X-Git-Url: https://bilbo.iut-bm.univ-fcomte.fr/and/gitweb/16dcc.git/blobdiff_plain/236f25b2f3a081b11c71bedad6d044d695ce2cca..refs/heads/master:/stopping.tex?ds=sidebyside diff --git a/stopping.tex b/stopping.tex index fb0b9e0..bb95663 100644 --- a/stopping.tex +++ b/stopping.tex @@ -1,6 +1,6 @@ This section considers functions $f: \Bool^{\mathsf{N}} \rightarrow \Bool^{\mathsf{N}} $ issued from an hypercube where an Hamiltonian path has been removed -as described in previous section. +as described in the previous section. Notice that the iteration graph is always a subgraph of ${\mathsf{N}}$-cube augmented with all the self-loop, \textit{i.e.}, all the edges $(v,v)$ for any $v \in \Bool^{\mathsf{N}}$. @@ -10,7 +10,7 @@ interpreted as Markov chains. \begin{xpl} Let us consider for instance the graph $\Gamma(f)$ defined -in \textsc{Figure~\ref{fig:iteration:f*}.} and +in Figure~\ref{fig:iteration:f*} and the probability function $p$ defined on the set of edges as follows: $$ p(e) \left\{ @@ -33,19 +33,19 @@ P=\dfrac{1}{6} \left( 0&0&0&0&1&0&4&1 \\ 0&0&0&1&0&1&0&4 \end{array} -\right) +\right). \] \end{xpl} A specific random walk in this modified hypercube is first -introduced (See section~\ref{sub:stop:formal}). We further +introduced (see Section~\ref{sub:stop:formal}). We further study this random walk in a theoretical way to provide an upper bound of fair sequences -(See section~\ref{sub:stop:bound}). -We finally complete these study with experimental +(see Section~\ref{sub:stop:bound}). +We finally complete this study with experimental results that reduce this bound (Sec.~\ref{sub:stop:exp}). -Notice that for a general references on Markov chains +For a general reference on Markov chains, see~\cite{LevinPeresWilmer2006}, and particularly Chapter~5 on stopping times. @@ -60,18 +60,25 @@ $$\tv{\pi-\mu}=\frac{1}{2}\sum_{X\in\Bool^{\mathsf{N}}}|\pi(X)-\mu(X)|.$$ Moreov $\nu$ is a distribution on $\Bool^{\mathsf{N}}$, one has $$\tv{\pi-\mu}\leq \tv{\pi-\nu}+\tv{\nu-\mu}$$ -Let $P$ be the matrix of a Markov chain on $\Bool^{\mathsf{N}}$. $P(X,\cdot)$ is the -distribution induced by the $X$-th row of $P$. If the Markov chain induced by -$P$ has a stationary distribution $\pi$, then we define +Let $P$ be the matrix of a Markov chain on $\Bool^{\mathsf{N}}$. For any +$X\in \Bool^{\mathsf{N}}$, let $P(X,\cdot)$ be the distribution induced by the +${\rm bin}(X)$-th row of $P$, where ${\rm bin}(X)$ is the integer whose +binary encoding is $X$. If the Markov chain induced by $P$ has a stationary +distribution $\pi$, then we define $$d(t)=\max_{X\in\Bool^{\mathsf{N}}}\tv{P^t(X,\cdot)-\pi}.$$ +%\ANNOT{incohérence de notation $X$ : entier ou dans $B^N$ ?} and $$t_{\rm mix}(\varepsilon)=\min\{t \mid d(t)\leq \varepsilon\}.$$ -Intuitively speaking, $t_{\rm mix}$ is a mixing time -\textit{i.e.}, is the time until the matrix $X$ of a Markov chain -is $\epsilon$-close to a stationary distribution. +%% Intuitively speaking, $t_{\rm mix}$ is a mixing time +%% \textit{i.e.}, is the time until the matrix $X$ of a Markov chain +%% is $\epsilon$-close to a stationary distribution. + +Intuitively speaking, $t_{\rm mix}(\varepsilon)$ is the time/steps required +to be sure to be $\varepsilon$-close to the stationary distribution, wherever +the chain starts. @@ -113,9 +120,8 @@ $$\P_X(X_\tau=Y)=\pi(Y).