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.
Given a sequence of distributions
fi
f
f[\varphi]=\limifi[\varphi]
\varphi
f
\varphi
fi[\varphi]
f
More generally, as with functions, one can also consider a limit of a family of distributions.
A distributional limit may still exist when the classical limit does not. Consider, for example, the function:
ft(x)={t\over1+t2x2}
\langleft,\phi\rangle=
0 | |
-\int | |
-infty |
\arctan(tx)\phi'(x)dx-
infty | |
\int | |
0 |
\arctan(tx)\phi'(x)dx,
\displaystyle\limt\langleft,\phi\rangle=\langle\pi\delta0,\phi\rangle
ft
t\toinfty
\pi\delta0
Let
f(x+i0)
f(x+iy)
y\to0+
f(x-i0)
One has
(x-i0)-1-(x+i0)-1=2\pii\delta0.
Let
\GammaN=[-N-1/2,N+1/2]2
IN\overset{def
\begin{align}
R | |
\int | |
-R |
\widehat{\phi}(\xi)\pi\operatorname{cot}(\pi\xi)d&=
R | |
\int | |
-R |
infty | |
\int | |
0 |
\phi(x)e-2dxd\xi+
R | |
\int | |
-R |
0 | |
\int | |
-infty |
\phi(x)e-2dxd\xi\\ &=\langle\phi,\cot( ⋅ -i0)-\cot( ⋅ -i0)\rangle \end{align}
See main article: Oscillatory integral.