Changeset 82 for papers


Ignore:
Timestamp:
Apr 5, 2012, 12:05:33 PM (12 years ago)
Author:
cecile
Message:

correction label AKS(cex)

Location:
papers/FDL2012
Files:
3 edited

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  • papers/FDL2012/abstraction_refinement.tex

    r81 r82  
    4848\begin{itemize}
    4949\item All its variables are concrete: $\forall s_i$ and $\forall p\in
    50 \widehat{AP}_i$, $p$ is either true or false according to $\check{L_i}$.
     50\widehat{AP}_i$, $p$ is either true or false according to $\widehat{L_i}$.
    5151(not {\it unknown}), and $s_0 $ is an initial state of the concrete system: $s_0 \in \mathbf{R}_0$
    5252\item  $\sigma$ is a counterexample in  $\widehat{M}_i$: $s_0\not\models \Phi$.
     
    7171
    7272\item $\widehat{S}_{\overline{\sigma}}$: $\{s_T\} \cup \{s_{i}'|\forall i\in
    73 [0..n-2] \vee s_i\in
    74 \sigma\}\cup \{\bar{s_{i}}|\forall i \in [0..n-1] \vee s_i\in \sigma\}$
     73[0..n-2] \wedge s_i\in
     74\sigma\}\cup \{\bar{s_{i}}|\forall i \in [0..n-1] \wedge s_i\in \sigma\}$
    7575
    7676\item $\widehat{L}_{\overline{\sigma}}$  with
    7777$L_{\overline{\sigma}}(s_i') = L_i(s_i), \forall i \in [0..n-2]$ and
    78 $L_{\overline{\sigma}}(\bar{s_i}) = \bar{L_i(s_i)}, \forall i \in [0..n-1]$
     78$L(s_T) = \{\top, \forall p \in AP_{\bar{\sigma}}\}$,
     79$L_{\overline{\sigma}}(\bar{s_i})$ is explained in the next construction step.
    7980
    8081\item $\widehat{S}_{0{\overline{\sigma}}} = \{ s_0',\bar{s_0}\}$
     
    8788\end{itemize}
    8889\end{definition}
    89 Note that in the labeling function represent (concrete) configuration of state $s_i$ and state $\bar{s_i}$  represents all
    90 configurations but the one of $s_i$. This last set may not be representable by
     90The labeling function fo $s_i'$ represents (concrete) configuration of state $s_i$ and state $\bar{s_i}$  represents all
     91configurations {\it but} the one of $s_i$. This last set may not be representable by
    9192the labeling function defined in def \ref{def-aks}. State labeling is treated
    9293in the second step. $s_T$ is a state where all atomic propositions are {\it unknown}.
     
    9697%We return back to the labeling of states of $AKS(\overline{\sigma})$. As states $s'$ are associated with the same (concrete) configuration as their corresponding state in $\sigma$, their labeling is straightforward : $\forall i \in [0..n-1], {L}_{\overline{\sigma}}(s'_i) = \widehat{L}_{i}(s_i)$.
    9798The set of configurations associated with a state $\bar{s_i}$ represents the
    98 negation of the one represented by ${L}_i(s'_i)$. This negation is not representable by the label of a single state but rather by a union of $\mid AP \mid$ labels.
     99negation of the one represented by ${L}_i(s_i)$. This negation is not representable by the label of a single state but rather by a union of $\mid AP \mid$ labels.
    99100
    100101\emph{Example}. Assume $AP = \{v_0,v_1,v_2\}$ and $\sigma = s_0 \rightarrow s_1$ and $\widehat{L}(s_0) = \{\mathbf{f},\mathbf{f},\mathbf{f}\}$ the configuration associated with $s_0$ assigns false to each variable. The negation of this configuration represents a set of seven concrete configurations which are covered by three (abstract) configurations: $\{\{\mathbf{t},\top,\top\},\{\mathbf{f},\mathbf{t},\top\},\{\mathbf{f},\mathbf{f},\mathbf{t}\}\}$.
     
    103104$\sigma$, one replaces in $AKS(\overline{\sigma})$ each state $\bar{s_i}$ by
    104105$k = \mid AP_{\overline\sigma} \mid$ states $\bar{s_i^j}$ with $j\in [0..k-1]$
    105 and assigns to each of them a label of $n$ variables $\{v_0, \ldots,
    106 v_{n-1}\}$ defined such that : ${L}(\bar{s_i^j} = \{\forall l \in [0..k-1],
     106and assigns to each of them a label of $k$ variables $\{v_0, \ldots,
     107v_{k-1}\}$ defined such that : ${L}(\bar{s_i^j} = \{\forall l \in [0..k-1],
    107108v_l = \neg  {L}_{i}(s_i)[v_l], \forall l \in [j+1..k-1], v_l = \top\}$. each
    108109state $\bar{s_i^j}$ is connected to the same predecessor and successor states
  • papers/FDL2012/framework.tex

