Note that this result does not depend on $\alpha$.
Friday, 5 June 2015
Holder Spaces
The space $C(\bar{\Omega})$
Note that we have convergence $f_n$ to $f$ in sup norm. (Just take the limit $m \to \infty$ in the cauchy criterion). It remains to show that $f$ is a bounded continuous function on $\bar{\Omega}$. \[\sup_x|f(x)| \leq \sup_x|f(x) - f_n(x)| + \sup_x|f_n(x)|\] For large enough $n$ the first term on the r.h.s can be made small and second term is finite as $f_n$ is bounded. Therefore $f$ is bounded.
As for continuity, we have \[|f(x)-f(y)| \leq |f(x)-f_n(x)| + |f_n(x)-f_m(x)| + |f_m(x)-f_m(y)| + |f_m(y)-f(y)|\] The first, second and the fourth terms can be made small by choosing large enough $n,m$ independent of $x,y$. The third term can be made arbitrarily small by choosing $y$ sufficiently close to $x$ due to the continuity of $f_m$.
Thursday, 4 June 2015
Taylor's Theorem
Monday, 1 December 2014
$C^k$ Space
Let $\Omega \subset \mathbb{R}^d$ be an open set and $C^k(\bar{\Omega})$ be the set of all bounded functions $u : \Omega \to \mathbb{R}$ whose partial derivatives $D^a u$ for $0 \leq |a| \leq k$ are continuous on $\Omega$ and can be continuously extended to $\bar{\Omega}$ in a bounded way. (Here $D^a u$ represents partial derivative where $a=(a_1,a_2,\cdots,a_d)$ is a multi-index). Define a norm on $C^k(\bar{\Omega})$ by $\|u\|_{C^k} = \underset{0 \leq |a| \leq k}{\max} \underset{x \in \bar{\Omega}} \sup|D^au(x)|$. Then $(C^k(\bar{\Omega}),\|\cdot\|_{C^k})$ is a Banach Space.
Note that $\Omega$ can be unbounded here. The norm is still meaningful as the functions themselves are bounded. The following Mean-Value theorem in higher dimensions is used in the proof. Let $f : \Omega \to \mathbb{R}$ be differentiable (e.g. all partial derivatives of $f$ are continuous). Take two points $x,y\in \Omega$ and assume that the line joining the two points is also contained in $\Omega$. Define $g : [0,1] \to \mathbb{R}$ by $g(t) = f((1-t)x+ty)$. Now, clearly $g$ is differentiable and hence by the Mean Value Theorem, $g(1) - g(0) = g^\prime(c)$ where $c\in (0,1)$. Hence, $f(y) - f(x) = \langle \nabla f((1-c)x+cy),(y-x)\rangle$.
Assume now that $\{u_n\}$ is a cauchy-sequence and let $0 \leq |a| < k$. Also, let $\lim_{n\to \infty} u_n = v^0$. This limit exists and belongs to $C(\bar{\Omega})$. Similarly, let $\lim_{n\to \infty} D^au_n = v^a$. We need to show that $D^av^0 = v^a$.
