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On the Schur Test forL2-Boundedness of Positive Integral Operators with a Wiener–Hopf Example
Authors:JF Toland  D Williams
Institution:Department of Mathematical Sciences, University of Bath, Bath, BA2 7AY, United Kingdomf1
Abstract:The Schur sufficiency condition for boundedness of any integral operator with non-negative kernel betweenL2-spaces is deduced from an observation, Proposition 1.2, about the central role played byL2-spaces in the general theory of these operators. Suppose (Ω, View the MathML source, μ) is a measure space and thatK: Ω×Ω→0, ∞) is an View the MathML source×View the MathML source-measurable kernel. The special case of Proposition 1.2 for symmetrical kernels says that such a linear integral operator is bounded onanyreasonable normed linear spaceXof View the MathML source-measurable functions only if it is bounded onL2(Ω, View the MathML source, μ) where its norm is no larger. The general form of Schur's condition (Halmos and Sunder “Bounded Integral Operators onL2-Spaces,” Springer-Verlag, Berlin/New York, 1978) is a simple corollary which, in the symmetrical case, says that the existence of an View the MathML source-measurable (not necessarily square-integrable) functionh>0μ-almost-everywhere onΩwithView the MathML sourceimplies thatKis a bounded (self-adjoint) operator onL2(Ω, View the MathML source, μ) of norm at mostΛ. When (Ω, View the MathML source, μ) isσ-finite, we show that Schur's condition is sharp: in the symmetrical case the boundedness of View the MathML source onL2(Ω, View the MathML source, μ) implies, for anyΛ>‖View the MathML source2, the existence of a functionhL2(Ω, View the MathML source, μ) which is positiveμ-almost-everywhere and satisfies (*). Such functionshsatisfying (*), whether inL2(Ω, View the MathML source, μ) or not, will be calledSchur test functions. They can be found explicitly in significant examples to yield best-possible estimates of the norms for classes of integral operators with non-negative kernels. In the general theory the operators are not required to be symmetrical (a theorem of Chisholm and Everitt (Proc. Roy. Soc. Edinburgh Sect. A69(14) (1970/1971), 199–204) on non-self-adjoint operators is derived in this way). They may even act between differentL2-spaces. Section 2 is a rather substantial study of how this method yields the exact value of the norm of a particular operator between differentL2-spaces which arises naturally in Wiener–Hopf theory and which has several puzzling features.
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