Limit of distributions
In mathematics, specifically in the theory of generalized functions, the limit 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 a limit 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 of calculus that is based on the notion of distributions, as opposed to classical calculus, which is based on the narrower concept of functions.
Definition
[edit ]Given a sequence of distributions {\displaystyle f_{i}}, its limit {\displaystyle f} is the distribution given by
- {\displaystyle f[\varphi ]=\lim _{i\to \infty }f_{i}[\varphi ]}
for each test function {\displaystyle \varphi }, provided that distribution exists. The existence of the limit {\displaystyle f} means that (1) for each {\displaystyle \varphi }, the limit of the sequence of numbers {\displaystyle f_{i}[\varphi ]} exists and that (2) the linear functional {\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
[edit ]A distributional limit may still exist when the classical limit does not. Consider, for example, the function:
- {\displaystyle f_{t}(x)={t \over 1+t^{2}x^{2}}}
Since, by integration by parts,
- {\displaystyle \langle f_{t},\phi \rangle =-\int _{-\infty }^{0}\arctan(tx)\phi '(x),円dx-\int _{0}^{\infty }\arctan(tx)\phi '(x),円dx,}
we have: {\displaystyle \displaystyle \lim _{t\to \infty }\langle f_{t},\phi \rangle =\langle \pi \delta _{0},\phi \rangle }. That is, the limit of {\displaystyle f_{t}} as {\displaystyle t\to \infty } is {\displaystyle \pi \delta _{0}}.
Let {\displaystyle f(x+i0)} denote the distributional limit of {\displaystyle f(x+iy)} as {\displaystyle y\to 0^{+}}, if it exists. The distribution {\displaystyle f(x-i0)} is defined similarly.
One has
- {\displaystyle (x-i0)^{-1}-(x+i0)^{-1}=2\pi i\delta _{0}.}
Let {\displaystyle \Gamma _{N}=[-N-1/2,N+1/2]^{2}} be the rectangle with positive orientation, with an integer N. By the residue formula,
- {\displaystyle I_{N}{\overset {\mathrm {def} }{=}}\int _{\Gamma _{N}}{\widehat {\phi }}(z)\pi \cot(\pi z),円dz={2\pi i}\sum _{-N}^{N}{\widehat {\phi }}(n).}
On the other hand,
- {\displaystyle {\begin{aligned}\int _{-R}^{R}{\widehat {\phi }}(\xi )\pi \operatorname {cot} (\pi \xi ),円d&=\int _{-R}^{R}\int _{0}^{\infty }\phi (x)e^{-2\pi Ix\xi },円dx,円d\xi +\int _{-R}^{R}\int _{-\infty }^{0}\phi (x)e^{-2\pi Ix\xi },円dx,円d\xi \\&=\langle \phi ,\cot(\cdot -i0)-\cot(\cdot -i0)\rangle \end{aligned}}}
Oscillatory integral
[edit ]See also
[edit ]References
[edit ]- Demailly, Complex Analytic and Differential Geometry
- Hörmander, Lars, The Analysis of Linear Partial Differential Operators, Springer-Verlag
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