    r81 r82  
    33description of our methodology is shown in figure \ref{cegar}.
    44We take into account the structure of the system as a set of synchronous components,
    5 each of which has been previously verified and a set of CTL properties is attached to each component. This set refers to the specification of the component. We would like to verify whether a concrete model, $M$ presumably huge sized and composed of several components, satisfies a global ACTL property $\Phi$.
     5each of which has been previously verified and a set of CTL properties is
     6attached to each component. This set refers to the specification of the
     7component. We would like to verify whether a concrete model, $M$ presumably
     8big sized and composed of several components, satisfies a global ACTL property $\Phi$.
    69%Due to state space combinatorial explosion phenomenon that occurs when verifying huge and complex systems, an abstraction or approximation of the concrete model has to be done in order to be able to verify the system with model-checking techniques.
    710Instead of building the product of the concrete components, we replace each concrete component by an abstraction of its behavior derived from a subset of the CTL properties it satisfies. Each abstract component represents an over-approximation of the set of behaviors of its related concrete component \cite{braunstein07ctl_abstraction}.
     
    8992false ($\mathbf{f}$), true ($\mathbf{t}$) and unknown ($\top$)).
    9093States with inconsistent truth values are not represented since they refer to non possible
    91 assignments of the atomic propositions. A set of fairness constraints eliminates non-progress cycles.
     94assignments of the atomic propositions. A set of fairness constraints
     95eliminates non-progress cycles. The transformation algorithm of a
     96CTL$\setminus$X property into an AKS is described in
     97\cite{braunstein07ctl_abstraction,braunstein_phd07}.
    9298
    9399
     
    158164Let $A_i$ and $A_j$ two abstractions such that $A_j$ is obtained by
    159165concretizing one abstract variable of $A_i$ (resp. $A_i$ is obtained by
    160 abstracting one variable in $A_j$). Then $A_i$ simulates $A_j$ and $A_j$
    161 concretizes $A_i$ , denoted by
     166abstracting one variable in $A_j$). Then $A_i$ simulates $A_j$, denoted by
    162167$A_j \sqsubseteq A_i$.
    163168\end{property}
     
    180185Let $s = (s_i,s_{\varphi_j^k})$ be a state in $S_{i+1}$, such that $s_i\in S_i$
    181186and $s_{\varphi_j^k} \in S_{\varphi_j^k}$.
    182 The label of $s_{i+1}$ respects the Belnap logic operator. For all $p \in
     187The label of $s_{i+1}$ is obtained by applying the Belnap logic operator and
     188to values of variables in $s_i$ and $s_{\varphi_j^k}$. For all $p \in
    183189AP_i \cup AP_{\varphi_j^k}$ we have the following label~:
    184190\begin{itemize}
     
    209215%In the following, we will name primary variables the set of variable that
    210216%appears in the global property.
    211 In the initial abstraction generation, all variables that appear int $\Phi$ have to be
     217In the initial abstraction generation, all variables that appear in $\Phi$ have to be
    212218represented. Therefore the properties in the specification of each component
    213219where these variables are present will be used to generate the initial
  • papers/FDL2012/ordering_filter_properties.tex

    r81 r82  
    1717the more closer a variable is from the primary
    1818variable the more it affects the primary variable. Hence, a property
    19 have higher priority according to the number of primary or close to primary variables it
     19has higher priority according to the number of primary or close to primary variables it
    2020contains.
    2121Moreover, a global property often specifies the behavior at the interface of
     
    2828\begin{enumerate}
    2929\item Build the structural dependency graph for all primary variables.
    30 \item Compute the depth of all variables (DFS or BFS)
     30\item Compute the depth of all variables
    3131in all dependency graphs.
    3232Note that a variable may belong to more than one dependency graph, in that case
     
    149149%are characterized. Hence there is more constrains behavior and more concretize
    150150%states.
    151 Unfortunately, this refinement does not ensure that the spurious counterexample
    152 is evicted.
    153151As we would like to ensure the elimination of the counter-example previously found,
    154152we filter out properties that do not have an impact on the counterexample
     
    158156the global property $\Phi$
    159157%as show in figure \ref{AKSNegCex}.
    160 In case where the spurious counter-example exhibits a bounded path, we add a last
    161 state $s_T$ where all variable are free({\it unknown}). The tree starting from this
    162 state represents all the possible future of the counterexample.
     158%In case where the spurious counter-example exhibits a bounded path, we add a last
     159%state $s_T$ where all variable are free({\it unknown}). The tree starting from this
     160%state represents all the possible future of the counterexample.
    163161
    164162
     
    185183\item $S_{\sigma} = \{s_{i}|s_i\in \sigma\}\cup\{s_T\}$
    186184\item $S_{0\sigma} = \{s_{0}\}$
    187 \item $L_{\sigma} = \widehat{L}_i$
     185\item $L_{\sigma} = \widehat{L}_i \cup L(s_T) = \{\top, \forall p \in AP_{\sigma}\}$
    188186\item $R_{\sigma} =  \{(s_{k}, s_{k+1})|(s_{k}\rightarrow s_{k+1})\in
    189187\sigma\}\cup\{(s_{n-1},s_T)\}$
     
    269267\end{proof}
    270268
    271 The propose approach ensure that the refinement excludes the counter-example
     269The proposed approach ensures that the refinement excludes the counter-example
    272270and  respects the definition \ref{def:goodrefinement}.
    273271We will show in our experiments that first the time needed to build an AKS is
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