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Natalie 24.4.2013
We first select a subsequence of $\mathbb{N}$ such that a point in the support $\chi_i$ of $v_{k_{i}}$ has limiting point $x_{\ast} \in \Omega$. This is possible since any bounded sequence in $\mathbb{R}$ has a convergent subsequence. We call it $k_{i}$ again.
Given $\epsilon>0$ there is $i>0$ such that $$
v_{k_{i}} - v_{\ast} |
$$ So we know that on the exterior of the support $\Omega_{k_{i}}$ of $v_{k_{i}}$ we have $$
v_{\ast} | _{L |
$$ For a function $v_{\ast} \in L^2(\Omega)$ we have that \begin{eqnarray}
\int_{\Omega_{k_{i}}} | v_{\ast}(y) | 2 dy |
---|
\left|\int_{\Omega} |v_{\ast}(y)|^2 |\chi_{k_{i}}(y)|^2 dy \right|
\nonumber
& \leq & ||v_{\ast}||_{L^2(\Omega)}^2 \cdot || \chi_{k_{i}} ||_{L^2(\Omega)}^2.
\end{eqnarray}
Now, we obtain
\begin{eqnarray}
v_{\ast} | _{L | 2(\Omega)} | {2} & = & | v_{\ast} | _{L | 2(\Omega \setminus \Omega_{k_{i}})} |
---|
+ ||v_{\ast}||_{L^2(\Omega_{k_{i}})}^2
\nonumber
& \rightarrow & 0, \;\; i \rightarrow \infty.
\end{eqnarray}
Natalie 9.5.2013
We use the series expansion $$ \frac{1}{x-y} = (-1) \sum_{n=1}^{\infty} \frac{x^n}{y^{n+1}} $$ for $|x|<|y|$, which I took from Wolfram.
For $|x|<\rho \cdot |y|$ with $\rho<1$ we have $$
\frac{x | n}{y | {n+1} | < \frac{1}{y} \rho |
---|
$$ such that $$
\sum_{n=1} | {\infty} \frac{x | n}{y | {n+1}} | < \frac{1}{ | y | } \sum_{n=1} | {\infty} \rho |
---|
$$ is absolutely convergent by the geometric series. Thus, $\frac{1}{x-y}$ is analytic on $|x|<|y|$. For $|x|>|y|$ we use $$ \frac{1}{x-y} = \sum_{n=1}^{\infty} \frac{y^n}{x^{n+1}} $$ analogously.