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victorballester7 committed Dec 26, 2023
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2 changes: 1 addition & 1 deletion Mathematics/4th/Dynamical_systems/Dynamical_systems.tex
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\begin{itemize}
\item {stable node} if $\lambda_1,\lambda_2\in\RR$ and $\abs{\lambda_1},\abs{\lambda_2}<1$.
\item {unstable node} if $\lambda_1,\lambda_2\in\RR$ and $\abs{\lambda_1},\abs{\lambda_2}>1$.
\item {saddle point} if $\lambda_1,\lambda_2\in\RR$ and $\abs{\lambda_1}<1$ and $\abs{\lambda_2}>1$ (or viceversa).
\item {saddle point} if $\lambda_1,\lambda_2\in\RR$ and $\abs{\lambda_1}<1$ and $\abs{\lambda_2}>1$ (or vice versa).
\item {stable focus} if $\lambda_1,\lambda_2\in\CC$ and $\abs{\lambda_1}<1$.
\item {unstable focus} if $\lambda_1,\lambda_2\in\CC$ and $\abs{\lambda_1}>1$.
\end{itemize}
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32 changes: 16 additions & 16 deletions Mathematics/4th/Stochastic_processes/Stochastic_processes.tex
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with $q_0=1$ and $q_a=0$, whose solution is straightforward.
\end{sproof}
\begin{proposition}
Consider the Gambler's ruin problem. Suppose that we play against another player (and so when we lose, he wins and viceversa). Let $p_z^*$, $q_z^*$ be the respective probabilities for the other player. Then:
Consider the Gambler's ruin problem. Suppose that we play against another player (and so when we lose, he wins and vice versa). Let $p_z^*$, $q_z^*$ be the respective probabilities for the other player. Then:
$$q_z+q_z^*=1$$
Hence, $D_z\almoste{<}\infty$.
\end{proposition}
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p_{ij}^{(n+1)} & =\Prob(X_{n+1}=j\mid X_0=i) \\
& =\sum_{k\in I}\Prob(X_{n+1}=j, X_n=k\mid X_0=i) \\
\begin{split}
& =\sum_{k\in I}\Prob(X_{n}=k\mid X_0=i)\cdot \\
& \hspace{2.5cm}\cdot\Prob(X_{n+1}=j\mid X_n=k, X_0=i)
\end{split} \\
& =\sum_{k\in I}\Prob(X_{n}=k\mid X_0=i)\cdot \\
& \hspace{2.5cm}\cdot\Prob(X_{n+1}=j\mid X_n=k, X_0=i)
\end{split} \\
& =\sum_{k\in I}p_{ik}^{(n)}p_{kj}^{(1)}
\end{align*}
where the penultimate equality follows from \mcref{SP:lema1Markov} and the last equality follows from \mcref{SP:lema2Markov} and the Markov property because if $D=\{X_n=k, X_0=i\}$ we have that:
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\begin{align*}
\begin{split}
p_\ell & =\Prob_i(X_{m_1+\cdots+m_\ell}=i,X_{m_1+\cdots+m_\ell-1}\ne i,\ldots, \\
& \hspace{4cm}X_{m_1+\cdots+m_{\ell-1}+1}\ne i\mid A)
& \hspace{4cm}X_{m_1+\cdots+m_{\ell-1}+1}\ne i\mid A)
\end{split} \\
& =\Prob_i(X_{m_\ell}=i,X_{m_\ell-1}\ne i,\ldots,X_{1}\mid X_{0}=i) \\
& =\Prob_i(X_{m_\ell}=i,X_{m_\ell-1}\ne i,\ldots,X_{1}\mid X_{0}=i) \\
& =\Prob(\tau_i=m_\ell)
\end{align*}
\end{proof}
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\begin{proof}
Note that $\{X_n=j\}\subseteq \{\tau_j\leq n\}=\bigsqcup_{m=1}^n\{\tau_j=m\}$. Hence, $\{X_n=j\}=\bigsqcup_{m=1}^n[\{X_n=j\}\cap \{\tau_j=m\}]$. Thus:
\begin{align*}
p_{ij}^{(n)} & =\Prob_i(X_n=j) \\
& =\sum_{m=1}^n \Prob_i(X_n=j,\tau_j=m) \\
& =\sum_{m=1}^n \Prob_i(X_n=j\mid\tau_j=m)\Prob_i(\tau_j=m) \\
