1 \chapter[chap:normalization]{Normalization}
2 % A helper to print a single example in the half the page width. The example
3 % text should be in a buffer whose name is given in an argument.
5 % The align=right option really does left-alignment, but without the program
6 % will end up on a single line. The strut=no option prevents a bunch of empty
7 % space at the start of the frame.
9 \framed[offset=1mm,align=right,strut=no,background=box,frame=off]{
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12 \setuptyping[option=none,style=\tttf,strip=auto]
16 \define[4]\transexample{
17 \placeexample[here][ex:trans:#1]{#2}
18 \startcombination[2*1]
19 {\example{#3}}{Original program}
20 {\example{#4}}{Transformed program}
24 The first step in the core to \small{VHDL} translation process, is normalization. We
25 aim to bring the core description into a simpler form, which we can
26 subsequently translate into \small{VHDL} easily. This normal form is needed because
27 the full core language is more expressive than \small{VHDL} in some
28 areas (higher-order expressions, limited polymorphism using type
29 classes, etc.) and because core can describe expressions that do not
30 have a direct hardware interpretation.
33 The transformations described here have a well-defined goal: To bring the
34 program in a well-defined form that is directly translatable to
35 \VHDL, while fully preserving the semantics of the program. We refer
36 to this form as the \emph{normal form} of the program. The formal
37 definition of this normal form is quite simple:
39 \placedefinition{}{\startboxed A program is in \emph{normal form} if none of the
40 transformations from this chapter apply.\stopboxed}
42 Of course, this is an \quote{easy} definition of the normal form, since our
43 program will end up in normal form automatically. The more interesting part is
44 to see if this normal form actually has the properties we would like it to
47 But, before getting into more definitions and details about this normal
48 form, let us try to get a feeling for it first. The easiest way to do this
49 is by describing the things that are unwanted in the intended normal form.
52 \item Any \emph{polymorphism} must be removed. When laying down hardware, we
53 cannot generate any signals that can have multiple types. All types must be
54 completely known to generate hardware.
56 \item All \emph{higher-order} constructions must be removed. We cannot
57 generate a hardware signal that contains a function, so all values,
58 arguments and return values used must be first order.
60 \item All complex \emph{nested scopes} must be removed. In the \small{VHDL}
61 description, every signal is in a single scope. Also, full expressions are
62 not supported everywhere (in particular port maps can only map signal
63 names and constants, not complete expressions). To make the \small{VHDL}
64 generation easy, a separate binder must be bound to ever application or
68 \todo{Intermezzo: functions vs plain values}
70 A very simple example of a program in normal form is given in
71 \in{example}[ex:MulSum]. As you can see, all arguments to the function (which
72 will become input ports in the generated \VHDL) are at the outer level.
73 This means that the body of the inner lambda abstraction is never a
74 function, but always a plain value.
76 As the body of the inner lambda abstraction, we see a single (recursive)
77 let expression, that binds two variables (\lam{mul} and \lam{sum}). These
78 variables will be signals in the generated \VHDL, bound to the output port
79 of the \lam{*} and \lam{+} components.
81 The final line (the \quote{return value} of the function) selects the
82 \lam{sum} signal to be the output port of the function. This \quote{return
83 value} can always only be a variable reference, never a more complex
86 \todo{Add generated VHDL}
89 alu :: Bit -> Word -> Word -> Word
98 \startuseMPgraphic{MulSum}
99 save a, b, c, mul, add, sum;
102 newCircle.a(btex $a$ etex) "framed(false)";
103 newCircle.b(btex $b$ etex) "framed(false)";
104 newCircle.c(btex $c$ etex) "framed(false)";
105 newCircle.sum(btex $sum$ etex) "framed(false)";
108 newCircle.mul(btex * etex);
109 newCircle.add(btex + etex);
111 a.c - b.c = (0cm, 2cm);
112 b.c - c.c = (0cm, 2cm);
113 add.c = c.c + (2cm, 0cm);
114 mul.c = midpoint(a.c, b.c) + (2cm, 0cm);
115 sum.c = add.c + (2cm, 0cm);
118 % Draw objects and lines
119 drawObj(a, b, c, mul, add, sum);
121 ncarc(a)(mul) "arcangle(15)";
122 ncarc(b)(mul) "arcangle(-15)";
128 \placeexample[here][ex:MulSum]{Simple architecture consisting of a
129 multiplier and a subtractor.}
130 \startcombination[2*1]
131 {\typebufferlam{MulSum}}{Core description in normal form.}
132 {\boxedgraphic{MulSum}}{The architecture described by the normal form.}
135 \in{Example}[ex:MulSum] showed a function that just applied two
136 other functions (multiplication and addition), resulting in a simple
137 architecture with two components and some connections. There is of
138 course also some mechanism for choice in the normal form. In a
139 normal Core program, the \emph{case} expression can be used in a few
140 different ways to describe choice. In normal form, this is limited
141 to a very specific form.
143 \in{Example}[ex:AddSubAlu] shows an example describing a
144 simple \small{ALU}, which chooses between two operations based on an opcode
145 bit. The main structure is similar to \in{example}[ex:MulSum], but this
146 time the \lam{res} variable is bound to a case expression. This case
147 expression scrutinizes the variable \lam{opcode} (and scrutinizing more
148 complex expressions is not supported). The case expression can select a
149 different variable based on the constructor of \lam{opcode}.
150 \refdef{case expression}
152 \startbuffer[AddSubAlu]
153 alu :: Bit -> Word -> Word -> Word
165 \startuseMPgraphic{AddSubAlu}
166 save opcode, a, b, add, sub, mux, res;
169 newCircle.opcode(btex $opcode$ etex) "framed(false)";
170 newCircle.a(btex $a$ etex) "framed(false)";
171 newCircle.b(btex $b$ etex) "framed(false)";
172 newCircle.res(btex $res$ etex) "framed(false)";
174 newCircle.add(btex + etex);
175 newCircle.sub(btex - etex);
178 opcode.c - a.c = (0cm, 2cm);
179 add.c - a.c = (4cm, 0cm);
180 sub.c - b.c = (4cm, 0cm);
181 a.c - b.c = (0cm, 3cm);
182 mux.c = midpoint(add.c, sub.c) + (1.5cm, 0cm);
183 res.c - mux.c = (1.5cm, 0cm);
186 % Draw objects and lines
187 drawObj(opcode, a, b, res, add, sub, mux);
189 ncline(a)(add) "posA(e)";
190 ncline(b)(sub) "posA(e)";
191 nccurve(a)(sub) "posA(e)", "angleA(0)";
192 nccurve(b)(add) "posA(e)", "angleA(0)";
193 nccurve(add)(mux) "posB(inpa)", "angleB(0)";
194 nccurve(sub)(mux) "posB(inpb)", "angleB(0)";
195 nccurve(opcode)(mux) "posB(n)", "angleA(0)", "angleB(-90)";
196 ncline(mux)(res) "posA(out)";
199 \placeexample[here][ex:AddSubAlu]{Simple \small{ALU} supporting two operations.}
200 \startcombination[2*1]
201 {\typebufferlam{AddSubAlu}}{Core description in normal form.}
202 {\boxedgraphic{AddSubAlu}}{The architecture described by the normal form.}
205 As a more complete example, consider
206 \in{example}[ex:NormalComplete]. This example shows everything that
207 is allowed in normal form, except for built-in higher-order functions
208 (like \lam{map}). The graphical version of the architecture contains
209 a slightly simplified version, since the state tuple packing and
210 unpacking have been left out. Instead, two separate registers are
211 drawn. Most synthesis tools will further optimize this architecture by
212 removing the multiplexers at the register input and instead use the write
213 enable port of the register (when it is available), but we want to show
214 the architecture as close to the description as possible.
216 As you can see from the previous examples, the generation of the final
217 architecture from the normal form is straightforward. In each of the
218 examples, there is a direct match between the normal form structure,
219 the generated VHDL and the architecture shown in the images.
221 \startbuffer[NormalComplete]
224 -> State (Word, Word)
225 -> (State (Word, Word), Word)
227 -- All arguments are an inital lambda (address, data, packed state)
229 -- There are nested let expressions at top level
231 -- Unpack the state by coercion (\eg, cast from
232 -- State (Word, Word) to (Word, Word))
233 s = sp ▶ (Word, Word)
234 -- Extract both registers from the state
235 r1 = case s of (a, b) -> a
236 r2 = case s of (a, b) -> b
237 -- Calling some other user-defined function.