$$ \subsection{Upper bound of Stopping Time}\label{sub:stop:bound} - A stopping time $\tau$ is a {\emph strong stationary time} if $X_{\tau}$ is -independent of $\tau$. +independent of $\tau$. The following result will be useful~\cite[Proposition~6.10]{LevinPeresWilmer2006}, \begin{thrm}\label{thm-sst} @@ -131,8 +137,8 @@ In other words, $E$ is the set of all the edges in the classical ${\mathsf{N}}$-cube. Let $h$ be a function from $\Bool^{\mathsf{N}}$ into $\llbracket 1, {\mathsf{N}} \rrbracket$. Intuitively speaking $h$ aims at memorizing for each node -$X \in \Bool^{\mathsf{N}}$ which edge is removed in the Hamiltonian cycle, -\textit{i.e.} which bit in $\llbracket 1, {\mathsf{N}} \rrbracket$ +$X \in \Bool^{\mathsf{N}}$ whose edge is removed in the Hamiltonian cycle, +\textit{i.e.}, which bit in $\llbracket 1, {\mathsf{N}} \rrbracket$ cannot be switched. @@ -158,7 +164,7 @@ P_h(X,Y)=\frac{1}{2{\mathsf{N}}} & \textrm{if $X\neq Y$ and $(X,Y) \in E_h$} We denote by $\ov{h} : \Bool^{\mathsf{N}} \rightarrow \Bool^{\mathsf{N}}$ the function such that for any $X \in \Bool^{\mathsf{N}} $, $(X,\ov{h}(X)) \in E$ and $X\oplus\ov{h}(X)=0^{{\mathsf{N}}-h(X)}10^{h(X)-1}$. -The function $\ov{h}$ is said {\it square-free} if for every $X\in \Bool^{\mathsf{N}}$, +The function $\ov{h}$ is said to be {\it square-free} if for every $X\in \Bool^{\mathsf{N}}$, $\ov{h}(\ov{h}(X))\neq X$. \begin{lmm}\label{lm:h} @@ -202,10 +208,10 @@ $$ An integer $\ell\in \llbracket 1,{\mathsf{N}} \rrbracket$ is said {\it fair} at time $t$ if there exists $0\leq j t)\leq \frac{E[\tau]}{t}$. -With $t=32N^2+16N\ln (N+1)$, one obtains: $\P_X(\tau > t)\leq \frac{1}{4}$. -Therefore, using the defintion of $t_{\rm mix)}$ and +With $t_n=32N^2+16N\ln (N+1)$, one obtains: $\P_X(\tau > t_n)\leq \frac{1}{4}$. +Therefore, using the definition of $t_{\rm mix}$ and Theorem~\ref{thm-sst}, it follows that -$t_{\rm mix}\leq 32N^2+16N\ln (N+1)=O(N^2)$. +$t_{\rm mix}(\frac{1}{4})\leq 32N^2+16N\ln (N+1)=O(N^2)$ and that + Notice that the calculus of the stationary time upper bound is obtained under the following constraint: for each vertex in the $\mathsf{N}$-cube there are one ongoing arc and one outgoing arc that are removed. -The calculus does not consider (balanced) Hamiltonian cycles, which +The calculus doesn't consider (balanced) Hamiltonian cycles, which are more regular and more binding than this constraint. Moreover, the bound -is obtained using Markov Inequality which is frequently coarse. For the -classical random walkin the $\mathsf{N}$-cube, without removing any -Hamiltonian cylce, the mixing time is in $\Theta(N\ln N)$. +is obtained using the coarse Markov Inequality. For the +classical (lazy) random walk the $\mathsf{N}$-cube, without removing any +Hamiltonian cycle, the mixing time is in $\Theta(N\ln N)$. We conjecture that in our context, the mixing time is also in $\Theta(N\ln N)$. -In this later context, we claim that the upper bound for the stopping time +In this latter context, we claim that the upper bound for the stopping time should be reduced. This fact is studied in the next section. \subsection{Practical Evaluation of Stopping Times}\label{sub:stop:exp} Let be given a function $f: \Bool^{\mathsf{N}} \rightarrow \Bool^{\mathsf{N}}$ and an initial seed $x^0$. -The pseudo code given in algorithm~\ref{algo:stop} returns the smallest +The pseudo code given in Algorithm~\ref{algo:stop} returns the smallest number of iterations such that all elements $\ell\in \llbracket 1,{\mathsf{N}} \rrbracket$ are fair. It allows to deduce an approximation of $E[\ts]$ by calling this code many times with many instances of function and many seeds. -Practically speaking, for each number $\mathsf{N}$,$ 3 \le \mathsf{N} \le 16$, -10 functions have been generaed according to method presented in section~\ref{sec:hamilton}. For each of them, the calculus of the approximation of $E[\ts]$ -is executed 10000 times with a random seed. The table~\ref{table:stopping:moy} -summarizes results. It can be observed that the approximation is largely -wœsmaller than the upper bound given in theorem~\ref{prop:stop}. - \begin{algorithm}[ht] %\begin{scriptsize} \KwIn{a function $f$, an initial configuration $x^0$ ($\mathsf{N}$ bits)} @@ -389,39 +402,59 @@ wœsmaller than the upper bound given in theorem~\ref{prop:stop}. $\textit{nbit} \leftarrow 0$\; $x\leftarrow x^0$\; -$\textit{visited}\leftarrow\emptyset$\; - -\While{$\left\vert{\textit{visited}}\right\vert < \mathsf{N} $} +$\textit{fair}\leftarrow\emptyset$\; +\While{$\left\vert{\textit{fair}}\right\vert < \mathsf{N} $} { - $ s \leftarrow \textit{Random}(n)$ \; + $ s \leftarrow \textit{Random}(\mathsf{N})$ \; $\textit{image} \leftarrow f(x) $\; - \If{$x[s] \neq \textit{image}[s]$}{ - $\textit{visited} \leftarrow \textit{visited} \cup \{s\}$ + \If{$\textit{Random}(1) \neq 0$ and $x[s] \neq \textit{image}[s]$}{ + $\textit{fair} \leftarrow \textit{fair} \cup \{s\}$\; + $x[s] \leftarrow \textit{image}[s]$\; } - $x[s] \leftarrow \textit{image}[s]$\; $\textit{nbit} \leftarrow \textit{nbit}+1$\; } \Return{$\textit{nbit}$}\; %\end{scriptsize} -\caption{Pseudo Code of the stoping time calculus} +\caption{Pseudo Code of stopping time computation} \label{algo:stop} \end{algorithm} +Practically speaking, for each number $\mathsf{N}$, $ 3 \le \mathsf{N} \le 16$, +10 functions have been generated according to the method presented in Section~\ref{sec:hamilton}. For each of them, the calculus of the approximation of $E[\ts]$ +is executed 10000 times with a random seed. Figure~\ref{fig:stopping:moy} +summarizes these results. A circle represents the +approximation of $E[\ts]$ for a given $\mathsf{N}$. +The line is the graph of the function $x \mapsto 2x\ln(2x+8)$. +It can firstly +be observed that the approximation is largely +smaller than the upper bound given in Theorem~\ref{prop:stop}. +It can be further deduced that the conjecture of the previous section +is realistic according to the graph of $x \mapsto 2x\ln(2x+8)$. -\begin{table} -$$ -\begin{array}{|*{15}{l|}} -\hline -\mathsf{N} & 3 & 4 & 5 & 6 & 7& 8 & 9 & 10& 11 & 12 & 13 & 14 & 15 & 16 \\ -\hline -\mathsf{N} & 3 & 10.9 & 5 & 17.7 & 7& 25 & 9 & 32.7& 11 & 40.8 & 13 & 49.2 & 15 & 16 \\ -\hline -\end{array} -$$ -\caption{Average Stopping Time}\label{table:stopping:moy} -\end{table} + + +% \begin{table} +% $$ +% \begin{array}{|*{14}{l|}} +% \hline +% \mathsf{N} & 4 & 5 & 6 & 7& 8 & 9 & 10& 11 & 12 & 13 & 14 & 15 & 16 \\ +% \hline +% \mathsf{N} & 21.8 & 28.4 & 35.4 & 42.5 & 50 & 57.7 & 65.6& 73.5 & 81.6 & 90 & 98.3 & 107.1 & 115.7 \\ +% \hline +% \end{array} +% $$ +% \caption{Average Stopping Time}\label{table:stopping:moy} +% \end{table} + +\begin{figure} +\centering +\includegraphics[width=0.49\textwidth]{complexity} +\caption{Average Stopping Time Approximation}\label{fig:stopping:moy} +\end{figure} + + %%% Local Variables: %%% mode: latex