Transition systems are a well established semantic model for both sequential and concurrent systems.
A transition system is a structure $T = (S,i,L,Tran)$, where
$S$ is a set of states with initial state, $i$;
$L$ is a set of labels, sometimes referred to also as events;
$Tran\subseteq S\times L\times S$ is the transition relation.
Let $(S, i, L, Tran )$ be a transition system. We write
to indicate that $(s, a, s')\in Tran$.
A morphism from one transition system, $T$, to another $T'$ will be a pair $(\sigma, \lambda)$, in which
$\sigma$ is a function from the states of $T$ to those of $T'$
$\lambda$ is a partial function from the labels of $T$ to those of $T'$ such that for any transition $s\stackrel{a}{\to} s'$ of $T$ if $\lambda(a)$ is defined, then $\sigma(s)\stackrel{\lambda(a)}{\to} \sigma(s')$ is a transition of $T'$; otherwise, if $\lambda(a)$ is undefined, then $\sigma(s) = \sigma(s')$.
It is useful to rework this definition of morphism using a variant of the idea, discussed at partial function, that replaces a partial function by a total function using the neat trick of adding an additional element $\bot$ to the codomain. (We will use the notation from partial function freely in what follows.) This is done here simply by introducing idle transitions $(s,\bot,s)$ thought of as going from $s$ to itself, and working with $L_\bot$ as a set of labels instead of $L$. (This is very neat here as it corresponds the label $\bot$ to ‘do nothing’ to the states.) After completing everything in this way we get new transition systems $T_\bot = (S,i,L_\bot, Tran_\bot)$, etc. and will work with these. (Of course, $Tran_\bot = Tran \cup \{ (s,\bot,s)\mid s\in S\}$.) Now a morphism $f$ is the same as given by a pair $\sigma: S\to S'$, as before, and $\lambda: L_\bot\to L'_\bot$, satisfying the compatibility condition that if $(s,a,s')\in Tran_\bot$, then $(\sigma(s),\lambda(a),\sigma(s'))\in Tran'_\bot$, (and that $\lambda_\bot(\bot) = \bot'$).
This way we get a category, $TS$, of transition systems.
The notions of transition system and of morphisms between them is clearly related to (low dimensional) cubical sets / labelled directed graphs/labelled transition systems, but we will need to consider labelled cubical sets.
In the above, we have used the notation $L$ to stand for the set of events and the set of labels for those events. It is sometimes useful to make a distinction between the events themselves and their labels and to explicitly give a labelling as a function. This is important, for instance, in treating ‘relabelling’ which leads to categorical fibrational situations (see the paper by Winskel and Nielsen, cited below.) In order to make the distinction clearer, we will replace $L$ by $E$ and refer to its elements as ‘events’ in what follows.
A labelled transition system consists of a transition system $T = (S, i, E, Tran)$ together with a set $L$ of labels, and a function $l : E \to L$. We denote it by $(T,L,l)$.
A morphism, $(\sigma, \tau , \lambda) : (T_1 , L_1 , l_1) \to (T_2 , L_2 , l_2 )$ between labeled transition systems consists of a morphism $(\sigma, \tau) : T_1 \to T_2$ between the underlying transition systems together with a partial function $\lambda : L_1 \to L_2$ such that $l_2 \circ \tau = \lambda \circ l_1$.
We write $LTS$ for the category of labeled transition systems.
The term labelled transition system can also refer to the data of a domain, a set of labels and a transition relation, without any distinguished initial or final sets.
We can view a transition system as a relational structure. The set of states is the ‘set of worlds’ and for each event, $e \in E$ we define a relation $R_e \subseteq S\times S$ by $(s,s')\in R_e$ if and only if, $(s,e,s')\in Trans$. We thus derive a relation for each event and, conversely, if we know the family $\{R_e \mid e\in E\}$, then we can rebuild $Trans$ in the obvious way.
There are tentative definitions of
higher dimensional transition system,
which take a more nPOV of this theory.
Mogens Nielsen, Glynn Winskel: Models for concurrency, in: Handbook of Logic in Computer Science vol 4, Oxford Univ. Press (1994) 1-148 [pdf, pdf, doi:10.5555/218623.218630, ISBN:9780198537809]
Eric Goubault and Samuel Mimram, Formal Relationships Between Geometrical and Classical Models for Concurrency
Discussion in relation to bisimulations and open morphisms:
Last revised on May 15, 2024 at 10:14:33. See the history of this page for a list of all contributions to it.