239 -- Conditional connections
251 -- pack the state by coercion (\eg, cast from
252 -- (Word, Word) to State (Word, Word))
253 sp' = s' ▶ State (Word, Word)
254 -- Pack our return value
261 \startuseMPgraphic{NormalComplete}
262 save a, d, r, foo, muxr, muxout, out;
265 newCircle.a(btex \lam{a} etex) "framed(false)";
266 newCircle.d(btex \lam{d} etex) "framed(false)";
267 newCircle.out(btex \lam{out} etex) "framed(false)";
269 %newCircle.add(btex + etex);
270 newBox.foo(btex \lam{foo} etex);
271 newReg.r1(btex $\lam{r1}$ etex) "dx(4mm)", "dy(6mm)";
272 newReg.r2(btex $\lam{r2}$ etex) "dx(4mm)", "dy(6mm)", "reflect(true)";
274 % Reflect over the vertical axis
275 reflectObj(muxr1)((0,0), (0,1));
278 rotateObj(muxout)(-90);
280 d.c = foo.c + (0cm, 1.5cm);
281 a.c = (xpart r2.c + 2cm, ypart d.c - 0.5cm);
282 foo.c = midpoint(muxr1.c, muxr2.c) + (0cm, 2cm);
283 muxr1.c = r1.c + (0cm, 2cm);
284 muxr2.c = r2.c + (0cm, 2cm);
285 r2.c = r1.c + (4cm, 0cm);
287 muxout.c = midpoint(r1.c, r2.c) - (0cm, 2cm);
288 out.c = muxout.c - (0cm, 1.5cm);
290 % % Draw objects and lines
291 drawObj(a, d, foo, r1, r2, muxr1, muxr2, muxout, out);
294 nccurve(foo)(muxr1) "angleA(-90)", "posB(inpa)", "angleB(180)";
295 nccurve(foo)(muxr2) "angleA(-90)", "posB(inpb)", "angleB(0)";
296 nccurve(muxr1)(r1) "posA(out)", "angleA(180)", "posB(d)", "angleB(0)";
297 nccurve(r1)(muxr1) "posA(out)", "angleA(0)", "posB(inpb)", "angleB(180)";
298 nccurve(muxr2)(r2) "posA(out)", "angleA(0)", "posB(d)", "angleB(180)";
299 nccurve(r2)(muxr2) "posA(out)", "angleA(180)", "posB(inpa)", "angleB(0)";
300 nccurve(r1)(muxout) "posA(out)", "angleA(0)", "posB(inpb)", "angleB(-90)";
301 nccurve(r2)(muxout) "posA(out)", "angleA(180)", "posB(inpa)", "angleB(-90)";
303 nccurve(a)(muxout) "angleA(-90)", "angleB(180)", "posB(sel)";
304 nccurve(a)(muxr1) "angleA(180)", "angleB(-90)", "posB(sel)";
305 nccurve(a)(muxr2) "angleA(180)", "angleB(-90)", "posB(sel)";
306 ncline(muxout)(out) "posA(out)";
309 \todo{Don't split registers in this image?}
310 \placeexample[here][ex:NormalComplete]{Simple architecture consisting of an adder and a
312 \startcombination[2*1]
313 {\typebufferlam{NormalComplete}}{Core description in normal form.}
314 {\boxedgraphic{NormalComplete}}{The architecture described by the normal form.}
319 \subsection[sec:normalization:intendednormalform]{Intended normal form definition}
320 Now we have some intuition for the normal form, we can describe how we want
321 the normal form to look like in a slightly more formal manner. The following
322 EBNF-like description captures most of the intended structure (and
323 generates a subset of \GHC's core format).
325 There are two things missing: Cast expressions are sometimes
326 allowed by the prototype, but not specified here and the below
327 definition allows uses of state that cannot be translated to \VHDL\
328 properly. These two problems are discussed in
329 \in{section}[sec:normalization:castproblems] and
330 \in{section}[sec:normalization:stateproblems] respectively.
332 Some clauses have an expression listed behind them in parentheses.
333 These are conditions that need to apply to the clause. The
334 predicates used there (\lam{lvar()}, \lam{representable()},
335 \lam{gvar()}) will be defined in
336 \in{section}[sec:normalization:predicates].
338 An expression is in normal form if it matches the first
339 definition, \emph{normal}.
341 \todo{Fix indentation}
342 \startbuffer[IntendedNormal]
343 \italic{normal} := \italic{lambda}
344 \italic{lambda} := λvar.\italic{lambda} (representable(var))
346 \italic{toplet} := letrec [\italic{binding}...] in var (representable(var))
347 \italic{binding} := var = \italic{rhs} (representable(rhs))
348 -- State packing and unpacking by coercion
349 | var0 = var1 ▶ State ty (lvar(var1))
350 | var0 = var1 ▶ ty (var1 :: State ty ∧ lvar(var1))
351 \italic{rhs} := \italic{userapp}
352 | \italic{builtinapp}
354 | case var of C a0 ... an -> ai (lvar(var))
356 | case var of (lvar(var))
357 [ DEFAULT -> var ] (lvar(var))
358 C0 w0,0 ... w0,n -> var0
360 Cm wm,0 ... wm,n -> varm (\forall{}i \forall{}j, wi,j \neq vari, lvar(vari))
361 \italic{userapp} := \italic{userfunc}
362 | \italic{userapp} {userarg}
363 \italic{userfunc} := var (gvar(var))
364 \italic{userarg} := var (lvar(var))
365 \italic{builtinapp} := \italic{builtinfunc}
366 | \italic{builtinapp} \italic{builtinarg}
367 \italic{built-infunc} := var (bvar(var))
368 \italic{built-inarg} := var (representable(var) ∧ lvar(var))
369 | \italic{partapp} (partapp :: a -> b)
370 | \italic{coreexpr} (¬representable(coreexpr) ∧ ¬(coreexpr :: a -> b))
371 \italic{partapp} := \italic{userapp}
372 | \italic{builtinapp}
375 \placedefinition[][def:IntendedNormal]{Definition of the intended nnormal form using an \small{EBNF}-like syntax.}
376 {\defref{intended normal form definition}
377 \typebufferlam{IntendedNormal}}
379 When looking at such a program from a hardware perspective, the
380 top level lambda abstractions define the input ports. Lambda
381 abstractions cannot appear anywhere else. The variable reference
382 in the body of the recursive let expression is the output port.
383 Most function applications bound by the let expression define a
384 component instantiation, where the input and output ports are
385 mapped to local signals or arguments. Some of the others use a
386 built-in construction (\eg\ the \lam{case} expression) or call a
387 built-in function (\eg\ \lam{+} or \lam{map}). For these, a
388 hardcoded \small{VHDL} translation is available.
390 \section[sec:normalization:transformation]{Transformation notation}
391 To be able to concisely present transformations, we use a specific format
392 for them. It is a simple format, similar to one used in logic reasoning.
394 Such a transformation description looks like the following.
399 <original expression>
400 -------------------------- <expression conditions>
401 <transformed expression>
406 This format describes a transformation that applies to \lam{<original
407 expression>} and transforms it into \lam{<transformed expression>}, assuming
408 that all conditions are satisfied. In this format, there are a number of placeholders
409 in pointy brackets, most of which should be rather obvious in their meaning.
410 Nevertheless, we will more precisely specify their meaning below:
412 \startdesc{<original expression>} The expression pattern that will be matched
413 against (subexpressions of) the expression to be transformed. We call this a
414 pattern, because it can contain \emph{placeholders} (variables), which match
415 any expression or binder. Any such placeholder is said to be \emph{bound} to
416 the expression it matches. It is convention to use an uppercase letter (\eg\
417 \lam{M} or \lam{E}) to refer to any expression (including a simple variable
418 reference) and lowercase letters (\eg\ \lam{v} or \lam{b}) to refer to
419 (references to) binders.
421 For example, the pattern \lam{a + B} will match the expression
422 \lam{v + (2 * w)} (binding \lam{a} to \lam{v} and \lam{B} to
423 \lam{(2 * w)}), but not \lam{(2 * w) + v}.
426 \startdesc{<expression conditions>}
427 These are extra conditions on the expression that is matched. These
428 conditions can be used to further limit the cases in which the
429 transformation applies, commonly to prevent a transformation from
430 causing a loop with itself or another transformation.
432 Only if these conditions are \emph{all} satisfied, the transformation
436 \startdesc{<context conditions>}
437 These are a number of extra conditions on the context of the function. In
438 particular, these conditions can require some (other) top level function to be
439 present, whose value matches the pattern given here. The format of each of
440 these conditions is: \lam{binder = <pattern>}.
442 Typically, the binder is some placeholder bound in the \lam{<original
443 expression>}, while the pattern contains some placeholders that are used in
444 the \lam{transformed expression}.
446 Only if a top level binder exists that matches each binder and pattern,
447 the transformation applies.
450 \startdesc{<transformed expression>}
451 This is the expression template that is the result of the transformation. If, looking
452 at the above three items, the transformation applies, the \lam{<original
453 expression>} is completely replaced by the \lam{<transformed expression>}.
454 We call this a template, because it can contain placeholders, referring to
455 any placeholder bound by the \lam{<original expression>} or the
456 \lam{<context conditions>}. The resulting expression will have those
457 placeholders replaced by the values bound to them.
459 Any binder (lowercase) placeholder that has no value bound to it yet will be
460 bound to (and replaced with) a fresh binder.
