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\newcommand{\widevec}{\overrightarrow} \newcommand{\darr}{\downarrow} \newcommand{\nearr}{\nearrow} \newcommand{\nwarr}{\nwarrow} \newcommand{\searr}{\searrow} \newcommand{\swarr}{\swarrow} \newcommand{\curvearrowbotright}{\curvearrowright} \newcommand{\uparr}{\uparrow} \newcommand{\downuparrow}{\updownarrow} \newcommand{\duparr}{\updownarrow} \newcommand{\updarr}{\updownarrow} \newcommand{\gt}{>} \newcommand{\lt}{<} \newcommand{\map}{\mapsto} \newcommand{\embedsin}{\hookrightarrow} \newcommand{\Alpha}{A} \newcommand{\Beta}{B} \newcommand{\Zeta}{Z} \newcommand{\Eta}{H} \newcommand{\Iota}{I} \newcommand{\Kappa}{K} \newcommand{\Mu}{M} \newcommand{\Nu}{N} \newcommand{\Rho}{P} \newcommand{\Tau}{T} \newcommand{\Upsi}{\Upsilon} \newcommand{\omicron}{o} \newcommand{\lang}{\langle} \newcommand{\rang}{\rangle} \newcommand{\Union}{\bigcup} \newcommand{\Intersection}{\bigcap} \newcommand{\Oplus}{\bigoplus} \newcommand{\Otimes}{\bigotimes} \newcommand{\Wedge}{\bigwedge} \newcommand{\Vee}{\bigvee} \newcommand{\coproduct}{\coprod} \newcommand{\product}{\prod} \newcommand{\closure}{\overline} \newcommand{\integral}{\int} \newcommand{\doubleintegral}{\iint} \newcommand{\tripleintegral}{\iiint} \newcommand{\quadrupleintegral}{\iiiint} \newcommand{\conint}{\oint} \newcommand{\contourintegral}{\oint} \newcommand{\infinity}{\infty} \newcommand{\bottom}{\bot} \newcommand{\minusb}{\boxminus} \newcommand{\plusb}{\boxplus} \newcommand{\timesb}{\boxtimes} \newcommand{\intersection}{\cap} \newcommand{\union}{\cup} \newcommand{\Del}{\nabla} \newcommand{\odash}{\circleddash} \newcommand{\negspace}{\!} \newcommand{\widebar}{\overline} \newcommand{\textsize}{\normalsize} \renewcommand{\scriptsize}{\scriptstyle} \newcommand{\scriptscriptsize}{\scriptscriptstyle} \newcommand{\mathfr}{\mathfrak} \newcommand{\statusline}[2]{#2} \newcommand{\tooltip}[2]{#2} \newcommand{\toggle}[2]{#2} % Theorem Environments \theoremstyle{plain} \newtheorem{theorem}{Theorem} \newtheorem{lemma}{Lemma} \newtheorem{prop}{Proposition} \newtheorem{cor}{Corollary} \newtheorem*{utheorem}{Theorem} \newtheorem*{ulemma}{Lemma} \newtheorem*{uprop}{Proposition} \newtheorem*{ucor}{Corollary} \theoremstyle{definition} \newtheorem{defn}{Definition} \newtheorem{example}{Example} \newtheorem*{udefn}{Definition} \newtheorem*{uexample}{Example} \theoremstyle{remark} \newtheorem{remark}{Remark} \newtheorem{note}{Note} \newtheorem*{uremark}{Remark} \newtheorem*{unote}{Note} %------------------------------------------------------------------- \begin{document} %------------------------------------------------------------------- \section*{rough paths} $\backslash$tableofcontents $\backslash$section\{Idea\} Rough Paths are a way of defining [[Stieltjes integral|Riemann-Stieltjes type integrals]] for paths with poor $p$-variation where Ito techniques don't work in the context of solving controlled [[differential equations]]. $\backslash$section\{Set-Up\} We want to solve differential equations of the form: \begin{displaymath} y_t=y_0+\int_0^t