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author | Camil Staps | 2018-04-12 23:00:01 +0200 |
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committer | Camil Staps | 2018-04-12 23:00:01 +0200 |
commit | 77a3809bc63d5571205fff9c62499094d2fb3727 (patch) | |
tree | 5461ff8f1f45ba4aad51261599f3dff56ca58b44 /Assignment1/assignment1.tex | |
parent | Notations (diff) |
Add an exercise based on Markey's proof; extend the grammar because we allow PLTL formulas inside LTL formulas
Diffstat (limited to 'Assignment1/assignment1.tex')
-rw-r--r-- | Assignment1/assignment1.tex | 210 |
1 files changed, 183 insertions, 27 deletions
diff --git a/Assignment1/assignment1.tex b/Assignment1/assignment1.tex index 0149906..610f7ec 100644 --- a/Assignment1/assignment1.tex +++ b/Assignment1/assignment1.tex @@ -6,6 +6,7 @@ \usepackage{amsmath} \usepackage{amsthm} \usepackage{amssymb} +\renewcommand{\qedsymbol}{$\blacksquare$} \let\leq\leqslant \let\le\leqslant % See http://www.ams.org/faq?faq_id=212 for the trick to add qed at the end of @@ -21,7 +22,7 @@ \theoremstyle{mydefinition} \newtheorem{xdefinition}{Definition} \newenvironment{definition}% - {\renewcommand{\qedsymbol}{$\blacksquare$}\pushQED{\qed}\begin{xdefinition}}% + {\pushQED{\qed}\begin{xdefinition}}% {\popQED\end{xdefinition}} \newtheoremstyle{myexample}% {2em}{2em}% Space above and below @@ -34,12 +35,15 @@ \theoremstyle{myexample} \newtheorem{xexample}{Example} \newenvironment{example}% - {\renewcommand{\qedsymbol}{$\blacksquare$}\pushQED{\qed}\begin{xexample}}% + {\pushQED{\qed}\begin{xexample}}% {\popQED\end{xexample}} \newtheorem{xremark}{Remark} \newenvironment{remark}% - {\renewcommand{\qedsymbol}{$\blacksquare$}\pushQED{\qed}\begin{xremark}}% + {\pushQED{\qed}\begin{xremark}}% {\popQED\end{xremark}} +\newtheoremstyle{exercise}{1em}{1em}{}{}{\scshape}{.}{1em}{} +\theoremstyle{exercise} +\newtheorem{exercise}{Exercise} \usepackage{mathtools} \usepackage{mdframed} \usepackage{tikz} @@ -47,6 +51,7 @@ \usepackage{relsize} \usepackage{parskip} \usepackage{cleveref} +\usepackage{enumitem} \usepackage{stackengine} \crefname{figure}{Figure}{Figures} \usepackage[color]{changebar} @@ -106,14 +111,8 @@ For this reason, it is useful to discuss them here. % Provide intuitive semantics %TODO: Provide formal semantics \erin -This subsection describes the syntax and semantics of PLTL.% -\footnote{% - Given that PLTL is an extension of LTL, we are left with two options. - The first option is to define the entire syntax of PLTL without considering that we have already defined LTL. - This option is slightly more verbose, but does not depend on subsection 5.1.1. - The second option, which we will adopt here, builds on the syntax and semantics that are already defined for LTL formulae.} -All LTL formulae are PLTL formulae. -Two additional operators are added: +This subsection describes the syntax of PLTL. +PLTL uses the same operators as LTL and adds two additional operators: $\Pop$ (pronounced \enquote{previously}) and $\Sop$ (pronounced \enquote{since}). The $\Pop$-modality is comparable to $\Xop$. @@ -122,17 +121,25 @@ The $\Sop$-modality is comparable to $\Uop$: $\phi_1\Sop\phi_2$ holds if $\phi_2 and $\phi_1$ held ever after that moment up to and including the current moment. \begin{definition}[Syntax of PLTL] - PLTL formulae over the set $LTL$ of LTL formulae are formed according to the following grammar: - $$ - \phi ::= l - \mid \Pop \phi - \mid \phi_1 \Sop \phi_2 - $$ - where $l \in LTL$. + PLTL formulae over the set $AP$ of atomic propositions are formed according to the following grammar: + \[ + \phi + ::= + \left.