p_{ij}^{(n)} & =\Prob_i(X_n=j) \\
& =\sum_{m=1}^n \Prob_i(X_n=j,\tau_j=m) \\
& =\sum_{m=1}^n \Prob_i(X_n=j\mid\tau_j=m)\Prob_i(\tau_j=m) \\
\begin{split}
& =\sum_{m=1}^n \Prob_i(X_n=j\mid X_m=j,X_{m-1}\ne j,\ldots, X_1\ne j)\cdot \\
& \hspace{7cm}\cdot f_{ij}^{(m)}
& =\sum_{m=1}^n \Prob_i(X_n=j\mid X_m=j,X_{m-1}\ne j,\ldots, X_1\ne j)\cdot \\
& \hspace{7cm}\cdot f_{ij}^{(m)}
\end{split} \\
& =\sum_{m=1}^n \Prob_j(X_{n-m}=j)f_{ij}^{(m)} \\
& =\sum_{m=1}^n \Prob_j(X_{n-m}=j)f_{ij}^{(m)} \\
& =\sum_{m=1}^nf_{ij}^{(m)}p_{jj}^{(n-m)}
\end{align*}
\end{proof}
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\begin{align*}
p_{ij}(t+s) & =\sum_{k\in I} \Prob(X_{t+s}=j,X_s=k\mid X_0=i) \\
\begin{split}
& =\sum_{k\in I} \Prob(X_{t+s}=j\mid X_s=k,X_0=i)\cdot \\
& \hspace{3.5cm}\cdot\Prob(X_s=k\mid X_0=i) \\
\end{split} \\
& =\sum_{k\in I} \Prob(X_{t+s}=j\mid X_s=k,X_0=i)\cdot \\
& \hspace{3.5cm}\cdot\Prob(X_s=k\mid X_0=i) \\
\end{split} \\
& =\sum_{k\in I} p_{ik}(t)p_{kj}(s)
\end{align*}
\end{proof}
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\end{enumerate}
\end{proposition}
\begin{definition}
Let ${(X_t)}_{t\in T}$ and ${(Y_t)}_{t\in T}$ be two stochastic processes. We say that ${(X_t)}_{t\in T}$ and ${(Y_t)}_{t\in T}$ are \emph{stochastically equivalent} if $\forall t\in T$ we have: $$\Prob(X_t=Y_t)=1$$ In that case we also say that ${(X_t)}_{t\in T}$ is a \emph{version} of ${(Y_t)}_{t\in T}$ (or viceversa). We say that ${(X_t)}_{t\in T}$ and ${(Y_t)}_{t\in T}$ are \emph{indistinguishable} if: $$
Let ${(X_t)}_{t\in T}$ and ${(Y_t)}_{t\in T}$ be two stochastic processes. We say that ${(X_t)}_{t\in T}$ and ${(Y_t)}_{t\in T}$ are \emph{stochastically equivalent} if $\forall t\in T$ we have: $$\Prob(X_t=Y_t)=1$$ In that case we also say that ${(X_t)}_{t\in T}$ is a \emph{version} of ${(Y_t)}_{t\in T}$ (or vice versa). We say that ${(X_t)}_{t\in T}$ and ${(Y_t)}_{t\in T}$ are \emph{indistinguishable} if: $$
\Prob(X_t=Y_t\ \forall t\in T)=1
$$
\end{definition}
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$$
By density, it is enough to prove the result for $u\in \mathcal{C}^1(\RR_{\geq 0})$. An easy check shows that $\bar{u}\in \mathcal{C}^1(\RR)$. Moreover, we have:
\begin{align*}
{\norm{\bar{u}}_{W^{1,p}(\RR)}}^p & =\int_{\RR}{\abs{\bar{u}}^p}+{\abs{\bar{u}'}^p} \\
{\norm{\bar{u}}_{W^{1,p}(\RR)}}^p & =\int_{\RR}{\abs{\bar{u}}^p}+{\abs{\bar{u}'}^p} \\
\begin{split}
& =\!\int_{\RR_{\geq 0}}\!{\abs{u}^p}\!+\!\!{\abs{u'}^p}\!+\!\int_{\RR_{\leq 0}}\![{\abs{-3u(-x)+4u(-x/2)}^p}+ \\
& \hspace{2.75cm}+{\abs{3u'(-x)-2u'(-x/2)}^p}]
& =\!\int_{\RR_{\geq 0}}\!{\abs{u}^p}\!+\!\!{\abs{u'}^p}\!+\!\int_{\RR_{\leq 0}}\![{\abs{-3u(-x)+4u(-x/2)}^p}+ \\
& \hspace{2.75cm}+{\abs{3u'(-x)-2u'(-x/2)}^p}]
\end{split} \\
& \leq C{\norm{u}_{W^{1,p}(\RR_{\geq 0})}}^p
\end{align*}
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where we have assumed that the boundary of $\Omega$ is smooth enough to define the normal vector $\vf{n}$. The condition is called \emph{homogeneous} if $g=0$. Note that if $\vf{A}=\vf{I}_d$, then the Neumann boundary condition is just $\partial_{\vf{n}} u=g$.