V(y_s)\otimes dX_s \end{displaymath} where $V=(V_1,...,V_d)$ with $V_i\in C_b^\infty(\mathbb{R}^d,\mathbb{R}^d)$ smooth bounded vector fields and $X\in C^p([0,T],\mathbb{R}^d)=\{f\colon \|f\|_{p-var}\colon = (\sup_{\mathcal{P}} |f_t-f_s|^p)^{1/p}\lt \infty\}$ is a signal with finite $p$ variation. We want to solve this by a fixed point argument/Picard iteration. That means we must define: \begin{displaymath} \int_0^t f(X_s)\otimes dX_s \end{displaymath} for smooth bounded $f$. The classical paper (\hyperlink{Young36}{Young 1936}) says, in short, that one can define this integral as a Riemann-Stieltjes integral iff $p\lt 2$. A theorem by Bichdeller-Dellecherie says, in short, that one can define this [[Itô integral|integral in Itô sense]] if and only if $X$ is a [[semimartingale]]. $\backslash$section\{Main Result\} Given a sequence of partitions, $\mathcal{P}_n=\{0=t_0\lt...\lt t_{n-1}\lt t\}$, if one can define $X^1_{su}\colon = \int_s^u dX_{r_1}$, $X^2_{su}\colon =\int_s^u\int_s^{r_2} dX_{r_1}\otimes dX_{r_2}$,\ldots{}, $X^\ell_{su}\colon =\int_s^u \int_s^{r_\ell}...\int_s^{r_2} dX_{r_1}\otimes...\otimes dX_{r_\ell}$ where $\ell=\lfloor p \rfloor$ for $s,u\in[0,t]$ then the following ``corrected Riemann sum'' converges almost surely as is called the rough integral: \begin{displaymath} \lim_{n\to\infty}\sum_{k=0}^{n} f(X_{t_k} )X^1_{t_k t_{k+1}}+Df(X_{t_k})X^2_{t_k t_{k+1}}+...+D^{\ell-1}f(X_{t_k})X^{\ell}_{t_k t_{k+1}}\colon = \int_0^t f(X_S)\otimes d\mathbf{X}_s \end{displaymath} The collection $\mathbf{X}=(X^1,...,X^\ell)$ is called a rough path of order $\ell$. We say that $(f(X),Df(X),...,D^{\ell-1}f(X))$ is controlled by $\mathbf{X}$. $\backslash$section\{Example\} Fractional Brownian motion (fBm), $B_t$, is a centered, continuous Gaussian process with covariance \begin{displaymath} E(B_t B_s)=\frac{1}{2}\left(t^{2H}+s^{2H}-|t-s|^{2H}\right) \end{displaymath} where $H\in(0,1)$ is called the Hurst parameter. When $H=1/2$ we recover regular [[Brownian motion]]. We have that $B_t\in C^p$ iff $p\gt 1/H$ and that fBm is not a semimartingale unless $H=1/2$. So SDEs driven by fBm with $H\lt 1/2$ are not solvable by classical means and rough paths must be used. $\backslash$section\{References\} \begin{itemize}% \item LC Young, \emph{An inequality of the Hölder type, connected with Stieltjes integration}, Acta Math. \textbf{67} (1936), 251--282. doi:\href{https://doi.org/10.1007/BF02401743}{10.1007/BF02401743}, (\href{https://projecteuclid.org/euclid.acta/1485888152}{Project Euclid}). \item Peter Friz and [[Martin Hairer]], A Course on Rough Paths, (2014), doi:\href{https://doi.org/10.1007/978-3-319-08332-2}{10.1007/978-3-319-08332-2}, (\href{http://www.hairer.org/notes/RoughPaths.pdf}{pdf}). \item Peter Friz and Nicolas Victoir, \emph{Multidimensional Stochastic Processes as Rough Paths: Theory and Applications} (2010) doi:\href{https://doi.org/10.1017/CBO9780511845079}{10.1017/CBO9780511845079} (\href{http://page.math.tu-berlin.de/~friz/master4_May6th.pdf}{pdf}). \end{itemize} \end{document}