463 \startdesc{<context additions>}
464 These are templates for new functions to be added to the context.
465 This is a way to let a transformation create new top level
468 Each addition has the form \lam{binder = template}. As above, any
469 placeholder in the addition is replaced with the value bound to it, and any
470 binder placeholder that has no value bound to it yet will be bound to (and
471 replaced with) a fresh binder.
474 To understand this notation better, the step by step application of
475 the η-abstraction transformation to a simple \small{ALU} will be
476 shown. Consider η-abstraction, which is a common transformation from
477 labmda calculus, described using above notation as follows:
481 -------------- \lam{E} does not occur on a function position in an application
482 λx.E x \lam{E} is not a lambda abstraction.
485 η-abstraction is a well known transformation from lambda calculus. What
486 this transformation does, is take any expression that has a function type
487 and turn it into a lambda expression (giving an explicit name to the
488 argument). There are some extra conditions that ensure that this
489 transformation does not apply infinitely (which are not necessarily part
490 of the conventional definition of η-abstraction).
492 Consider the following function, in Core notation, which is a fairly obvious way to specify a
493 simple \small{ALU} (Note that it is not yet in normal form, but
494 \in{example}[ex:AddSubAlu] shows the normal form of this function).
495 The parentheses around the \lam{+} and \lam{-} operators are
496 commonly used in Haskell to show that the operators are used as
497 normal functions, instead of \emph{infix} operators (\eg, the
498 operators appear before their arguments, instead of in between).
501 alu :: Bit -> Word -> Word -> Word
502 alu = λopcode. case opcode of
507 There are a few subexpressions in this function to which we could possibly
508 apply the transformation. Since the pattern of the transformation is only
509 the placeholder \lam{E}, any expression will match that. Whether the
510 transformation applies to an expression is thus solely decided by the
511 conditions to the right of the transformation.
513 We will look at each expression in the function in a top down manner. The
514 first expression is the entire expression the function is bound to.
517 λopcode. case opcode of
522 As said, the expression pattern matches this. The type of this expression is
523 \lam{Bit -> Word -> Word -> Word}, which matches \lam{a -> b} (Note that in
524 this case \lam{a = Bit} and \lam{b = Word -> Word -> Word}).
526 Since this expression is at top level, it does not occur at a function
527 position of an application. However, The expression is a lambda abstraction,
528 so this transformation does not apply.
530 The next expression we could apply this transformation to, is the body of
531 the lambda abstraction:
539 The type of this expression is \lam{Word -> Word -> Word}, which again
540 matches \lam{a -> b}. The expression is the body of a lambda expression, so
541 it does not occur at a function position of an application. Finally, the
542 expression is not a lambda abstraction but a case expression, so all the
543 conditions match. There are no context conditions to match, so the
544 transformation applies.
546 By now, the placeholder \lam{E} is bound to the entire expression. The
547 placeholder \lam{x}, which occurs in the replacement template, is not bound
548 yet, so we need to generate a fresh binder for that. Let us use the binder
549 \lam{a}. This results in the following replacement expression:
557 Continuing with this expression, we see that the transformation does not
558 apply again (it is a lambda expression). Next we look at the body of this
567 Here, the transformation does apply, binding \lam{E} to the entire
568 expression (which has type \lam{Word -> Word}) and binding \lam{x}
569 to the fresh binder \lam{b}, resulting in the replacement:
577 The transformation does not apply to this lambda abstraction, so we
578 look at its body. For brevity, we will put the case expression on one line from
582 (case opcode of Low -> (+); High -> (-)) a b
585 The type of this expression is \lam{Word}, so it does not match \lam{a -> b}
586 and the transformation does not apply. Next, we have two options for the
587 next expression to look at: The function position and argument position of
588 the application. The expression in the argument position is \lam{b}, which
589 has type \lam{Word}, so the transformation does not apply. The expression in
590 the function position is:
593 (case opcode of Low -> (+); High -> (-)) a
596 Obviously, the transformation does not apply here, since it occurs in
597 function position (which makes the second condition false). In the same
598 way the transformation does not apply to both components of this
599 expression (\lam{case opcode of Low -> (+); High -> (-)} and \lam{a}), so
600 we will skip to the components of the case expression: The scrutinee and
601 both alternatives. Since the opcode is not a function, it does not apply
604 The first alternative is \lam{(+)}. This expression has a function type
605 (the operator still needs two arguments). It does not occur in function
606 position of an application and it is not a lambda expression, so the
607 transformation applies.
609 We look at the \lam{<original expression>} pattern, which is \lam{E}.
610 This means we bind \lam{E} to \lam{(+)}. We then replace the expression
611 with the \lam{<transformed expression>}, replacing all occurences of
612 \lam{E} with \lam{(+)}. In the \lam{<transformed expression>}, the This gives us the replacement expression:
613 \lam{λx.(+) x} (A lambda expression binding \lam{x}, with a body that
614 applies the addition operator to \lam{x}).
616 The complete function then becomes:
618 (case opcode of Low -> λa1.(+) a1; High -> (-)) a
621 Now the transformation no longer applies to the complete first alternative
622 (since it is a lambda expression). It does not apply to the addition
623 operator again, since it is now in function position in an application. It
624 does, however, apply to the application of the addition operator, since
625 that is neither a lambda expression nor does it occur in function
626 position. This means after one more application of the transformation, the
630 (case opcode of Low -> λa1.λb1.(+) a1 b1; High -> (-)) a
633 The other alternative is left as an exercise to the reader. The final
634 function, after applying η-abstraction until it does no longer apply is:
637 alu :: Bit -> Word -> Word -> Word
638 alu = λopcode.λa.b. (case opcode of
639 Low -> λa1.λb1 (+) a1 b1
640 High -> λa2.λb2 (-) a2 b2) a b
643 \subsection{Transformation application}
644 In this chapter we define a number of transformations, but how will we apply
645 these? As stated before, our normal form is reached as soon as no
646 transformation applies anymore. This means our application strategy is to
647 simply apply any transformation that applies, and continuing to do that with
648 the result of each transformation.
650 In particular, we define no particular order of transformations. Since
651 transformation order should not influence the resulting normal form,
652 this leaves the implementation free to choose any application order that
653 results in an efficient implementation. Unfortunately this is not
654 entirely true for the current set of transformations. See
655 \in{section}[sec:normalization:non-determinism] for a discussion of this
658 When applying a single transformation, we try to apply it to every (sub)expression
659 in a function, not just the top level function body. This allows us to
660 keep the transformation descriptions concise and powerful.
662 \subsection{Definitions}
663 A \emph{global variable} is any variable (binder) that is bound at the
664 top level of a program, or an external module. A \emph{local variable} is any
665 other variable (\eg, variables local to a function, which can be bound by
666 lambda abstractions, let expressions and pattern matches of case
667 alternatives). This is a slightly different notion of global versus
668 local than what \small{GHC} uses internally, but for our purposes
669 the distinction \GHC\ makes is not useful.
670 \defref{global variable} \defref{local variable}
672 A \emph{hardware representable} (or just \emph{representable}) type or value
673 is (a value of) a type that we can generate a signal for in hardware. For
674 example, a bit, a vector of bits, a 32 bit unsigned word, etc. Values that are
675 not runtime representable notably include (but are not limited to): Types,
676 dictionaries, functions.
677 \defref{representable}
679 A \emph{built-in function} is a function supplied by the Cλash framework, whose
680 implementation is not valid Cλash. The implementation is of course valid
681 Haskell, for simulation, but it is not expressable in Cλash.
682 \defref{built-in function} \defref{user-defined function}
684 For these functions, Cλash has a \emph{built-in hardware translation}, so calls
685 to these functions can still be translated. These are functions like
686 \lam{map}, \lam{hwor} and \lam{length}.
688 A \emph{user-defined} function is a function for which we do have a Cλash
689 implementation available.
691 \subsubsection[sec:normalization:predicates]{Predicates}
692 Here, we define a number of predicates that can be used below to concisely
695 \emph{gvar(expr)} is true when \emph{expr} is a variable that references a
696 global variable. It is false when it references a local variable.
698 \emph{lvar(expr)} is the complement of \emph{gvar}; it is true when \emph{expr}
699 references a local variable, false when it references a global variable.
701 \emph{representable(expr)} is true when \emph{expr} is \emph{representable}.
703 \subsection[sec:normalization:uniq]{Binder uniqueness}
704 A common problem in transformation systems, is binder uniqueness. When not
705 considering this problem, it is easy to create transformations that mix up
706 bindings and cause name collisions. Take for example, the following core
710 (λa.λb.λc. a * b * c) x c
713 By applying β-reduction (see \in{section}[sec:normalization:beta]) once,
714 we can simplify this expression to:
720 Now, we have replaced the \lam{a} binder with a reference to the \lam{x}
721 binder. No harm done here. But note that we see multiple occurences of the
722 \lam{c} binder. The first is a binding occurence, to which the second refers.
