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<record version="14" id="6655">
 <title>regularity theorem for the Laplace equation</title>
 <name>RegularityTheoremForTheLaplaceEquation</name>
 <created>2005-01-21 02:20:07</created>
 <modified>2007-06-02 23:07:10</modified>
 <type>Theorem</type>
<parent id="3593">Laplace equation</parent>
 <creator id="6075" name="rspuzio"/>
 <author id="13753" name="Mathprof"/>
 <author id="6075" name="rspuzio"/>
 <classification>
	<category scheme="msc" code="26B12"/>
 </classification>
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 <content>{\bf Warning: This entry is still in the process of being written, hence is not yet \PMlinkescapetext{complete}.}

Let $D$ be an open subset of $\mathbb{R}^n$.  Suppose that $f \colon D \to \mathbb{R}$ is twice differentiable and satisfies Laplace's equation.  Then $f$ has derivatives of all orders and is, in fact analytic.

{\it Proof: \,}  Let ${\bf p}$ be any point of $D$.  We shall show that $f$ is analytic at ${\bf p}$.  Since $D$ is an open set, there must exist a real number $r &gt; 0$ such that the closed ball of radius $r$ about ${\bf p}$ lies inside of $D$.

Since $f$ satisfies Laplace's equation, we can express the value of $f$ inside this ball in terms of its values on the boundary of the ball by using Poisson's formula:
 $$f({\bf x}) = {1 \over r^{n-1} A(n-1)} \int_{|{\bf y} - p| = r} f({\bf y}) {r^2 - |{\bf x} - {\bf p}|^2 \over |{\bf x} - {\bf y}|^n} \, d\Omega({\bf y})$$
Here, $A(k)$ denotes the \PMlinkid{area of the $k$-dimensional sphere}{4495} and $d\Omega$ denotes the measure on the sphere of radius $r$ about ${\bf p}$.

We shall show that $f$ is analytic by deriving a convergent power series for $f$.  From this, it will automatically follow that $f$ has derivatives of all orders, so a separate proof of this fact will not be necessary.  

Since this involves manipulating power series in several variables, we shall make use of multi-index notation to keep the equations from becoming unnecessarily complicated and drowning in a plethora of indices.

First, note that since $f$ is assumed to be twice differentiable in $D$, it is continuous in $D$ and, hence, since the sphere of radius $r$ about $s$ is compact, it attains a maximum on this sphere.  Let us denote this maxmum by $M$.  Next, let us consider the quantity
 $${1 \over |{\bf x} - {\bf y}|^n}$$
which appears in the integral.  We may write this quantity more explicitly as
 $$\left( |{\bf y} - {\bf p}|^2 - 2 ({\bf x} - {\bf p}) \cdot ({\bf y} - {\bf p}) + |{\bf x} - {\bf p}|^2 \right)^{-{n \over 2}}.$$
Since the values of the variable $y$ has been restricted by the condition $|{\bf y} - {\bf p}| = r$, we may rewrite this as
 $${1 \over r^n} \left( 1 + {- 2({\bf x} - {\bf p}) \cdot ({\bf y} - {\bf p}) + |{\bf x} - {\bf p}|^2 \over r^2} \right)^{-{n \over 2}}.$$

Assume that $|{\bf x} - {\bf p}| &lt; r/4$.  Then we have 
 $$\left| {- 2({\bf x} - {\bf p}) \cdot ({\bf y} - {\bf p}) + |{\bf x} - {\bf p}|^2 \over r^2} \right| \le {2 |({\bf x} - {\bf p}) \cdot ({\bf y} - {\bf p})| \over r^2} + {|{\bf x} - {\bf p}|^2 \over r^2} \le $$ 
$${2 |{\bf x} - {\bf p}| \&gt; |{\bf y} - {\bf p}| \over r^2} + \left( {|{\bf x} - {\bf p}| \over r} \right)^2 \le 2 \cdot {1 \over 4} + \left( {1 \over 4} \right)^2 = {9 \over 16} &lt; 1.$$

Since this absolute value is less than one, we may apply the binomial theorem to obtain the series
 $${1 \over |{\bf x} - {\bf y}|^n} = {1 \over r^n} \left( 1 + {- 2({\bf x} - {\bf p}) \cdot ({\bf y} - {\bf p}) + |{\bf x} - {\bf p}|^2 \over r^2} \right)^{n \over 2} = $$
$$\sum_{m = 0}^\infty {\left( {n \over 2} \right)^{\underline{m}} \over m!}  \left( {- 2({\bf x} - {\bf p}) \cdot ({\bf y} - {\bf p}) + |{\bf x} - {\bf p}|^2 \over r^2} \right)^m$$

Note that each term in this sum is a polynomial in $x-p$.  The powers of the various components of $x-p$ that appear in the $m$-th term range between $m$ and $2m$.  Moreover, let us note that we can strengthen the assertion used to show that the binomial series converged by inserting absolute value bars.  If we write
 $${- 2(x - p) \cdot (y - p) + |x - p|^2 \over r^2} = \sum_{k = 0}^n c_k (y) \&gt; (x - p)_k + \sum_{k_1, k_2 = 0}^n c_{k_1 k_2} (y) \&gt; (x - p)_{k_1} (x - p)_{k_2},$$
(actually, the coefficients $c_{k_1 k_2}$ depend on $y$ trivially, but the dependence on $y$ has been indicated for the sake of uniformity) then
 $$\sum_{k = 0}^n |c_k (y)| \&gt; |(x - p)_k| + \sum_{k_1, k_2 = 0}^n |c_{k_1 k_2} (y)| \&gt; |(x - p)_{k_1}| \&gt; |(x - p)_{k_2}| \le {9 \over 16}.$$
Raising this to the $m$-th power, we see that, if we define
 $$\left( {- 2(x - p) \cdot (y - p) + |x - p|^2 \over r^2} \right)^m = \sum_{k_1, k_2, \ldots, k_m = 0}^n c_{k_1 k_2, \cdots k_m} (y) (x - p)_{k_1} (x - p)_{k_2} \cdots (x - p)_{k_m},$$
then we have
 $$\sum_{k_1, k_2, \ldots, k_m = 0}^n |c_{k_1 k_2, \cdots k_m} (y)| \&gt; |(x - p)_{k_1}| \&gt; |(x - p)_{k_2}| \cdots |(x - p)_{k_m}| \le \left( {9 \over 16} \right)^m$$
Because of the fact that one may freely rearrange and regroup the terms in an absolutely convegent series, we may conclude that the expansion of $|x - y|^{-n}$ in powers of $x - p$ converges absolutely.  Furthermore, there exist constants $b_{k_1 k_2, \cdots k_m}$ such that the term involving $|(x - p)_{k_1}| \&gt; |(x - p)_{k_2}| \cdots |(x - p)_{k_m}|$ in the power series is bounded by $b_{k_1 k_2, \cdots k_m}$.</content>
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