In mathematics, a function is said to vanish at infinity if its values approach 0 as the input grows without bounds. There are two different ways to define this with one definition applying to functions defined on normed vector spaces and the other applying to functions defined on locally compact spaces. Aside from this difference, both of these notions correspond to the intuitive notion of adding a point at infinity, and requiring the values of the function to get arbitrarily close to zero as one approaches it. This definition can be formalized in many cases by adding an (actual) point at infinity.
A function on a normed vector space is said to if the function approaches
0
f(x)\to0
\|x\|\toinfty
\limxf(x)=\limxf(x)=0.
in the specific case of functions on the real line.
For example, the function
f(x)=
1 | |
x2+1 |
defined on the real line vanishes at infinity.
Alternatively, a function
f
K
\|f(x)\|<\varepsilon
whenever the point
x
K.
\left\{x\inX:\|f(x)\|\geq\varepsilon\right\}
\Omega
f:\Omega\toK
valued in
K,
\R
\C,
K
C0(\Omega).
As an example, the function
h(x,y)=
1 | |
x+y |
where
x
y
(x,y)
2 | |
\R | |
\ge1 |
A normed space is locally compact if and only if it is finite-dimensional so in this particular case, there are two different definitions of a function "vanishing at infinity". The two definitions could be inconsistent with each other: if
f(x)=\|x\|-1
f
\|f(x)\|\to0
See main article: Schwartz space.
Refining the concept, one can look more closely to the of functions at infinity. One of the basic intuitions of mathematical analysis is that the Fourier transform interchanges smoothness conditions with rate conditions on vanishing at infinity. The test functions of tempered distribution theory are smooth functions that are
O\left(|x|-N\right)
for all
N
|x|\toinfty