723 The last, however refers to \emph{another} instance of \lam{c}, which is
724 bound somewhere outside of this expression. Now, if we would apply beta
725 reduction without taking heed of binder uniqueness, we would get:
731 This is obviously not what was supposed to happen! The root of this problem is
732 the reuse of binders: Identical binders can be bound in different,
733 but overlapping scopes. Any variable reference in those
734 overlapping scopes then refers to the variable bound in the inner
735 (smallest) scope. There is not way to refer to the variable in the
736 outer scope. This effect is usually referred to as
737 \emph{shadowing}: When a binder is bound in a scope where the
738 binder already had a value, the inner binding is said to
739 \emph{shadow} the outer binding. In the example above, the \lam{c}
740 binder was bound outside of the expression and in the inner lambda
741 expression. Inside that lambda expression, only the inner \lam{c}
744 There are a number of ways to solve this. \small{GHC} has isolated this
745 problem to their binder substitution code, which performs \emph{deshadowing}
746 during its expression traversal. This means that any binding that shadows
747 another binding on a higher level is replaced by a new binder that does not
748 shadow any other binding. This non-shadowing invariant is enough to prevent
749 binder uniqueness problems in \small{GHC}.
751 In our transformation system, maintaining this non-shadowing invariant is
752 a bit harder to do (mostly due to implementation issues, the prototype
753 does not use \small{GHC}'s subsitution code). Also, the following points
757 \item Deshadowing does not guarantee overall uniqueness. For example, the
758 following (slightly contrived) expression shows the identifier \lam{x} bound in
759 two seperate places (and to different values), even though no shadowing
763 (let x = 1 in x) + (let x = 2 in x)
766 \item In our normal form (and the resulting \small{VHDL}), all binders
767 (signals) within the same function (entity) will end up in the same
768 scope. To allow this, all binders within the same function should be
771 \item When we know that all binders in an expression are unique, moving around
772 or removing a subexpression will never cause any binder conflicts. If we have
773 some way to generate fresh binders, introducing new subexpressions will not
774 cause any problems either. The only way to cause conflicts is thus to
775 duplicate an existing subexpression.
778 Given the above, our prototype maintains a unique binder invariant. This
779 means that in any given moment during normalization, all binders \emph{within
780 a single function} must be unique. To achieve this, we apply the following
783 \todo{Define fresh binders and unique supplies}
786 \item Before starting normalization, all binders in the function are made
787 unique. This is done by generating a fresh binder for every binder used. This
788 also replaces binders that did not cause any conflict, but it does ensure that
789 all binders within the function are generated by the same unique supply.
790 \refdef{fresh binder}
791 \item Whenever a new binder must be generated, we generate a fresh binder that
792 is guaranteed to be different from \emph{all binders generated so far}. This
793 can thus never introduce duplication and will maintain the invariant.
794 \item Whenever (a part of) an expression is duplicated (for example when
795 inlining), all binders in the expression are replaced with fresh binders
796 (using the same method as at the start of normalization). These fresh binders
797 can never introduce duplication, so this will maintain the invariant.
798 \item Whenever we move part of an expression around within the function, there
799 is no need to do anything special. There is obviously no way to introduce
800 duplication by moving expressions around. Since we know that each of the
801 binders is already unique, there is no way to introduce (incorrect) shadowing
805 \section{Transform passes}
806 In this section we describe the actual transforms.
808 Each transformation will be described informally first, explaining
809 the need for and goal of the transformation. Then, we will formally define
810 the transformation using the syntax introduced in
811 \in{section}[sec:normalization:transformation].
813 \subsection{General cleanup}
814 These transformations are general cleanup transformations, that aim to
815 make expressions simpler. These transformations usually clean up the
816 mess left behind by other transformations or clean up expressions to
817 expose new transformation opportunities for other transformations.
819 Most of these transformations are standard optimizations in other
820 compilers as well. However, in our compiler, most of these are not just
821 optimizations, but they are required to get our program into intended
825 \defref{substitution notation}
826 \startframedtext[width=8cm,background=box,frame=no]
827 \startalignment[center]
828 {\tfa Substitution notation}
832 In some of the transformations in this chapter, we need to perform
833 substitution on an expression. Substitution means replacing every
834 occurence of some expression (usually a variable reference) with
837 There have been a lot of different notations used in literature for
838 specifying substitution. The notation that will be used in this report
845 This means expression \lam{E} with all occurences of \lam{A} replaced
850 \subsubsection[sec:normalization:beta]{β-reduction}
851 β-reduction is a well known transformation from lambda calculus, where it is
852 the main reduction step. It reduces applications of lambda abstractions,
853 removing both the lambda abstraction and the application.
855 In our transformation system, this step helps to remove unwanted lambda
856 abstractions (basically all but the ones at the top level). Other
857 transformations (application propagation, non-representable inlining) make
858 sure that most lambda abstractions will eventually be reducable by
861 Note that β-reduction also works on type lambda abstractions and type
862 applications as well. This means the substitution below also works on
863 type variables, in the case that the binder is a type variable and teh
864 expression applied to is a type.
881 \transexample{beta}{β-reduction}{from}{to}
891 \transexample{beta-type}{β-reduction for type abstractions}{from}{to}
893 \subsubsection{Unused let binding removal}
894 This transformation removes let bindings that are never used.
895 Occasionally, \GHC's desugarer introduces some unused let bindings.
897 This normalization pass should really be not be necessary to get
898 into intended normal form (since the intended normal form
899 definition \refdef{intended normal form definition} does not
900 require that every binding is used), but in practice the
901 desugarer or simplifier emits some bindings that cannot be
902 normalized (e.g., calls to a
903 \hs{Control.Exception.Base.patError}) but are not used anywhere
904 either. To prevent the \VHDL\ generation from breaking on these
905 artifacts, this transformation removes them.
907 \todo{Do not use old-style numerals in transformations}
916 M \lam{ai} does not occur free in \lam{M}
917 ---------------------------- \lam{\forall j, 0 ≤ j ≤ n, j ≠ i} (\lam{ai} does not occur free in \lam{Ej})
943 \transexample{unusedlet}{Unused let binding removal}{from}{to}
945 \subsubsection{Empty let removal}
946 This transformation is simple: It removes recursive lets that have no bindings
947 (which usually occurs when unused let binding removal removes the last
950 Note that there is no need to define this transformation for
951 non-recursive lets, since they always contain exactly one binding.
970 \transexample{emptylet}{Empty let removal}{from}{to}
972 \subsubsection[sec:normalization:simplelet]{Simple let binding removal}
973 This transformation inlines simple let bindings, that bind some
974 binder to some other binder instead of a more complex expression (\ie\
977 This transformation is not needed to get an expression into intended
978 normal form (since these bindings are part of the intended normal
979 form), but makes the resulting \small{VHDL} a lot shorter.
981 \refdef{substitution notation}
991 ----------------------------- \lam{b} is a variable reference
992 letrec \lam{ai} ≠ \lam{b}
1005 \subsubsection{Cast propagation / simplification}
1006 This transform pushes casts down into the expression as far as
1007 possible. This transformation has been added to make a few
1008 specific corner cases work, but it is not clear yet if this
1009 transformation handles cast expressions completely or in the
1010 right way. See \in{section}[sec:normalization:castproblems].
1013 (let binds in E) ▶ T
1014 -------------------------
1015 let binds in (E ▶ T)
1024 -------------------------
1031 \subsubsection{Top level binding inlining}
1032 \refdef{top level binding}
1033 This transform takes simple top level bindings generated by the
1034 \small{GHC} compiler. \small{GHC} sometimes generates very simple
1035 \quote{wrapper} bindings, which are bound to just a variable
1036 reference, or contain just a (partial) function appliation with
1037 the type and dictionary arguments filled in (such as the
1038 \lam{(+)} in the example below).
1040 Note that this transformation is completely optional. It is not
1041 required to get any function into intended normal form, but it does help making
1042 the resulting VHDL output easier to read (since it removes components
1043 that do not add any real structure, but do hide away operations and
1044 cause extra clutter).
1046 This transform takes any top level binding generated by \GHC,
1047 whose normalized form contains only a single let binding.
1050 x = λa0 ... λan.let y = E in y
1053 -------------------------------------- \lam{x} is generated by the compiler
1054 λa0 ... λan.let y = E in y
1058 (+) :: Word -> Word -> Word
1059 (+) = GHC.Num.(+) @Word \$dNum
1064 GHC.Num.(+) @ Alu.Word \$dNum a b
1067 \transexample{toplevelinline}{Top level binding inlining}{from}{to}
1069 \in{Example}[ex:trans:toplevelinline] shows a typical application of
1070 the addition operator generated by \GHC. The type and dictionary
1071 arguments used here are described in
1072 \in{Section}[section:prototype:polymorphism].
