diff options
author | Camil Staps | 2018-04-19 20:35:02 +0200 |
---|---|---|
committer | Camil Staps | 2018-04-19 20:35:18 +0200 |
commit | 1bf7cdf415488f7a7dbc10d9b76011b14214e41a (patch) | |
tree | 348c73df069e35b82ff9659bc2f256e6243e3027 | |
parent | Merge branch 'master' of gitlab.science.ru.nl:eveen/Model-Checking (diff) |
Finish semantics example
-rw-r--r-- | Assignment1/equivalence.tex | 5 | ||||
-rw-r--r-- | Assignment1/semantics.tex | 17 |
2 files changed, 19 insertions, 3 deletions
diff --git a/Assignment1/equivalence.tex b/Assignment1/equivalence.tex index 6195afc..6373088 100644 --- a/Assignment1/equivalence.tex +++ b/Assignment1/equivalence.tex @@ -8,9 +8,12 @@ we can define equivalence on PLTL formulas. \[\text{for any path } \pi \text{ and any position } i, \pi \vDash_i \phi \Leftrightarrow \pi \vDash_i \psi \qedhere\] \end{definition} -Additionally, we can define another form of equivalence, initial equivalence: +Additionally, we can define another form of equivalence, initial equivalence. +When two formulas are initially equivalent, they are equivalent for all paths at position 0. +This is mainly useful to compare PLTL and LTL formulas. \begin{definition}[Initial Equivalence of PLTL Formulae] 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 +%TODO: examples diff --git a/Assignment1/semantics.tex b/Assignment1/semantics.tex index 1bca0b2..d99e636 100644 --- a/Assignment1/semantics.tex +++ b/Assignment1/semantics.tex @@ -117,7 +117,20 @@ The only difference is that $\vDash$ now is a ternary relation, and we use $\pi\ \end{figure} \begin{example}[Satisfaction of PLTL Formulae by Transition Systems] - Consider again the transition system from Figure 5.3, reproduced as \cref{fig:pltl:example-ts}. - % TODO + Consider again the transition system $TS$ from Figure 5.3, reproduced as \cref{fig:pltl:example-ts}. + \begin{itemize} + \item + Recall that $TS \vDash \square a$. + A noteworthy peculiarity is that $TS \nvDash \square\Xop^{-1}a$, since $\Xop^{-1}\phi$ is always false at position 0. + Clearly, we do have $TS \vDash_i \square\Xop^{-1}a$ for $i \ge 1$. + \item + We also have $TS \vDash \square(b \rightarrow \square^{-1}b)$. + After all, if $b$ does not hold, $b$ will never hold again. + \item + We have $s_1 \vDash \square(a \Sop b)$: + since $a$ always holds, this is for $TS$ equivalent to $\square(\top \Sop b) \equiv \square(\lozenge^{-1}b)$, and $s_1 \vDash b$. + However, since $s_2 \nvDash \square(a \Sop b)$ (because $a^\omega \nvDash \square(a \Sop b)$), also $TS \nvDash \square(a \Sop b)$. + \qedhere + \end{itemize} \end{example} \cbend |