As $\{u_n\}$ is cauchy, for a given $\epsilon > 0$, there exists $N$ such that $\underset{x \in \bar{\Omega}} \sup |\frac{\partial}{\partial x_i} D^a u_n (x) - \frac{\partial}{\partial x_i} D^a u_m (x)| < \epsilon$ for all $m,n \geq N$. Choose $f = D^au_n - D^au_m : \Omega \to \mathbb{R}$ in the previous paragraph. Then \begin{array} a\frac{\|(D^au_n(y) - D^au_m(y)) - (D^au_n(x) - D^au_m(x))\|}{\|y - x\|} &\leq \|\nabla f((1-c)x+cy)\| \\ &\leq \epsilon \sqrt{d} \end{array}
Now let $x\in \Omega$ and $\phi_n^i : \Omega_i \to \mathbb{R}$ given by $\phi_n^i(y) = \frac{\|D^au_n(x_1,x_2,\cdots,x_{i-1},y,x_{i+1},\cdots,x_d)- D^au_n(x_1,x_2,\cdots,x_{i-1},x_i,x_{i+1},\cdots,x_d)\|} {|y - x_i|}$. Here $\Omega_i \subset \mathbb{R}$ is an open ball around $x_i$ minus the point $x_i$ From the above we get that $\phi_n^i$ is uniformly-cauchy and hence converges uniformly in $\Omega_i$. Let $\lim_{n\to\infty} \phi_n^i(y)= \phi^i(y)$ in $\Omega_i$. Then, $\lim_{y \to x_i}\lim_{n \to \infty} \phi_n^i(y)= \lim_{n \to \infty} \lim_{y \to x_i} \phi_n^i(y)$ (i.e. the limits can be interchanged because of uniform convergence, see Rudin's PrinMathAnalysis Theorem 7.11) if $\lim_{y \to x_i} \phi_n^i(y)$ exists. In this case, this is true. Let $b=(a_1,a_2,\cdots,a_i+1,\cdots,a_n)$, then we get using recursion, \[D^bu(x)= \lim_{n\to \infty} D^{b}u_n(x)\]
Thursday, 27 November 2014
Ascoli-Arzela Theorem
- Equicontinuity : For each $\epsilon > 0$, for all $x\in X$, there exists a neighbourhood $U_x$ such that $\|f(y) - f(x)\| < \epsilon$ for all $y \in U_x$ and all $f \in F$
- Pointwise Boundedness : For each $x\in X$, $\sup\{\|f(x)\| : f \in F\} < \infty$
Let $\epsilon_n = \frac{1}{2^n}$. For each $x$, choose $U_x$ (from the equicontinuity of $\mathcal{F}$) such that the oscillation of any function in $\mathcal{F}$ is less than $\epsilon_1$. As $U_x$ form an open cover of $X$ and since $X$ is compact there exists a finite subcover which covers $X$. Denote this cover by $U_{x_{11}},U_{x_{12}},\cdots,U_{x_{1N_1}}$. With this process, we obtain for every $n$ a finite open cover $U_{x_{n1}},U_{x_{n2}},\cdots,U_{x_{nN_n}}$.
Rename the points $x_{11},x_{12},\cdots,x_{1N_1},x_{21}\cdots,x_{2N_2}\cdots$ as $x_1,x_2,\cdots$
Let $\{f_n\}$ be a sequence in $\mathcal{F}$. We want to show that there exists a sub-sequence which converges uniformly. As the space $\bar{\mathcal{F}}$ is a metric space (with the metric mentioned above) we get that it is compact.Step 1 : As $\{\|f_n(x_1)\|\}$ is bounded, there exists a sub-sequence $\{f_{n_1}\}$ such that $f_{n_1}(x_1)$ converges. Now, we can choose a sub-sequence $f_{n_2}$ of $f_{n_1}$ such that $f_{n_2}(x_2)$ converges. This process is repeated ad-infinitum. Now, the "diagonal" sequence whose $m$th term is $m$th term in the $m$th subsequence $f_{n_m}$ is chosen and denoted by $f_m$. By construction, $f_m(x_i)$ converges for all $i$. This seems to be the central idea. For the next steps fix $l$.
Step 2: From the above, we know that for each $x_k$, there exists an integer $N(\epsilon,x_k)$ such that $\|f_n(x_k) - f_m(x_k)| < \epsilon_l$ for all $n,m > N(\epsilon_l,x_k)$.
Step 3 : Clearly, for $K=\sum_{i=1}^l N_i$ each open set $U_{lj}$, $1 \leq j \leq N_l$, contains at-least one point $x_k$ with $1 \leq k \leq K$
Step 4: For any $x \in X$, there exist $j,k$ such that $x \in U_{lj}, x_k \in U_{lj}$ where $1 \leq j \leq N_l$. For this $k$, \[\|f_n(x) - f_m(x)\| \leq \|f_n(x)-f_n(x_k)\| + \|f_n(x_k) - f_m(x_k)\| + \|f_m(x_k) - f_m(x)\| < 3\epsilon_l\] for all $n,m > \max(N(\epsilon,x_1),N(\epsilon,x_2),\cdots,N(\epsilon,x_K))$. Therefore, the sequence is uniformly-cauchy and hence converges to a continuous function $g \in C(X;\mathbb{R}^n)$. It is obvious that $g \in \bar{\mathcal{F}}$