1074 Without this transformation, there would be a \lam{(+)} entity
1075 in the \VHDL\ which would just add its inputs. This generates a
1076 lot of overhead in the \VHDL, which is particularly annoying
1077 when browsing the generated RTL schematic (especially since most
1078 non-alphanumerics, like all characters in \lam{(+)}, are not
1079 allowed in \VHDL\ architecture names\footnote{Technically, it is
1080 allowed to use non-alphanumerics when using extended
1081 identifiers, but it seems that none of the tooling likes
1082 extended identifiers in filenames, so it effectively does not
1083 work.}, so the entity would be called \quote{w7aA7f} or
1084 something similarly meaningless and autogenerated).
1086 \subsection{Program structure}
1087 These transformations are aimed at normalizing the overall structure
1088 into the intended form. This means ensuring there is a lambda abstraction
1089 at the top for every argument (input port or current state), putting all
1090 of the other value definitions in let bindings and making the final
1091 return value a simple variable reference.
1093 \subsubsection[sec:normalization:eta]{η-abstraction}
1094 This transformation makes sure that all arguments of a function-typed
1095 expression are named, by introducing lambda expressions. When combined with
1096 β-reduction and non-representable binding inlining, all function-typed
1097 expressions should be lambda abstractions or global identifiers.
1101 -------------- \lam{E} does not occur on a function position in an application
1102 λx.E x \lam{E} is not a lambda abstraction.
1112 foo = λa.λx.(case a of
1117 \transexample{eta}{η-abstraction}{from}{to}
1119 \subsubsection[sec:normalization:appprop]{Application propagation}
1120 This transformation is meant to propagate application expressions downwards
1121 into expressions as far as possible. This allows partial applications inside
1122 expressions to become fully applied and exposes new transformation
1123 opportunities for other transformations (like β-reduction and
1126 Since all binders in our expression are unique (see
1127 \in{section}[sec:normalization:uniq]), there is no risk that we will
1128 introduce unintended shadowing by moving an expression into a lower
1129 scope. Also, since only move expression into smaller scopes (down into
1130 our expression), there is no risk of moving a variable reference out
1131 of the scope in which it is defined.
1134 (letrec binds in E) M
1135 ------------------------
1155 \transexample{appproplet}{Application propagation for a let expression}{from}{to}
1183 \transexample{apppropcase}{Application propagation for a case expression}{from}{to}
1185 \subsubsection[sec:normalization:letrecurse]{Let recursification}
1186 This transformation makes all non-recursive lets recursive. In the
1187 end, we want a single recursive let in our normalized program, so all
1188 non-recursive lets can be converted. This also makes other
1189 transformations simpler: They only need to be specified for recursive
1190 let expressions (and simply will not apply to non-recursive let
1191 expressions until this transformation has been applied).
1198 ------------------------------------------
1205 \subsubsection{Let flattening}
1206 This transformation puts nested lets in the same scope, by lifting the
1207 binding(s) of the inner let into the outer let. Eventually, this will
1208 cause all let bindings to appear in the same scope.
1210 This transformation only applies to recursive lets, since all
1211 non-recursive lets will be made recursive (see
1212 \in{section}[sec:normalization:letrecurse]).
1214 Since we are joining two scopes together, there is no risk of moving a
1215 variable reference out of the scope where it is defined.
1221 ai = (letrec bindings in M)
1226 ------------------------------------------
1261 \transexample{letflat}{Let flattening}{from}{to}
1263 \subsubsection{Return value simplification}
1264 This transformation ensures that the return value of a function is always a
1265 simple local variable reference.
1267 This transformation only applies to the entire body of a
1268 function instead of any subexpression in a function. This is
1269 achieved by the contexts, like \lam{x = E}, though this is
1270 strictly not correct (you could read this as "if there is any
1271 function \lam{x} that binds \lam{E}, any \lam{E} can be
1272 transformed, while we only mean the \lam{E} that is bound by
1275 Note that the return value is not simplified if its not
1276 representable. Otherwise, this would cause a direct loop with
1277 the inlining of unrepresentable bindings. If the return value is
1278 not representable because it has a function type, η-abstraction
1279 should make sure that this transformation will eventually apply.
1280 If the value is not representable for other reasons, the
1281 function result itself is not representable, meaning this
1282 function is not translatable anyway.
1285 x = E \lam{E} is representable
1286 ~ \lam{E} is not a lambda abstraction
1287 E \lam{E} is not a let expression
1288 --------------------------- \lam{E} is not a local variable reference
1294 ~ \lam{E} is representable
1295 E \lam{E} is not a let expression
1296 --------------------------- \lam{E} is not a local variable reference
1301 x = λv0 ... λvn.let ... in E
1302 ~ \lam{E} is representable
1303 E \lam{E} is not a local variable reference
1304 -----------------------------
1313 x = letrec x = add 1 2 in x
1316 \transexample{retvalsimpl}{Return value simplification}{from}{to}
1318 \todo{More examples}
1320 \subsection[sec:normalization:argsimpl]{Representable arguments simplification}
1321 This section contains just a single transformation that deals with
1322 representable arguments in applications. Non-representable arguments are
1323 handled by the transformations in
1324 \in{section}[sec:normalization:nonrep].
1326 This transformation ensures that all representable arguments will become
1327 references to local variables. This ensures they will become references
1328 to local signals in the resulting \small{VHDL}, which is required due to
1329 limitations in the component instantiation code in \VHDL\ (one can only
1330 assign a signal or constant to an input port). By ensuring that all
1331 arguments are always simple variable references, we always have a signal
1332 available to map to the input ports.
1334 To reduce a complex expression to a simple variable reference, we create
1335 a new let expression around the application, which binds the complex
1336 expression to a new variable. The original function is then applied to
1339 \refdef{global variable}
1340 Note that references to \emph{global variables} (like a top level
1341 function without arguments, but also an argumentless dataconstructors
1342 like \lam{True}) are also simplified. Only local variables generate
1343 signals in the resulting architecture. Even though argumentless
1344 dataconstructors generate constants in generated \VHDL\ code and could be
1345 mapped to an input port directly, they are still simplified to make the
1346 normal form more regular.
1348 \refdef{representable}
1351 -------------------- \lam{N} is representable
1352 letrec x = N in M x \lam{N} is not a local variable reference
1354 \refdef{local variable}
1361 letrec x = add a 1 in add x 1
1364 \transexample{argsimpl}{Argument simplification}{from}{to}
1366 \subsection[sec:normalization:built-ins]{Built-in functions}
1367 This section deals with (arguments to) built-in functions. In the
1368 intended normal form definition\refdef{intended normal form definition}
1369 we can see that there are three sorts of arguments a built-in function
1373 \item A representable local variable reference. This is the most
1374 common argument to any function. The argument simplification
1375 transformation described in \in{section}[sec:normalization:argsimpl]
1376 makes sure that \emph{any} representable argument to \emph{any}
1377 function (including built-in functions) is turned into a local variable
1379 \item (A partial application of) a top level function (either built-in on
1380 user-defined). The function extraction transformation described in
1381 this section takes care of turning every functiontyped argument into
1382 (a partial application of) a top level function.
1383 \item Any expression that is not representable and does not have a
1384 function type. Since these can be any expression, there is no
1385 transformation needed. Note that this category is exactly all
1386 expressions that are not transformed by the transformations for the
1387 previous two categories. This means that \emph{any} core expression
1388 that is used as an argument to a built-in function will be either
1389 transformed into one of the above categories, or end up in this
1390 categorie. In any case, the result is in normal form.
1393 As noted, the argument simplification will handle any representable
1394 arguments to a built-in function. The following transformation is needed
1395 to handle non-representable arguments with a function type, all other
1396 non-representable arguments do not need any special handling.
1398 \subsubsection[sec:normalization:funextract]{Function extraction}
1399 This transform deals with function-typed arguments to built-in
1401 Since built-in functions cannot be specialized (see
1402 \in{section}[sec:normalization:specialize]) to remove the arguments,
1403 these arguments are extracted into a new global function instead. In
1404 other words, we create a new top level function that has exactly the
1405 extracted argument as its body. This greatly simplifies the
1406 translation rules needed for built-in functions, since they only need
1407 to handle (partial applications of) top level functions.
1409 Any free variables occuring in the extracted arguments will become
1410 parameters to the new global function. The original argument is replaced
1411 with a reference to the new function, applied to any free variables from
1412 the original argument.
1414 This transformation is useful when applying higher-order built-in functions
1415 like \hs{map} to a lambda abstraction, for example. In this case, the code
1416 that generates \small{VHDL} for \hs{map} only needs to handle top level functions and
1417 partial applications, not any other expression (such as lambda abstractions or
1418 even more complicated expressions).
1421 M N \lam{M} is (a partial aplication of) a built-in function.
1422 --------------------- \lam{f0 ... fn} are all free local variables of \lam{N}
1423 M (x f0 ... fn) \lam{N :: a -> b}
1424 ~ \lam{N} is not a (partial application of) a top level function
1429 addList = λb.λxs.map (λa . add a b) xs
1433 addList = λb.λxs.map (f b) xs
1438 \transexample{funextract}{Function extraction}{from}{to}
1440 Note that the function \lam{f} will still need normalization after
1443 \subsection{Case normalisation}
1444 The transformations in this section ensure that case statements end up
1447 \subsubsection{Scrutinee simplification}
1448 This transform ensures that the scrutinee of a case expression is always
1449 a simple variable reference.
