in F} for which y x K {\displaystyle y-x\in K} , and so < a {\displaystyle -\infty <a} . However, it may be the case that there are no x F {\displaystyle x\in F} for which x y K {\displaystyle x-y\in K} , in which case b = {\displaystyle b=\infty } and the inequality is trivial (in this case notice that the third case above cannot happen). Therefore, we may assume that b < {\displaystyle b<\infty } and there is at least one x F {\displaystyle x\in F} for which x y K {\displaystyle x-y\in K} . To prove the inequality, it suffices to show that whenever x F {\displaystyle x\in F} and y x K {\displaystyle y-x\in K} , and x F {\displaystyle x'\in F} and x y K {\displaystyle x'-y\in K} , then ϕ ( x ) ϕ ( x ) {\displaystyle \phi (x)\leq \phi (x')} . Indeed,

x x = ( x y ) + ( y x ) K {\displaystyle x'-x=(x'-y)+(y-x)\in K}

since K {\displaystyle K} is a convex cone, and so

0 ϕ ( x x ) = ϕ ( x ) ϕ ( x ) {\displaystyle 0\leq \phi (x'-x)=\phi (x')-\phi (x)}

since ϕ {\displaystyle \phi } is K {\displaystyle K} -positive.

Corollary: Krein's extension theorem

Let E be a real linear space, and let K ⊂ E be a convex cone. Let x ∈ E/(−K) be such that R x + K = E. Then there exists a K-positive linear functional φE → R such that φ(x) > 0.

Connection to the Hahn–Banach theorem

The Hahn–Banach theorem can be deduced from the M. Riesz extension theorem.

Let V be a linear space, and let N be a sublinear function on V. Let φ be a functional on a subspace U ⊂ V that is dominated by N:

ϕ ( x ) N ( x ) , x U . {\displaystyle \phi (x)\leq N(x),\quad x\in U.}

The Hahn–Banach theorem asserts that φ can be extended to a linear functional on V that is dominated by N.

To derive this from the M. Riesz extension theorem, define a convex cone K ⊂ R×V by

K = { ( a , x ) N ( x ) a } . {\displaystyle K=\left\{(a,x)\,\mid \,N(x)\leq a\right\}.}

Define a functional φ1 on R×U by

ϕ 1 ( a , x ) = a ϕ ( x ) . {\displaystyle \phi _{1}(a,x)=a-\phi (x).}

One can see that φ1 is K-positive, and that K + (R × U) = R × V. Therefore φ1 can be extended to a K-positive functional ψ1 on R×V. Then

ψ ( x ) = ψ 1 ( 0 , x ) {\displaystyle \psi (x)=-\psi _{1}(0,x)}

is the desired extension of φ. Indeed, if ψ(x) > N(x), we have: (N(x), x) ∈ K, whereas

ψ 1 ( N ( x ) , x ) = N ( x ) ψ ( x ) < 0 , {\displaystyle \psi _{1}(N(x),x)=N(x)-\psi (x)<0,}

leading to a contradiction.

References

Sources

  • Castillo, Reńe E. (2005), "A note on Krein's theorem" (PDF), Lecturas Matematicas, 26, archived from the original (PDF) on 2014-02-01, retrieved 2014-01-18
  • Riesz, M. (1923), "Sur le problème des moments. III.", Arkiv för Matematik, Astronomi och Fysik (in French), 17 (16), JFM 49.0195.01
  • Akhiezer, N.I. (1965), The classical moment problem and some related questions in analysis, New York: Hafner Publishing Co., MR 0184042
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