\raisebox{0pt}[5pt][5pt]{} \text{true} + \enspace\middle|\enspace a + \enspace\middle|\enspace \phi_1 \land \phi_2 + \enspace\middle|\enspace \lnot \phi + \enspace\middle|\enspace \bigcirc \phi + \enspace\middle|\enspace \phi_1 \Uop \phi_2 + \enspace\middle|\enspace \Pop \phi + \enspace\middle|\enspace \phi_1 \Sop \phi_2 + \right. + \] + where $a \in AP$. \end{definition} \camil -The precedence order of the LTL operators remains the same. +The precedence order of the operators borrowed from LTL remains the same. $\Pop$ binds equally strong as $\Xop$ and $\lnot$. $\Sop$ takes precedence over $\Uop$, and like $\Uop$ is right-associative. @@ -273,16 +280,22 @@ We use $\sigma \vDash \phi$ as a shorthand for $\sigma \vDash_0 \phi$. \erin \begin{definition}[Semantics of PLTL (Interpretation over Words)] Let $\phi$ be a PLTL formula over $AP$. The LT property induced by $\phi$ is - $$Words(\phi) = \{\sigma \in \left(2^{AP}\right)^\omega \mid \sigma \vDash \phi\}$$ + \[Words(\phi) = \{\sigma \in \left(2^{AP}\right)^\omega \mid \sigma \vDash \phi\}\] where $\vDash\ \subseteq \left(2^{AP}\right)^\omega \times \mathbb{N} \times PLTL$ is the smallest relation with the properties in \cref{fig:PLTL-semantics}. \end{definition} \camil Note that we must redefine the satisfaction relation for the LTL operators, because $\vDash$ is now a ternary relation. +The difference with LTL formulae is well illustrated by the $\bigcirc$ operator. +In the LTL case, $\sigma=A_0A_1A_2\dots\vDash\bigcirc\phi$ iff $\sigma[1\dots]=A_1A_2\dots\vDash\phi$. +Thus, whether $\bigcirc\phi$ holds for $\sigma$ cannot depend on $A_0$. +In the PLTL case, $\sigma\vDash_i\bigcirc\phi$ iff $\sigma\vDash_{i+1}\phi$. +The information about $A_0$ is not lost, so whether $\bigcirc\phi$ holds for $\sigma$ may depend on $A_0$, + as is trivially the case with $\bigcirc\bigcirc^{-1}a$. \begin{figure} \centering \begin{mdframed} - $$ + \[ \begin{matrix*}[l] \sigma &\vDash_i & \text{true}\\ \sigma &\vDash_i & a &\text{iff} & a\in A_i\\ @@ -293,7 +306,7 @@ Note that we must redefine the satisfaction relation for the LTL operators, beca \sigma &\vDash_i & \phi_1\Sop\phi_2 &\text{iff} & \exists_{j \le i}.\text{$\sigma \vDash_j \phi_2$ and $\sigma \vDash_k \phi_1$ for all $j < k \le i$}\\ \sigma &\vDash_i & \Pop\phi &\text{iff} & i \geq 1 \wedge \sigma \vDash_{i-1} \phi \end{matrix*} - $$ + \] \end{mdframed} \caption{PLTL semantics for infinite words $\sigma=A_0A_1A_2\dots \in \left(2^{AP}\right)^\omega$.} \label{fig:PLTL-semantics} @@ -304,9 +317,9 @@ Note that we must redefine the satisfaction relation for the LTL operators, beca Let $TS = (S, Act, \rightarrow, I, AP, L)$ be a transition system without terminal states, and let $\phi$ be an PLTL-formula over AP. \begin{itemize} \item For infinite path fragments $\pi$ of $TS$, the satisfaction relation is defined by - $$\pi \vDash \phi \Leftrightarrow trace(\pi) \vDash \phi$$ + \[\pi \vDash \phi \Leftrightarrow trace(\pi) \vDash \phi\] \item For state $s \in S$, the satisfaction relation $\vDash$ is defined by - $$s \vDash \phi \Leftrightarrow \forall_{\pi \in Paths(s)}[\pi \vDash \phi]$$ + \[s \vDash \phi \Leftrightarrow \forall_{\pi \in Paths(s)}[\pi \vDash \phi]\] \item $TS$ satisfies $\phi$, denoted by $TS \vDash \phi$ if $Traces \vDash \phi$, if $Traces(TS) \subseteq Words(\phi)$ \qedhere \end{itemize} @@ -317,12 +330,12 @@ we must provide their semantics. Note that we need to add a index $i$, since we must also be able to look in the past. Given these definitions, it is possible to derive the formal semantics of the $\Fop^{-1}$ and $\Gop^{-1}$ operators as well: -$$ +\[ \begin{matrix*}[l] \sigma &\vDash_i &\Fop^{-1}\phi &\text{iff} &\exists_{k \leq i}[\sigma \vDash_k \phi]\\ \sigma &\vDash_i &\Gop^{-1}\phi &\text{iff} &\forall_{k \leq i}[\sigma \vDash_k \phi] \end{matrix*} -$$ +\] \subsubsection{Specifying Properties} % TODO Once operator @@ -350,7 +363,7 @@ we can define equivalence on PLTL formulas. Additionally, we can define another form of equivalence, initial equivalence: \begin{definition}[Initial Equivalence of PLTL Formulae] - PLTL formulae $\phi_1,\phi_2$ are initial equivalent, denoted $\phi_1 \equiv_0 \phi_2$ iff they verify the following property: + PLTL formulae $\phi_1,\phi_2$ are initially equivalent, denoted $\phi_1 \equiv_0 \phi_2$ iff they verify the following property: \[\text{for any path } \pi, \pi \vDash_0 \phi \Leftrightarrow \pi \vDash_0 \psi \qedhere\] \end{definition} \cbend @@ -376,6 +389,149 @@ Additionally, we can define another form of equivalence, initial equivalence: % A possibly helpful list is at https://cstheory.stackexchange.com/a/29452 % Also the bibliography file should be worked through. +\section{Exercises} +% After the exam documentclass; http://compgroups.net/comp.text.tex/-if-else-fi-in-new-environment/263869 +\newif\ifshowanswers\showanswerstrue +\newenvironment{answer}% + {\ifshowanswers\par\bgroup\small\textit{Answer:}\else\setbox0\vbox\bgroup\fi}% + {\egroup} +\newcommand{\hint}[1]{\par\textit{Hint: #1}} +\camil +\begin{exercise} + In this exercise we prove that PLTL formulas can be exponentially more succinct. + The proof followed here is that of \citet{Markey2003} which, in turn, is based on work by \citet{Etessami2002}. + The proof is achieved by giving an example of a formula which can be expressed in $\mathcal O(n)$ in PLTL but requires $\Omega(n)$ in LTL. + + Take $n\in\mathbb N$ and $AP=\{p_0,\dots,p_n\}$. + We first show that there is no polynomial-size LTL formula expressing property~\ref{ex:proof-markey:prop-agreement}. + \begin{equation} + \phi_n(\sigma) \defeq + \forall_{i,j\in\mathbb N} + \left[ + \forall_{k\in[1,n]} + [(A_i\vDash p_k) \Leftrightarrow (A_j\vDash p_k)] + \rightarrow + ((A_i\vDash p_0) \Leftrightarrow (A_j\vDash p_0)) + \right] + \label{ex:proof-markey:prop-agreement} + \end{equation} + where $\sigma=A_0A_1A_2\dots$. + In other words, if two points on path $\sigma$ agree on $p_k$ for all $k\in[1,n]$, the points must also agree on $p_0$. + + \begin{enumerate}[label=(\alph*)] + \item Find an $\mathcal O\left(2^n\right)$ LTL formula expressing property~\ref{ex:proof-markey:prop-agreement}. + \hint{if the formula can be $\mathcal O\left(2^n\right)$, what are you allowed to quantify over?} + \begin{answer}% + \footnote{Note that this is slightly different from the version in \citet[p. 4]{Markey2003}. + The limit on the leftmost $\wedge$ has $i\in[1,n]$ rather than $i\in[0,n]$ in the original paper. + We believe this to be an error, because otherwise $a_0$ is a free variable.} %TODO do you agree? + \[\phi_n(\sigma) = + \bigwedge_{\substack{a_i\in\{\top,\bot\}\\i\in[0,n]}} \left[ + \left(\lozenge(\bigwedge\nolimits_{i=0}^n p_i=a_i)\right) + \rightarrow + \square\left((\bigwedge\nolimits_{i=1}^n p_i=a_i) \rightarrow p_0=a_0\right) + \right] + \] + \end{answer} + + \item Assume a polynomial-size LTL formula exists for property~\ref{ex:proof-markey:prop-agreement}. + What can you say of the size of a B\"uchi automaton $\mathcal A$ recognizing $\textsl{Words}(\phi_n)$? + \label{ex:proof-markey:assumption} + \hint{consider Theorem 5.41.} + \begin{answer} + There exists a B\"uchi automaton of size $\mathcal O(2^{n^k})$ for some $k\in\mathbb N$. + \end{answer} + + \item Let $A=a_0,\dots,a_{2^n-1}$ be any permutation of $2^{AP\setminus\{p_0\}}$. + Define $w_K=b_{K,0}\dots b_{K,2^n-1}$ with + \[ + b_{K,i} \defeq + \begin{cases} + a_i & \text{iff $i\notin K$}\\ + a_i \cup \{p_0\} & \text{iff $i\in K$.