1454 ----------------- \lam{E} is not a local variable reference
1473 \transexample{letflat}{Case normalisation}{from}{to}
1477 \defref{wild binders}
1478 \startframedtext[width=7cm,background=box,frame=no]
1479 \startalignment[center]
1483 In a functional expression, a \emph{wild binder} refers to any
1484 binder that is never referenced. This means that even though it
1485 will be bound to a particular value, that value is never used.
1487 The Haskell syntax offers the underscore as a wild binder that
1488 cannot even be referenced (It can be seen as introducing a new,
1489 anonymous, binder everytime it is used).
1491 In these transformations, the term wild binder will sometimes be
1492 used to indicate that a binder must not be referenced.
1496 \subsubsection{Case normalization}
1497 This transformation ensures that all case expressions get a form
1498 that is allowed by the intended normal form. This means they
1502 \item An extractor case with a single alternative that picks a field
1503 from a datatype, \eg\ \lam{case x of (a, b) -> a}.
1504 \item A selector case with multiple alternatives and only wild binders, that
1505 makes a choice between expressions based on the constructor of another
1506 expression, \eg\ \lam{case x of Low -> a; High -> b}.
1509 For an arbitrary case, that has \lam{n} alternatives, with
1510 \lam{m} binders in each alternatives, this will result in \lam{m
1511 * n} extractor case expression to get at each variable, \lam{n}
1512 let bindings for each of the alternatives' value and a single
1513 selector case to select the right value out of these.
1515 Technically, the defintion of this transformation would require
1516 that the constructor for every alternative has exactly the same
1517 amount (\lam{m}) of arguments, but of course this transformation
1518 also applies when this is not the case.
1522 C0 v0,0 ... v0,m -> E0
1524 Cn vn,0 ... vn,m -> En
1525 --------------------------------------------------- \lam{\forall i \forall j, 0 ≤ i ≤ n, 0 ≤ i < m} (\lam{wi,j} is a wild (unused) binder)
1526 letrec The case expression is not an extractor case
1527 v0,0 = case E of C0 x0,0 .. x0,m -> x0,0 The case expression is not a selector case
1529 v0,m = case E of C0 x0,0 .. x0,m -> x0,m
1531 vn,m = case E of Cn xn,0 .. xn,m -> xn,m
1537 C0 w0,0 ... w0,m -> y0
1539 Cn wn,0 ... wn,m -> yn
1542 Note that this transformation applies to case expressions with any
1543 scrutinee. If the scrutinee is a complex expression, this might
1544 result in duplication of work (hardware). An extra condition to
1545 only apply this transformation when the scrutinee is already
1546 simple (effectively causing this transformation to be only
1547 applied after the scrutinee simplification transformation) might
1566 \transexample{selcasesimpl}{Selector case simplification}{from}{to}
1574 b = case a of (,) b c -> b
1575 c = case a of (,) b c -> c
1582 \transexample{excasesimpl}{Extractor case simplification}{from}{to}
1584 \refdef{selector case}
1585 In \in{example}[ex:trans:excasesimpl] the case expression is expanded
1586 into multiple case expressions, including a pretty useless expression
1587 (that is neither a selector or extractor case). This case can be
1588 removed by the Case removal transformation in
1589 \in{section}[sec:transformation:caseremoval].
1591 \subsubsection[sec:transformation:caseremoval]{Case removal}
1592 This transform removes any case expression with a single alternative and
1593 only wild binders.\refdef{wild binder}
1595 These "useless" case expressions are usually leftovers from case simplification
1596 on extractor case (see the previous example).
1601 ---------------------- \lam{\forall i, 0 ≤ i ≤ m} (\lam{vi} does not occur free in E)
1614 \transexample{caserem}{Case removal}{from}{to}
1616 \subsection[sec:normalization:nonrep]{Removing unrepresentable values}
1617 The transformations in this section are aimed at making all the
1618 values used in our expression representable. There are two main
1619 transformations that are applied to \emph{all} unrepresentable let
1620 bindings and function arguments. These are meant to address three
1621 different kinds of unrepresentable values: Polymorphic values,
1622 higher-order values and literals. The transformation are described
1623 generically: They apply to all non-representable values. However,
1624 non-representable values that do not fall into one of these three
1625 categories will be moved around by these transformations but are
1626 unlikely to completely disappear. They usually mean the program was not
1627 valid in the first place, because unsupported types were used (for
1628 example, a program using strings).
1630 Each of these three categories will be detailed below, followed by the
1631 actual transformations.
1633 \subsubsection{Removing Polymorphism}
1634 As noted in \in{section}[sec:prototype:polymporphism],
1635 polymorphism is made explicit in Core through type and
1636 dictionary arguments. To remove the polymorphism from a
1637 function, we can simply specialize the polymorphic function for
1638 the particular type applied to it. The same goes for dictionary
1639 arguments. To remove polymorphism from let bound values, we
1640 simply inline the let bindings that have a polymorphic type,
1641 which should (eventually) make sure that the polymorphic
1642 expression is applied to a type and/or dictionary, which can
1643 then be removed by β-reduction (\in{section}[sec:normalization:beta]).
1645 Since both type and dictionary arguments are not representable,
1646 \refdef{representable}
1647 the non-representable argument specialization and
1648 non-representable let binding inlining transformations below
1649 take care of exactly this.
1651 There is one case where polymorphism cannot be completely
1652 removed: Built-in functions are still allowed to be polymorphic
1653 (Since we have no function body that we could properly
1654 specialize). However, the code that generates \VHDL\ for built-in
1655 functions knows how to handle this, so this is not a problem.
1657 \subsubsection[sec:normalization:defunctionalization]{Defunctionalization}
1658 These transformations remove higher-order expressions from our
1659 program, making all values first-order. The approach used for
1660 defunctionalization uses a combination of specialization, inlining and
1661 some cleanup transformations, was also proposed in parallel research
1662 by Neil Mitchell \cite[mitchell09].
1664 Higher order values are always introduced by lambda abstractions, none
1665 of the other Core expression elements can introduce a function type.
1666 However, other expressions can \emph{have} a function type, when they
1667 have a lambda expression in their body.
1669 For example, the following expression is a higher-order expression
1670 that is not a lambda expression itself:
1672 \refdef{id function}
1679 The reference to the \lam{id} function shows that we can introduce a
1680 higher-order expression in our program without using a lambda
1681 expression directly. However, inside the definition of the \lam{id}
1682 function, we can be sure that a lambda expression is present.
1684 Looking closely at the definition of our normal form in
1685 \in{section}[sec:normalization:intendednormalform], we can see that
1686 there are three possibilities for higher-order values to appear in our
1687 intended normal form:
1690 \item[item:toplambda] Lambda abstractions can appear at the highest level of a
1691 top level function. These lambda abstractions introduce the
1692 arguments (input ports / current state) of the function.
1693 \item[item:built-inarg] (Partial applications of) top level functions can appear as an
1694 argument to a built-in function.
1695 \item[item:completeapp] (Partial applications of) top level functions can appear in
1696 function position of an application. Since a partial application
1697 cannot appear anywhere else (except as built-in function arguments),
1698 all partial applications are applied, meaning that all applications
1699 will become complete applications. However, since application of
1700 arguments happens one by one, in the expression:
1704 the subexpression \lam{f 1} has a function type. But this is
1705 allowed, since it is inside a complete application.
