X-Git-Url: https://bilbo.iut-bm.univ-fcomte.fr/and/gitweb/16dcc.git/blobdiff_plain/2cf19b6a4aa1800981fa0b35e6f555119b94910e..66ea391a3e386a6ed3b47d5011977ca136f65ad2:/stopping.tex diff --git a/stopping.tex b/stopping.tex index 3a07e06..d72f8bb 100644 --- a/stopping.tex +++ b/stopping.tex @@ -144,7 +144,7 @@ A stopping time $\tau$ is a {\emph strong stationary time} if $X_{\tau}$ is independent of $\tau$. -\begin{thrm} +\begin{thrm}\label{thm-sst} If $\tau$ is a strong stationary time, then $d(t)\leq \max_{X\in\Bool^{\mathsf{N}}} \P_X(\tau > t)$. \end{thrm} @@ -362,16 +362,27 @@ One can now prove Theorem~\ref{prop:stop}. \begin{proof} Since $\ts^\prime$ is the time used to obtain $\mathsf{N}-1$ fair bits. Assume that the last unfair bit is $\ell$. One has -$\ts=\ts^\prime+S_{X_\tau,\ell}$, and therefore -$E[\ts] = E[\ts^\prime]+E[S_{X_\tau,\ell}]$. Therefore, -Theorem~\ref{prop:stop} is a direct application of -lemma~\ref{prop:lambda} and~\ref{lm:stopprime}. +$\ts=\ts^\prime+S_{X_\tau,\ell}$, and therefore $E[\ts] = +E[\ts^\prime]+E[S_{X_\tau,\ell}]$. Therefore, Theorem~\ref{prop:stop} is a +direct application of lemma~\ref{prop:lambda} and~\ref{lm:stopprime}. \end{proof} +Now using Markov Inequality, one has $\P_X(\tau > t)\leq \frac{E[\tau]}{t}$. +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 +Theorem~\ref{thm-sst}, it follows that +$t_{\rm mix}\leq 32N^2+16N\ln (N+1)=O(N^2)$. + + 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 -are more regular and more binding than this constraint. -In this later context, we claim that the upper bound for the stopping time -should be reduced. +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 $\Theta(N\ln N)$. +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 +%should be reduced.