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CompilerCorrectness chapter: basic simulation and constant folding
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@ -1328,7 +1328,7 @@ If so, our process of \emph{multi-step closure}\index{multi-step closure} has te
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Again, keep in mind that multi-step closure will not terminate for most transition systems, and there is an art to phrasing a problem in terms of systems where it \emph{will} terminate.
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\section{Abstracting a Transition System}
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\section{\label{trs_simulation}Abstracting a Transition System}
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When analyzing an infinite-state system, it is not necessary to give up hope for model checking.
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For instance, consider this program.
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@ -2346,6 +2346,78 @@ That is, the output program has the same traces as the input program.
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For nondeterministic languages, subtler conditions are called for, but we're happy to stay within the safe confines of determinism for this chapter.
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\section{Basic Simulation Arguments and Optimizing Expressions}
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\newcommand{\cfold}[1]{\mathsf{cfold}_1(#1)}
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As our first example compiler phase, we consider a limited form of \emph{constant folding}\index{constant folding}, where expressions with statically known values are replaced by constants.
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The whole of the optimization is (1) finding all maximal program subexpressions that don't contain variables and (2) replacing each such subexpression with its known constant value.
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We write $\cfold{c}$ for the result of applying this optimization on command $c$.
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(For the optimizations in this chapter, we stick to informal descriptions of how they operate, leaving the details to the accompanying Coq code.)
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A program optimized in this way proceeds in a very regular manner, compared to executions of the original, unoptimized program.
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The small steps line up one-to-one.
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Therefore, a very regular kind of \emph{simulation relation} connects them.
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(This notion is very similar to the one from Section \ref{trs_simulation}, though now it incorporates labels.)
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\begin{definition}[Simulation relation]
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We say that binary relation $R$ over states of our object language is a \emph{simulation relation} iff:
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\begin{enumerate}
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\item Whenever $(v_1, \skipe) \; R \; (v_2, c_2)$, it follows that $c_2 = \skipe$.
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\item Whenever $s_1 \; R \; s_2$ and $\smallstepcl{s_1}{\ell}{s'_1}$, there exists $s'_2$ such that $\smallstepcl{s_2}{\ell}{s'_2}$ and $s'_1 \; R \; s'_2$.
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\end{enumerate}
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\end{definition}
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The crucial second condition can be drawn like this.
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\[
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\begin{tikzcd}
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s_1 \arrow{r}{R} \arrow{d}{\forall \to_{\mathsf{c}}} & s_2 \arrow{d}{\exists \to_{\mathsf{c}}} \\
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s'_1 & s'_2 \arrow{l}{R^{-1}}
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\end{tikzcd}
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\]
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\invariants
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As usual, the diagram tells us that when a path along the left exists, a matching roundabout path exists, too.
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That is, any step on the left can be matched by a step on the right.
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Notice the similarity to the invariant-induction principle that we have mostly relied on so far.
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Instead of showing that every step preserves a one-state predicate, we show that every step preserves a two-state predicate in a particular way.
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The simulation approach is as general for relating programs as the invariant approach is for verifying individual programs.
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\begin{theorem}
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If there exists a simulation $R$ such that $s_1 \; R \; s_2$, then $\treq{s_1}{s_2}$.
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\end{theorem}
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\begin{proof}
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We prove the two trace-inclusion directions separately.
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The left-to-right direction proceeds by induction over the definition of traces on the left, while the right-to-left direction proceeds by similar induction on the right.
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While most of the proof is generic in details of the labelled transition system, for the right-to-left direction we do rely on proofs of two important properties of this object language.
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First, the semantics is \emph{total}, in the sense that any state whose command isn't $\skipe$ can take a step.
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Second, the semantics is \emph{deterministic}, in that there can be at most one label/state pair reachable in one step from a particular starting state.
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In the inductive step of the right-to-left inclusion proof, we know that the righthand system has taken a step.
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The lefthand system might already be a $\skipe$, in which case, by the definition of simulations, the righthand system is already a $\skipe$, contradicting the assumption that the righthand side stepped.
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Otherwise, by totality, the lefthand system can take a step.
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By the definition of simulation, there exists a matching step on the righthand side.
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By determinism, the matching step is the same as the one we were already aware of.
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Therefore, we have a new $R$ relationship to connect to that step and apply the induction hypothesis.
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\end{proof}
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We can apply this very general principle to constant folding.
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\begin{theorem}
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For any $v$ and $c$, $\treq{(v, c)}{(v, \cfold{c})}$.
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\end{theorem}
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\begin{proof}
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By a simulation argument using this relation:
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\begin{eqnarray*}
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(v_1, c_1) \; R \; (v_2, c_2) &=& v_1 = v_2 \land c_2 = \cfold{c_1}
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\end{eqnarray*}
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What we have done is translate the original theorem statement into the language of binary relations, as this simple case needs no equivalent of strengthening the induction hypothesis.
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Internally to the proof, we need to define constant folding of evaluation contexts $C$, and we need to prove that primitive steps $\to_0$ may be lifted to apply over constant-folded states, this second proof by case analysis on $\to_0$ derivations.
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Another more obvious workhorse is a lemma showing that constant folding of expressions preserves interpretation results.
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\end{proof}
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\chapter{Lambda Calculus and Simple Type Safety}
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