1708 We will take a typical function with some higher-order values as an
1709 example. The following function takes two arguments: a \lam{Bit} and a
1710 list of numbers. Depending on the first argument, each number in the
1711 list is doubled, or the list is returned unmodified. For the sake of
1712 the example, no polymorphism is shown. In reality, at least map would
1716 λy.let double = λx. x + x in
1722 This example shows a number of higher-order values that we cannot
1723 translate to \VHDL\ directly. The \lam{double} binder bound in the let
1724 expression has a function type, as well as both of the alternatives of
1725 the case expression. The first alternative is a partial application of
1726 the \lam{map} built-in function, whereas the second alternative is a
1729 To reduce all higher-order values to one of the above items, a number
1730 of transformations we have already seen are used. The η-abstraction
1731 transformation from \in{section}[sec:normalization:eta] ensures all
1732 function arguments are introduced by lambda abstraction on the highest
1733 level of a function. These lambda arguments are allowed because of
1734 \in{item}[item:toplambda] above. After η-abstraction, our example
1735 becomes a bit bigger:
1738 λy.λq.(let double = λx. x + x in
1745 η-abstraction also introduces extra applications (the application of
1746 the let expression to \lam{q} in the above example). These
1747 applications can then propagated down by the application propagation
1748 transformation (\in{section}[sec:normalization:appprop]). In our
1749 example, the \lam{q} and \lam{r} variable will be propagated into the
1750 let expression and then into the case expression:
1753 λy.λq.let double = λx. x + x in
1759 This propagation makes higher-order values become applied (in
1760 particular both of the alternatives of the case now have a
1761 representable type). Completely applied top level functions (like the
1762 first alternative) are now no longer invalid (they fall under
1763 \in{item}[item:completeapp] above). (Completely) applied lambda
1764 abstractions can be removed by β-abstraction. For our example,
1765 applying β-abstraction results in the following:
1768 λy.λq.let double = λx. x + x in
1774 As you can see in our example, all of this moves applications towards
1775 the higher-order values, but misses higher-order functions bound by
1776 let expressions. The applications cannot be moved towards these values
1777 (since they can be used in multiple places), so the values will have
1778 to be moved towards the applications. This is achieved by inlining all
1779 higher-order values bound by let applications, by the
1780 non-representable binding inlining transformation below. When applying
1781 it to our example, we get the following:
1785 Low -> map (λx. x + x) q
1789 We have nearly eliminated all unsupported higher-order values from this
1790 expressions. The one that is remaining is the first argument to the
1791 \lam{map} function. Having higher-order arguments to a built-in
1792 function like \lam{map} is allowed in the intended normal form, but
1793 only if the argument is a (partial application) of a top level
1794 function. This is easily done by introducing a new top level function
1795 and put the lambda abstraction inside. This is done by the function
1796 extraction transformation from
1797 \in{section}[sec:normalization:funextract].
1805 This also introduces a new function, that we have called \lam{func}:
1811 Note that this does not actually remove the lambda, but now it is a
1812 lambda at the highest level of a function, which is allowed in the
1813 intended normal form.
1815 There is one case that has not been discussed yet. What if the
1816 \lam{map} function in the example above was not a built-in function
1817 but a user-defined function? Then extracting the lambda expression
1818 into a new function would not be enough, since user-defined functions
1819 can never have higher-order arguments. For example, the following
1820 expression shows an example:
1823 twice :: (Word -> Word) -> Word -> Word
1824 twice = λf.λa.f (f a)
1826 main = λa.app (λx. x + x) a
1829 This example shows a function \lam{twice} that takes a function as a
1830 first argument and applies that function twice to the second argument.
1831 Again, we have made the function monomorphic for clarity, even though
1832 this function would be a lot more useful if it was polymorphic. The
1833 function \lam{main} uses \lam{twice} to apply a lambda epression twice.
1835 When faced with a user defined function, a body is available for that
1836 function. This means we could create a specialized version of the
1837 function that only works for this particular higher-order argument
1838 (\ie, we can just remove the argument and call the specialized
1839 function without the argument). This transformation is detailed below.
1840 Applying this transformation to the example gives:
1843 twice' :: Word -> Word
1844 twice' = λb.(λf.λa.f (f a)) (λx. x + x) b
1849 The \lam{main} function is now in normal form, since the only
1850 higher-order value there is the top level lambda expression. The new
1851 \lam{twice'} function is a bit complex, but the entire original body
1852 of the original \lam{twice} function is wrapped in a lambda
1853 abstraction and applied to the argument we have specialized for
1854 (\lam{λx. x + x}) and the other arguments. This complex expression can
1855 fortunately be effectively reduced by repeatedly applying β-reduction:
1858 twice' :: Word -> Word
1859 twice' = λb.(b + b) + (b + b)
1862 This example also shows that the resulting normal form might not be as
1863 efficient as we might hope it to be (it is calculating \lam{(b + b)}
1864 twice). This is discussed in more detail in
1865 \in{section}[sec:normalization:duplicatework].
1867 \subsubsection{Literals}
1868 There are a limited number of literals available in Haskell and Core.
1869 \refdef{enumerated types} When using (enumerating) algebraic
1870 datatypes, a literal is just a reference to the corresponding data
1871 constructor, which has a representable type (the algebraic datatype)
1872 and can be translated directly. This also holds for literals of the
1873 \hs{Bool} Haskell type, which is just an enumerated type.
1875 There is, however, a second type of literal that does not have a
1876 representable type: Integer literals. Cλash supports using integer
1877 literals for all three integer types supported (\hs{SizedWord},
1878 \hs{SizedInt} and \hs{RangedWord}). This is implemented using
1879 Haskell's \hs{Num} type class, which offers a \hs{fromInteger} method
1880 that converts any \hs{Integer} to the Cλash datatypes.
1882 When \GHC\ sees integer literals, it will automatically insert calls to
1883 the \hs{fromInteger} method in the resulting Core expression. For
1884 example, the following expression in Haskell creates a 32 bit unsigned
1885 word with the value 1. The explicit type signature is needed, since
1886 there is no context for \GHC\ to determine the type from otherwise.
1892 This Haskell code results in the following Core expression:
1895 fromInteger @(SizedWord D32) \$dNum (smallInteger 10)
1898 The literal 10 will have the type \lam{GHC.Prim.Int\#}, which is
1899 converted into an \lam{Integer} by \lam{smallInteger}. Finally, the
1900 \lam{fromInteger} function will finally convert this into a
1901 \lam{SizedWord D32}.
1903 Both the \lam{GHC.Prim.Int\#} and \lam{Integer} types are not
1904 representable, and cannot be translated directly. Fortunately, there
1905 is no need to translate them, since \lam{fromInteger} is a built-in
1906 function that knows how to handle these values. However, this does
1907 require that the \lam{fromInteger} function is directly applied to
1908 these non-representable literal values, otherwise errors will occur.
1909 For example, the following expression is not in the intended normal
1910 form, since one of the let bindings has an unrepresentable type
1914 let l = smallInteger 10 in fromInteger @(SizedWord D32) \$dNum l
1917 By inlining these let-bindings, we can ensure that unrepresentable
1918 literals bound by a let binding end up in an application of the
1919 appropriate built-in function, where they are allowed. Since it is
1920 possible that the application of that function is in a different
1921 function than the definition of the literal value, we will always need
1922 to specialize away any unrepresentable literals that are used as
1923 function arguments. The following two transformations do exactly this.
1925 \subsubsection{Non-representable binding inlining}
1926 This transform inlines let bindings that are bound to a
1927 non-representable value. Since we can never generate a signal
1928 assignment for these bindings (we cannot declare a signal assignment
1929 with a non-representable type, for obvious reasons), we have no choice
1930 but to inline the binding to remove it.
1932 As we have seen in the previous sections, inlining these bindings
1933 solves (part of) the polymorphism, higher-order values and
1934 unrepresentable literals in an expression.
1936 \refdef{substitution notation}
1946 -------------------------- \lam{Ei} has a non-representable type.
1948 a0 = E0 [ai=>Ei] \vdots
1949 ai-1 = Ei-1 [ai=>Ei]
1950 ai+1 = Ei+1 [ai=>Ei]
1969 x = fromInteger (smallInteger 10)
1971 (λb -> add b 1) (add 1 x)
1974 \transexample{nonrepinline}{Nonrepresentable binding inlining}{from}{to}
1976 \subsubsection[sec:normalization:specialize]{Function specialization}
1977 This transform removes arguments to user-defined functions that are
1978 not representable at runtime. This is done by creating a
1979 \emph{specialized} version of the function that only works for one
1980 particular value of that argument (in other words, the argument can be
1983 Specialization means to create a specialized version of the called
1984 function, with one argument already filled in. As a simple example, in
1985 the following program (this is not actual Core, since it directly uses
1986 a literal with the unrepresentable type \lam{GHC.Prim.Int\#}).
1993 We could specialize the function \lam{f} against the literal argument
1994 1, with the following result:
2001 In some way, this transformation is similar to β-reduction, but it
2002 operates across function boundaries. It is also similar to
2003 non-representable let binding inlining above, since it sort of
2004 \quote{inlines} an expression into a called function.
2006 Special care must be taken when the argument has any free variables.
2007 If this is the case, the original argument should not be removed
2008 completely, but replaced by all the free variables of the expression.
2009 In this way, the original expression can still be evaluated inside the
2012 To prevent us from propagating the same argument over and over, a
2013 simple local variable reference is not propagated (since is has
2014 exactly one free variable, itself, we would only replace that argument
2017 This shows that any free local variables that are not runtime
2018 representable cannot be brought into normal form by this transform. We
2019 rely on an inlining or β-reduction transformation to replace such a
2020 variable with an expression we can propagate again.
2025 x Y0 ... Yi ... Yn \lam{Yi} is not representable
2026 --------------------------------------------- \lam{Yi} is not a local variable reference
2027 x' Y0 ... Yi-1 f0 ... fm Yi+1 ... Yn \lam{f0 ... fm} are all free local vars of \lam{Yi}
2028 ~ \lam{T0 ... Tn} are the types of \lam{Y0 ... Yn}
2029 x' = λ(y0 :: T0) ... λ(yi-1 :: Ty-1).
2031 λ(yi+1 :: Ty+1) ... λ(yn :: Tn).
