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单词 operatornamepvfrac1xIsADistributionOfFirstOrder
释义

p.\\tmspace-.1667emv.(1x) is a distribution of first order


(Following [1, 2].)Let u𝒟(U). Then suppu[-k,k] forsome k>0. For any ε>0, u(x)/x is Lebesgue integrableMathworldPlanetmathin |x|[ε,k]. Thus, by a change of variable, we have

p.v.(1x)(u)=limε0+[ε,k]u(x)-u(-x)x𝑑x.

Now it is clear that the integrand is continuousMathworldPlanetmathPlanetmath for all x{0}.What is more, the integrand approaches 2u(0) for x0, so theintegrand has a removable discontinuity at x=0. That is, by assigning the value2u(0) to the integrand at x=0, the integrand becomes continuous in [0,k].This means that the integrand is Lebesgue measurable on [0,k].Then, by definingfn(x)=χ[1/n,k](u(x)-u(-x))/x(where χ is the characteristic functionMathworldPlanetmathPlanetmathPlanetmathPlanetmath), andapplying the Lebesgue dominated convergence theoremMathworldPlanetmath, we have

p.v.(1x)(u)=[0,k]u(x)-u(-x)x𝑑x.

It follows that p.v.(1x)(u) is finite, i.e., p.v.(1x) takes values in .Since 𝒟(U) is a vector space, if follows easily from the above expressionthat p.v.(1x) is linear.

To prove that p.v.(1x) is continuous, we shall use condition (3) onthis page (http://planetmath.org/Distribution4).For this, suppose K is a compact subset of andu𝒟K. Again, we can assume that K[-k,k] for some k>0.For x>0, we have

|u(x)-u(-x)x|=|1x(-x,x)u(t)𝑑t|
2||u||,

where |||| is the supremum norm. In the first equality we have used thefundamental theorem of calculusMathworldPlanetmathPlanetmath for the Lebesgue integral (valid sinceu is absolutely continuousMathworldPlanetmath on [-k,k]). Thus

|p.v.(1x)(u)|2k||u||

and p.v.(1x) is a distributionPlanetmathPlanetmathPlanetmath of first order (http://planetmath.org/Distribution4) as claimed.

References

  • 1 M. Reed, B. Simon,Methods of Modern Mathematical Physics: Functional AnalysisMathworldPlanetmath I,Revised and enlarged edition, Academic Press, 1980.
  • 2 S. Igari, Real analysis - With an introduction to Wavelet Theory, American Mathematical Society, 1998.
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