\end{definition}
\begin{remark}
If the coefficients $a_{ij}\in\mathcal{C}^1$, then we convert the equation from non-divergence form to divergence form and viceversa.
If the coefficients $a_{ij}\in\mathcal{C}^1$, then we are able to convert the equation from non-divergence form to divergence form and vice versa.
\end{remark}
\begin{definition}
Let $a_{ij},b_j,c$ be known functions on $\Omega\subseteq \RR^d$. We say that the operator
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Let $H$ be Hilbert and $K:H\to H$ be a compact linear operator. Then, $\dim \ker(\id-K)<\infty$.
\end{lemma}
\begin{proof}
We first prove that $\dim\ker(\id-K)<\infty$. If $\dim\ker(\id-K)=\infty$, then $\exists (u_n)\in \ker(\id-K)$ orthonormal, and thus bounded. In particular, $u_n=Ku_n$ and since $K$ is compact, we have that $(Ku_n)$ has a convergent subsequence. But:
If $\dim\ker(\id-K)=\infty$, then $\exists (u_n)\in \ker(\id-K)$ orthonormal, and thus bounded. In particular, $u_n=Ku_n$ and since $K$ is compact, we have that $(Ku_n)$ has a convergent subsequence. But:
\begin{align*}
0 & =\lim_{k\to\infty}\norm{Ku_{n_k}-Ku_{n_{k+1}}}^2 \\
& =\lim_{k\to\infty}\norm{u_{n_k}-u_{n_{k+1}}}^2 \\
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Let $H$ be Hilbert and $K:H\to H$ be a compact linear operator. Then, $\im(\id-K)$ is closed.
\end{lemma}
\begin{proof}
Let $(v_n)\in \im(\id-K)$ be such that $v_n\to v\in H$. Then, $\exists (u_n)\in H$ such that $v_n=(\id-K)u_n$. Thanks to \mnameref{RFA:projection}, we can write $u_n=u_n^{\text{ker}}+ u_n^{\text{ker}^\perp}$, where $u_n^{\text{ker}}\in \ker(\id-K)$ and $u_n^{\text{ker}^\perp}\in {\ker(\id-K)}^{\perp}$. Thus, $v_n=(\id-K)u_n^{\text{ker}^\perp}$ and by \mcref{INEPDE:lemma2_fredholm}, we have:
Let $(v_n)\in \im(\id-K)$ be such that $v_n\to v\in H$. Then, $\exists (u_n)\in H$ such that $v_n=(\id-K)u_n$. By \mnameref{RFA:projection}, we can write $u_n=u_n^{\text{ker}}+ u_n^{\text{ker}^\perp}$, where $u_n^{\text{ker}}\in \ker(\id-K)$ and $u_n^{\text{ker}^\perp}\in {\ker(\id-K)}^{\perp}$. Thus, $v_n=(\id-K)u_n^{\text{ker}^\perp}$ and by \mcref{INEPDE:lemma2_fredholm}, we have:
$$
\norm{v_n-v_m}\geq c\norm{u_n^{\text{ker}^\perp}-u_m^{\text{ker}^\perp}}
$$
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