} + \end{cases} + \] + Show that if $K,K' \subseteq \{0,\dots,2^n-1\}$ and $K\ne K'$, also $w_K \ne w_{K'}$. + \label{ex:proof-markey:different-w_K} + \begin{answer} + Without loss of generality, assume there exists an $i\in K$ with $i\notin K'$. + Then $p_0\in b_{K,i}$ but $p_0\notin b_{K',i}$. + Hence, $w_K\ne w_{K'}$. + \end{answer} + + \item How many distinct words $w_K$ exist? + \label{ex:proof-markey:nr-of-w_k} + \begin{answer} + There are $2^{|\{0,\dots,2^n-1\}|} = 2^{2^n}$ distinct $K$ (and equally many distinct $w_K$). + \end{answer} + + \item Show that $w_K^\omega$ is accepted by $\mathcal A$. + \begin{answer} + Since all $a_i$ are distinct, + two points $b_{K,j}, b_{K,k}$ on $w_K^\omega$ agree on all $p_i$ for $i\in[1,n]$ iff $j\equiv k \pmod{2^n}$. + In this case, they also agree on $p_0$. + \end{answer} + + \item It follows that there are paths $\pi_K$ and $\pi_{K'}$ in $\mathcal A$ accepting $w_K^\omega$ and $w_{K'}^\omega$ respectively. + Let $q_K$ and $q_{K'}$ be the $2^n$-th states of each of these paths. + Assume that $q_K = q_{K'}$. + Construct from $w_K$ and $w_{K'}$ an infinite word $v$ that is accepted by $\mathcal A$ but does not satisfy $\phi_n$. + \hint{take the simplest infinite word using both words that you can think of.} + \begin{answer} + Take $v=w_Kw_{K'}^\omega$. + Apart from the prefix of size $2^n$, the path of this word is equal to that of $w_{K'}^\omega$, which is accepted. + So $v$ is accepted. + From \ref{ex:proof-markey:different-w_K} we have an $i$ such that $p_0\in b_{K,i}$ but $p_0\notin b_{K',i}$. + However, for all $i\in[1,n]$, $p_i\in b_{K,i} \Leftrightarrow p_i\in b_{K',i}$. + Therefore, $i=i, j=i+2^n$ is a counterexample to the outermost quantifier of $\phi_n$. + \end{answer} + + \item Show that this contradicts the assumption from \ref{ex:proof-markey:assumption}. + \begin{answer} + Since we have $2^{2^n}$ distinct $w_K$ [cf. \ref{ex:proof-markey:nr-of-w_k}] and the $2^n$-th states of their accepting paths must all be distinct, + $\mathcal A$ has at least $2^{2^n}$ states. + But $2^{2^n} \notin \mathcal O(2^{n^k})$. + \end{answer} + + \item We now turn to a slightly different property: + \begin{equation} + \psi_n(\sigma) \defeq + \forall_{i\in\mathbb N} + \left[ + \forall_{k\in[1,n]} + [(A_i\vDash p_k) \Leftrightarrow (A_0\vDash p_k)] + \rightarrow + ((A_i\vDash p_0) \Leftrightarrow (A_0\vDash p_0)) + \right] + \label{ex:proof-markey:prop-agreement-2} + \end{equation} + Property \ref{ex:proof-markey:prop-agreement-2} holds if all points on $\sigma$ that agree with all $p_k$ for $k\in[1,n]$ with $A_n$ also agree on $p_0$. + Give an $\mathcal O(n)$ PLTL formula expressing property \ref{ex:proof-markey:prop-agreement-2}. + \hint{recall the semantics of the dual modalities in PLTL.} + \begin{answer} + \[\psi_n(\sigma) = + \square\left[ + \left(\bigwedge\nolimits_{i=1}^n (p_i \Leftrightarrow \lozenge^{-1}\square^{-1}p_i)\right) + \Rightarrow + (p_0 \Leftrightarrow \lozenge^{-1}\square^{-1}p_0) + \right] + \] + \end{answer} + + \item Construct an LTL formula for $\phi_n$ using the PLTL formula for $\psi_n$ and conclude the proof. + \hint{first construct an LTL formula for $\psi_n$.} + \begin{answer} + Take $\phi'_n \defeq \square\psi'_n$, where $\psi'_n$ is an LTL formula initially equivalent to $\psi_n$. + By virtue of the $\square$ operator, $\phi_n\equiv\phi'_n$. + But $\phi_n$ is $\mathcal O(2^n$, so also $\phi'_n$ is exponential. + Since $\phi'_n$ is $\mathcal O(2^n)$ and $\psi_n$ is $\mathcal O(n)$, + the PLTL formula for property~\ref{ex:proof-markey:prop-agreement-2} is exponentially more succinct than the LTL formula. + \qed + \end{answer} + \end{enumerate} +\end{exercise} +\cbend + \section{Contribution} %TODO: Like we are some immature group of children, we have to provide proof of contribution \camil |