-
Notifications
You must be signed in to change notification settings - Fork 3
Expand file tree
/
Copy path30B10-SeriesInversion.tex
More file actions
142 lines (124 loc) · 5.19 KB
/
30B10-SeriesInversion.tex
File metadata and controls
142 lines (124 loc) · 5.19 KB
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
51
52
53
54
55
56
57
58
59
60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84
85
86
87
88
89
90
91
92
93
94
95
96
97
98
99
100
101
102
103
104
105
106
107
108
109
110
111
112
113
114
115
116
117
118
119
120
121
122
123
124
125
126
127
128
129
130
131
132
133
134
135
136
137
138
139
140
141
142
\documentclass[12pt]{article}
\usepackage{pmmeta}
\pmcanonicalname{SeriesInversion}
\pmcreated{2013-03-22 15:39:09}
\pmmodified{2013-03-22 15:39:09}
\pmowner{stevecheng}{10074}
\pmmodifier{stevecheng}{10074}
\pmtitle{series inversion}
\pmrecord{8}{37585}
\pmprivacy{1}
\pmauthor{stevecheng}{10074}
\pmtype{Derivation}
\pmcomment{trigger rebuild}
\pmclassification{msc}{30B10}
\endmetadata
\usepackage{amssymb}
\usepackage{amsmath}
\usepackage{amsfonts}
\begin{document}
The method of \emph{series inversion} allows us to derive the power series
of an inverse function $f^{-1}$ given the power series of $f$.
Clearly, since we are representing function $f$ and $f^{-1}$ by power series,
the function $f$ must necessarily be holomorphic; that is, it is differentiable
as a complex-valued function on an open subset of the complex plane.
(It follows that $f^{-1}$ must also be holomorphic.)
Holomorphic functions include the elementary functions studied in calculus
such as $\sin$, $\cos$, $\tan$ and $\exp$.
For the method to work smoothly, it is best to assume that we want
to invert $f$ at around the origin, and its value there is zero.
There is no loss of generality, since
if $f(b) = a$, we can apply series inversion to the function $g$ defined
by $f(z) = a + g(z-b)$.
Then $f^{-1}(w) = g^{-1}(w-a) + b$;
we obtain the power series for $f^{-1}$ centred at $a$.
Also, it must be true that $f'(0) \neq 0$, otherwise $f$ will not even
be invertible around the origin.
\section*{An example}
We explain the method by an example, for $f(z) = \arctan z$.
In the following, we will consistently use the notation $O(z^n)$
to denote a holomorphic function $h(z)$ whose power series expansion begins
with $z^n$. And similarly when $z$ is replaced with the variable $w$.
First, we start with the well-known power series expansion for $w = \arctan z$:
\begin{equation}
\label{eq:arctan}
w = z - \frac{z^3}{3} + \frac{z^5}{5} + O(z^7)\,.
\end{equation}
The number of explicit terms in the power series expansion determines
the number of terms that we will be able to obtain
in the power series expansion of $f^{-1}$.
So in this case, we are going to seek an expansion
of $f^{-1}(w) = \tan w$ up to (but excluding) the $w^7$ term.
A simple rearrangement of \eqref{eq:arctan} gives
\begin{equation}
\label{eq:z}
z = w + \frac{z^3}{3} - \frac{z^5}{5} + O(z^7)
\end{equation}
Now we \emph{substitute equation \eqref{eq:z} into itself}.
Of course, usually when we substitute an equation into itself
we do not get anything, but here it works because we can
\emph{perform simplications using the $O$ notation}.
So for instance, in the following,
in second term $z^3/3$ on the right of equation \eqref{eq:z}, we put in
equation \eqref{eq:z} simplified to $z = w + O(z^3)$.
Why we should choose this simplication will be clear in a moment:
\begin{align}
\label{eq:z3}
z &= w + \frac{1}{3} \Bigl( w + O(z^3) \Bigr)^3 - \frac{z^5}{5} + O(z^7) \\
&= w + \frac{1}{3} \Bigl( w^3 + O(z^3) (w^2 + \dotsb) \Bigr) - \frac{z^5}{5} + O(z^7) \\
\label{eq:Ow3}
&= w + \frac{1}{3} \Bigl( w^3 + O(w^3) \cdot O(w^2) \Bigr) + O(w^5)\,.
\end{align}
In equation \eqref{eq:Ow3} we used the fact that the expansion
for $z = f^{-1}(w)$ \emph{must begin} with a $w$ term, i.e.
$f^{-1}(0) = 0$. Also note that we are guaranteed that the $w$ and $z$ terms
have non-zero coefficients, because $f'(0) \neq 0$. (Otherwise
we would not be able to isolate $z$ in equation \eqref{eq:z}.)
Now equation \eqref{eq:Ow3} simplifies to
\begin{equation}
\label{eq:Ow5}
z = w + \frac{w^3}{3} + O(w^5)\,,
\end{equation}
which is already an achievement, because we have identified
exactly what the $w^3$ term must be.
We substitute \eqref{eq:Ow5} into the $z^3$ and $z^5$ terms of \eqref{eq:z},
and obtain:
\begin{align}
z &= w + \frac{1}{3} \left( w + \frac{w^3}{3} + O(w^5) \right)^3 - \frac{1}{5} \left( w + \frac{w^3}{3} + O(w^5) \right)^5 + O(z^7) \\
&= w + \frac{1}{3} \left( w^3 + \binom{3}{1} \frac{w^3}{3} w^2 + O(w^7) \right) - \frac{1}{5} \left( w^5 + O(w^7) \right) + O(w^7) \\
&= w + \frac{1}{3} w^3 + \frac{2}{15} w^5 + O(w^7)\,.
\end{align}
And this gives our desired expansion of $z = \tan w$
of degree $<7$.
\section*{Summary}
To summarize the procedure in general,
we start with the expansion
\begin{equation}
\label{eq:f}
w = f(z) = a_1 z + a_2 z^2 + a_3 z^3 + \dotsb \,, \quad a_1 \neq 0\,,
\end{equation}
and rearrange it to,
\begin{equation}
\label{eq:z-general}
z = b_1 \Bigl( w - a_2 z^2 - a_3 z^3 - \dotsb - a_n z^n \Bigr) + O(w^{n+1})\,, \quad b_1 = \frac{1}{a_1}\,.
\end{equation}
So we know that $z = b_1 w + O(w^2)$,
and we can substitute
this into the term $z^2$ of equation \eqref{eq:z-general}.
At the end we will get an equation of the form
$z = b_1 w + b_2 w^2 + O(w^3)$, and we can substitute this
into the terms $z^2$ and $z^3$ of \eqref{eq:z-general}.
And what ever results we will substitute back into the
terms $z^2$, $z^3$, $z^4$ of equation \eqref{eq:z-general}.
We can repeat this process until
we have all the terms of $z = f^{-1}(w)$ that we need.
We probably should normalize
the functions so that $a_1 = b_1 = 1$
to make the computations easier.
\begin{thebibliography}{XXXXX}
\bibitem{Ahlfors}
Lars V. Ahlfors. {\it Complex Analysis}. McGraw-Hill, 1979.
\end{thebibliography}
%%%%%
%%%%%
\end{document}