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Limit of distributions

From Wikipedia, the free encyclopedia
This article is about limits of sequences of generalized functions. For limits of probability distributions, seeConvergence of random variables § Convergence in distribution.

Inmathematics, specifically in the theory ofgeneralized functions, thelimit of a sequence of distributions is the distribution that sequence approaches. The distance, suitably quantified, to the limiting distribution can be made arbitrarily small by selecting a distribution sufficiently far along the sequence. This notion generalizes alimit of a sequence of functions; a limit as a distribution may exist when a limit of functions does not.

The notion is a part of distributional calculus, a generalized form ofcalculus that is based on the notion of distributions, as opposed to classical calculus, which is based on the narrower concept offunctions.

Definition

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Given a sequence of distributionsfi{\displaystyle f_{i}}, its limitf{\displaystyle f} is the distribution given by

f[φ]=limifi[φ]{\displaystyle f[\varphi ]=\lim _{i\to \infty }f_{i}[\varphi ]}

for each test functionφ{\displaystyle \varphi }, provided that distribution exists. The existence of the limitf{\displaystyle f} means that (1) for eachφ{\displaystyle \varphi }, thelimit of the sequence of numbersfi[φ]{\displaystyle f_{i}[\varphi ]} exists and that (2) the linear functionalf{\displaystyle f} defined by the above formula is continuous with respect to the topology on the space of test functions.

More generally, as with functions, one can also consider a limit of a family of distributions.

Examples

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A distributional limit may still exist when theclassical limit does not. Consider, for example, the function:

ft(x)=t1+t2x2{\displaystyle f_{t}(x)={t \over 1+t^{2}x^{2}}}

Since, byintegration by parts,

ft,ϕ=0arctan(tx)ϕ(x)dx0arctan(tx)ϕ(x)dx,{\displaystyle \langle f_{t},\phi \rangle =-\int _{-\infty }^{0}\arctan(tx)\phi '(x)\,dx-\int _{0}^{\infty }\arctan(tx)\phi '(x)\,dx,}

we have:limtft,ϕ=πδ0,ϕ{\displaystyle \displaystyle \lim _{t\to \infty }\langle f_{t},\phi \rangle =\langle \pi \delta _{0},\phi \rangle }. That is, the limit offt{\displaystyle f_{t}} ast{\displaystyle t\to \infty } isπδ0{\displaystyle \pi \delta _{0}}.

Letf(x+i0){\displaystyle f(x+i0)} denote the distributional limit off(x+iy){\displaystyle f(x+iy)} asy0+{\displaystyle y\to 0^{+}}, if it exists. The distributionf(xi0){\displaystyle f(x-i0)} is defined similarly.

One has

(xi0)1(x+i0)1=2πiδ0.{\displaystyle (x-i0)^{-1}-(x+i0)^{-1}=2\pi i\delta _{0}.}

LetΓN=[N1/2,N+1/2]2{\displaystyle \Gamma _{N}=[-N-1/2,N+1/2]^{2}} be the rectangle with positive orientation, with an integerN. By theresidue formula,

IN=defΓNϕ^(z)πcot(πz)dz=2πiNNϕ^(n).{\displaystyle I_{N}{\overset {\mathrm {def} }{=}}\int _{\Gamma _{N}}{\widehat {\phi }}(z)\pi \cot(\pi z)\,dz={2\pi i}\sum _{-N}^{N}{\widehat {\phi }}(n).}

On the other hand,

RRϕ^(ξ)πcot(πξ)d=RR0ϕ(x)e2πIxξdxdξ+RR0ϕ(x)e2πIxξdxdξ=ϕ,cot(i0)cot(i0){\displaystyle {\begin{aligned}\int _{-R}^{R}{\widehat {\phi }}(\xi )\pi \operatorname {cot} (\pi \xi )\,d&=\int _{-R}^{R}\int _{0}^{\infty }\phi (x)e^{-2\pi Ix\xi }\,dx\,d\xi +\int _{-R}^{R}\int _{-\infty }^{0}\phi (x)e^{-2\pi Ix\xi }\,dx\,d\xi \\&=\langle \phi ,\cot(\cdot -i0)-\cot(\cdot -i0)\rangle \end{aligned}}}

Oscillatory integral

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Main article:Oscillatory integral

See also

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References

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  • Demailly, Complex Analytic and Differential Geometry
  • Hörmander, Lars,The Analysis of Linear Partial Differential Operators, Springer-Verlag


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