The Titchmarsh convolution theorem describes the properties of the support of the convolution of two functions. It was proven by Edward Charles Titchmarsh in 1926.
Titchmarsh convolution theorem If φ ( t ) {\textstyle \varphi (t)\,} and ψ ( t ) {\textstyle \psi (t)} are integrable functions, such that
φ ∗ ψ = ∫ 0 x φ ( t ) ψ ( x − t ) d t = 0 {\displaystyle \varphi *\psi =\int _{0}^{x}\varphi (t)\psi (x-t)\,dt=0}
almost everywhere in the interval 0 < x < κ {\displaystyle 0<x<\kappa \,} , then there exist λ ≥ 0 {\displaystyle \lambda \geq 0} and μ ≥ 0 {\displaystyle \mu \geq 0} satisfying λ + μ ≥ κ {\displaystyle \lambda +\mu \geq \kappa } such that φ ( t ) = 0 {\displaystyle \varphi (t)=0\,} almost everywhere in 0 < t < λ {\displaystyle 0<t<\lambda } and ψ ( t ) = 0 {\displaystyle \psi (t)=0\,} almost everywhere in 0 < t < μ . {\displaystyle 0<t<\mu .}
As a corollary, if the integral above is 0 for all x > 0 , {\textstyle x>0,} then either φ {\textstyle \varphi \,} or ψ {\textstyle \psi } is almost everywhere 0 in the interval [ 0 , + ∞ ) . {\textstyle [0,+\infty ).} Thus the convolution of two functions on [ 0 , + ∞ ) {\textstyle [0,+\infty )} cannot be identically zero unless at least one of the two functions is identically zero. As another corollary, if φ ∗ ψ ( x ) = 0 {\displaystyle \varphi *\psi (x)=0} for all x ∈ [ 0 , κ ] {\displaystyle x\in [0,\kappa ]} and one of the function φ {\displaystyle \varphi } or ψ {\displaystyle \psi } is almost everywhere not null in this interval, then the other function must be null almost everywhere in [ 0 , κ ] {\displaystyle [0,\kappa ]} . The theorem can be restated in the following form:
Let φ , ψ ∈ L 1 ( R ) {\displaystyle \varphi ,\psi \in L^{1}(\mathbb {R} )} . Then inf supp φ ∗ ψ = inf supp φ + inf supp ψ {\displaystyle \inf \operatorname {supp} \varphi \ast \psi =\inf \operatorname {supp} \varphi +\inf \operatorname {supp} \psi } if the left-hand side is finite. Similarly, sup supp φ ∗ ψ = sup supp φ + sup supp ψ {\displaystyle \sup \operatorname {supp} \varphi \ast \psi =\sup \operatorname {supp} \varphi +\sup \operatorname {supp} \psi } if the right-hand side is finite. Above, supp {\displaystyle \operatorname {supp} } denotes the support of a function f (i.e., the closure of the complement of f−1(0)) and inf {\displaystyle \inf } and sup {\displaystyle \sup } denote the infimum and supremum. This theorem essentially states that the well-known inclusion supp φ ∗ ψ ⊂ supp φ + supp ψ {\displaystyle \operatorname {supp} \varphi \ast \psi \subset \operatorname {supp} \varphi +\operatorname {supp} \psi } is sharp at the boundary. The higher-dimensional generalization in terms of the convex hull of the supports was proven by Jacques-Louis Lions in 1951:
If φ , ψ ∈ E ′ ( R n ) {\displaystyle \varphi ,\psi \in {\mathcal {E}}'(\mathbb {R} ^{n})} , then c . h . supp φ ∗ ψ = c . h . supp φ + c . h . supp ψ {\displaystyle \operatorname {c.h.} \operatorname {supp} \varphi \ast \psi =\operatorname {c.h.} \operatorname {supp} \varphi +\operatorname {c.h.} \operatorname {supp} \psi }
… excerpt ends here. Continue reading the full article.
