Difference between revisions of "Pole (of a function)"
(TeX) |
(MSC) |
||
Line 1: | Line 1: | ||
+ | {{MSC|}} | ||
+ | {{TEX|done}} | ||
$ | $ | ||
\newcommand{\abs}[1]{\left| #1 \right|} | \newcommand{\abs}[1]{\left| #1 \right|} | ||
\newcommand{\set}[1]{\left\{ #1 \right\}} | \newcommand{\set}[1]{\left\{ #1 \right\}} | ||
$ | $ | ||
+ | |||
An isolated [[Singular point|singular point]] of single-valued character of an analytic function f(z) of the complex variable z for which \abs{f(z)} increases without bound when z approaches a: \lim_{z\rightarrow a} f(z) = \infty. In a sufficiently small punctured neighbourhood V=\set{z\in\C : 0 < \abs{z-a} < R} of the point a \neq \infty, or V'=\set{z\in\C : r < \abs{z} < \infty} in the case of the point at infinity a=\infty, the function f(z) can be written as a [[Laurent series]] of special form: | An isolated [[Singular point|singular point]] a of single-valued character of an analytic function f(z) of the complex variable z for which \abs{f(z)} increases without bound when z approaches a: \lim_{z\rightarrow a} f(z) = \infty. In a sufficiently small punctured neighbourhood V=\set{z\in\C : 0 < \abs{z-a} < R} of the point a \neq \infty, or V'=\set{z\in\C : r < \abs{z} < \infty} in the case of the point at infinity a=\infty, the function f(z) can be written as a [[Laurent series]] of special form: | ||
Line 27: | Line 30: | ||
====References==== | ====References==== | ||
− | + | {| | |
+ | |- | ||
+ | |valign="top"|{{Ref|Sh}}||valign="top"| B.V. Shabat, "Introduction of complex analysis", '''2''', Moscow (1976) (In Russian) | ||
+ | |- | ||
+ | |} | ||
+ | |||
====Comments==== | ====Comments==== | ||
− | For n=1 see | + | For n=1 see {{Cite|Ah}}. For n \geq 2 see {{Cite|GrFr}}, {{Cite|Ra}}. |
For the use of poles in the representation of analytic functions see [[Integral representation of an analytic function]]; [[Cauchy integral]]. | For the use of poles in the representation of analytic functions see [[Integral representation of an analytic function]]; [[Cauchy integral]]. | ||
Line 37: | Line 45: | ||
====References==== | ====References==== | ||
− | + | {| | |
+ | |- | ||
+ | |valign="top"|{{Ref|Ah}}||valign="top"| L.V. Ahlfors, "Complex analysis", McGraw-Hill (1979) pp. Chapt. 8 | ||
+ | |- | ||
+ | |valign="top"|{{Ref|GrFr}}||valign="top"| H. Grauert, K. Fritzsche, "Several complex variables", Springer (1976) (Translated from German) | ||
+ | |- | ||
+ | |valign="top"|{{Ref|Ra}}||valign="top"| R.M. Range, "Holomorphic functions and integral representation in several complex variables", Springer (1986) pp. Chapt. 1, Sect. 3 | ||
+ | |- | ||
+ | |} |
Revision as of 21:55, 29 April 2012
\newcommand{\abs}[1]{\left| #1 \right|} \newcommand{\set}[1]{\left\{ #1 \right\}}
An isolated singular point a of single-valued character of an analytic function f(z) of the complex variable z for which \abs{f(z)} increases without bound when z approaches a: \lim_{z\rightarrow a} f(z) = \infty. In a sufficiently small punctured neighbourhood V=\set{z\in\C : 0 < \abs{z-a} < R} of the point a \neq \infty, or V'=\set{z\in\C : r < \abs{z} < \infty} in the case of the point at infinity a=\infty, the function f(z) can be written as a Laurent series of special form:
\begin{equation}
\label{eq1}
f(z) = \sum_{k=-m}^\infty c_k (z-a)^k,\quad
\text{$a \neq \infty$, $c_{-m} \neq 0$, $z \in V$},
\end{equation}
or, respectively,
\begin{equation}
\label{eq2}
f(z) = \sum_{k=-m}^\infty \frac{c_k}{z^k},\quad
\text{$a = \infty$, $c_{-m} \neq 0$, $z \in V'$},
\end{equation}
with finitely many negative exponents if a\neq\infty, or, respectively, finitely many positive exponents if a=\infty. The natural number m in these expressions is called the order, or multiplicity, of the pole a; when m=1 the pole is called simple. The expressions \ref{eq1} and \ref{eq2} show that the function p(z)=(z-a)^mf (z) if a\neq\infty, or p(z)=z^{-m}f(z) if a=\infty, can be [[Analytic continuation|analytically continued]] to a full neighbourhood of the pole a, and, moreover, p(a) \neq 0. Alternatively, a pole a of order m can also be characterized by the fact that the function 1/f(z) has a zero of multiplicity m at a.
A point a=(a_1,\ldots,a_n) of the complex space \C^n, n\geq2, is called a pole of the analytic function f(z) of several complex variables z=(z_1,\ldots,z_n) if the following conditions are satisfied: 1) f(z) is holomorphic everywhere in some neighbourhood U of a except at a set P \subset U, a \in P; 2) f(z) cannot be analytically continued to any point of P; and 3) there exists a function q(z) \not\equiv 0, holomorphic in U, such that the function p(z) = q(z)f(z), which is holomorphic in U \setminus P, can be holomorphically continued to the full neighbourhood U, and, moreover, p(a) \neq 0. Here also
'"UNIQ-MathJax1-QINU"'
however, for n \geq 2, poles, as with singular points in general, cannot be isolated.
===='"UNIQ--h-0--QINU"'References====
{|
|-
|valign="top"|<span id="Sh"></span>[Sh]||valign="top"| B.V. Shabat, "Introduction of complex analysis", '''2''', Moscow (1976) (In Russian)
|-
|}
===='"UNIQ--h-1--QINU"'Comments====
For n=1 see [[#Ah|[Ah]]]. For n \geq 2 see [GrFr], [Ra].
For the use of poles in the representation of analytic functions see Integral representation of an analytic function; Cauchy integral.
References
[Ah] | L.V. Ahlfors, "Complex analysis", McGraw-Hill (1979) pp. Chapt. 8 |
[GrFr] | H. Grauert, K. Fritzsche, "Several complex variables", Springer (1976) (Translated from German) |
[Ra] | R.M. Range, "Holomorphic functions and integral representation in several complex variables", Springer (1986) pp. Chapt. 1, Sect. 3 |
Pole (of a function). Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Pole_(of_a_function)&oldid=25727