2032 E y0 ... yi-1 Yi yi+1 ... yn
2035 This is a bit of a complex transformation. It transforms an
2036 application of the function \lam{x}, where one of the arguments
2037 (\lam{Y_i}) is not representable. A new
2038 function \lam{x'} is created that wraps the body of the old function.
2039 The body of the new function becomes a number of nested lambda
2040 abstractions, one for each of the original arguments that are left
2043 The ith argument is replaced with the free variables of
2044 \lam{Y_i}. Note that we reuse the same binders as those used in
2045 \lam{Y_i}, since we can then just use \lam{Y_i} inside the new
2046 function body and have all of the variables it uses be in scope.
2048 The argument that we are specializing for, \lam{Y_i}, is put inside
2049 the new function body. The old function body is applied to it. Since
2050 we use this new function only in place of an application with that
2051 particular argument \lam{Y_i}, behaviour should not change.
2053 Note that the types of the arguments of our new function are taken
2054 from the types of the \emph{actual} arguments (\lam{T0 ... Tn}). This
2055 means that any polymorphism in the arguments is removed, even when the
2056 corresponding explicit type lambda is not removed
2059 \todo{Examples. Perhaps reference the previous sections}
2061 \section{Unsolved problems}
2062 The above system of transformations has been implemented in the prototype
2063 and seems to work well to compile simple and more complex examples of
2064 hardware descriptions. \todo{Ref christiaan?} However, this normalization
2065 system has not seen enough review and work to be complete and work for
2066 every Core expression that is supplied to it. A number of problems
2067 have already been identified and are discussed in this section.
2069 \subsection[sec:normalization:duplicatework]{Work duplication}
2070 A possible problem of β-reduction is that it could duplicate work.
2071 When the expression applied is not a simple variable reference, but
2072 requires calculation and the binder the lambda abstraction binds to
2073 is used more than once, more hardware might be generated than strictly
2076 As an example, consider the expression:
2082 When applying β-reduction to this expression, we get:
2088 which of course calculates \lam{(a * b)} twice.
2090 A possible solution to this would be to use the following alternative
2091 transformation, which is of course no longer normal β-reduction. The
2092 followin transformation has not been tested in the prototype, but is
2093 given here for future reference:
2101 This does not seem like much of an improvement, but it does get rid of
2102 the lambda expression (and the associated higher-order value), while
2103 at the same time introducing a new let binding. Since the result of
2104 every application or case expression must be bound by a let expression
2105 in the intended normal form anyway, this is probably not a problem. If
2106 the argument happens to be a variable reference, then simple let
2107 binding removal (\in{section}[sec:normalization:simplelet]) will
2108 remove it, making the result identical to that of the original
2109 β-reduction transformation.
2111 When also applying argument simplification to the above example, we
2112 get the following expression:
2120 Looking at this, we could imagine an alternative approach: Create a
2121 transformation that removes let bindings that bind identical values.
2122 In the above expression, the \lam{y} and \lam{z} variables could be
2123 merged together, resulting in the more efficient expression:
2126 let y = (a * b) in y + y
2129 \subsection[sec:normalization:non-determinism]{Non-determinism}
2130 As an example, again consider the following expression:
2136 We can apply both β-reduction (\in{section}[sec:normalization:beta])
2137 as well as argument simplification
2138 (\in{section}[sec:normalization:argsimpl]) to this expression.
2140 When applying argument simplification first and then β-reduction, we
2141 get the following expression:
2144 let y = (a * b) in y + y
2147 When applying β-reduction first and then argument simplification, we
2148 get the following expression:
2156 As you can see, this is a different expression. This means that the
2157 order of expressions, does in fact change the resulting normal form,
2158 which is something that we would like to avoid. In this particular
2159 case one of the alternatives is even clearly more efficient, so we
2160 would of course like the more efficient form to be the normal form.
2162 For this particular problem, the solutions for duplication of work
2163 seem from the previous section seem to fix the determinism of our
2164 transformation system as well. However, it is likely that there are
2165 other occurences of this problem.
2167 \subsection[sec:normalization:castproblems]{Casts}
2168 We do not fully understand the use of cast expressions in Core, so
2169 there are probably expressions involving cast expressions that cannot
2170 be brought into intended normal form by this transformation system.
2172 The uses of casts in the core system should be investigated more and
2173 transformations will probably need updating to handle them in all
2176 \subsection[sec:normalization:stateproblems]{Normalization of stateful descriptions}
2177 Currently, the intended normal form definition\refdef{intended
2178 normal form definition} offers enough freedom to describe all
2179 valid stateful descriptions, but is not limiting enough. It is
2180 possible to write descriptions which are in intended normal
2181 form, but cannot be translated into \VHDL\ in a meaningful way
2182 (\eg, a function that swaps two substates in its result, or a
2183 function that changes a substate itself instead of passing it to
2186 It is now up to the programmer to not do anything funny with
2187 these state values, whereas the normalization just tries not to
2188 mess up the flow of state values. In practice, there are
2189 situations where a Core program that \emph{could} be a valid
2190 stateful description is not translateable by the prototype. This
2191 most often happens when statefulness is mixed with pattern
2192 matching, causing a state input to be unpacked multiple times or
2193 be unpacked and repacked only in some of the code paths.
2195 Without going into detail about the exact problems (of which
2196 there are probably more than have shown up so far), it seems
2197 unlikely that these problems can be solved entirely by just
2198 improving the \VHDL\ state generation in the final stage. The
2199 normalization stage seems the best place to apply the rewriting
2200 needed to support more complex stateful descriptions. This does
2201 of course mean that the intended normal form definition must be
2202 extended as well to be more specific about how state handling
2203 should look like in normal form.
2204 \in{Section}[sec:prototype:statelimits] already contains a
2205 tight description of the limitations on the use of state
2206 variables, which could be adapted into the intended normal form.
2208 \section[sec:normalization:properties]{Provable properties}
2209 When looking at the system of transformations outlined above, there are a
2210 number of questions that we can ask ourselves. The main question is of course:
2211 \quote{Does our system work as intended?}. We can split this question into a
2212 number of subquestions:
2215 \item[q:termination] Does our system \emph{terminate}? Since our system will
2216 keep running as long as transformations apply, there is an obvious risk that
2217 it will keep running indefinitely. This typically happens when one
2218 transformation produces a result that is transformed back to the original
2219 by another transformation, or when one or more transformations keep
2220 expanding some expression.
2221 \item[q:soundness] Is our system \emph{sound}? Since our transformations
2222 continuously modify the expression, there is an obvious risk that the final
2223 normal form will not be equivalent to the original program: Its meaning could
2225 \item[q:completeness] Is our system \emph{complete}? Since we have a complex
2226 system of transformations, there is an obvious risk that some expressions will
2227 not end up in our intended normal form, because we forgot some transformation.
2228 In other words: Does our transformation system result in our intended normal
2229 form for all possible inputs?
2230 \item[q:determinism] Is our system \emph{deterministic}? Since we have defined
2231 no particular order in which the transformation should be applied, there is an
2232 obvious risk that different transformation orderings will result in
2233 \emph{different} normal forms. They might still both be intended normal forms
2234 (if our system is \emph{complete}) and describe correct hardware (if our
2235 system is \emph{sound}), so this property is less important than the previous
2236 three: The translator would still function properly without it.
2239 Unfortunately, the final transformation system has only been
2240 developed in the final part of the research, leaving no more time
2241 for verifying these properties. In fact, it is likely that the
2242 current transformation system still violates some of these
2243 properties in some cases and should be improved (or extra conditions
2244 on the input hardware descriptions should be formulated).
2246 This is most likely the case with the completeness and determinism
2247 properties, perhaps als the termination property. The soundness
2248 property probably holds, since it is easier to manually verify (each
2249 transformation can be reviewed separately).
2251 Even though no complete proofs have been made, some ideas for
2252 possible proof strategies are shown below.
2254 \subsection{Graph representation}
2255 Before looking into how to prove these properties, we will look at
2256 transformation systems from a graph perspective. We will first define
2257 the graph view and then illustrate it using a simple example from lambda
2258 calculus (which is a different system than the Cλash normalization
2259 system). The nodes of the graph are all possible Core expressions. The
2260 (directed) edges of the graph are transformations. When a transformation
2261 α applies to an expression \lam{A} to produce an expression \lam{B}, we
2262 add an edge from the node for \lam{A} to the node for \lam{B}, labeled
2265 \startuseMPgraphic{TransformGraph}
2269 newCircle.a(btex \lam{(λx.λy. (+) x y) 1} etex);
2270 newCircle.b(btex \lam{λy. (+) 1 y} etex);
2271 newCircle.c(btex \lam{(λx.(+) x) 1} etex);
2272 newCircle.d(btex \lam{(+) 1} etex);
2275 c.c = b.c + (4cm, 0cm);
2276 a.c = midpoint(b.c, c.c) + (0cm, 4cm);
2277 d.c = midpoint(b.c, c.c) - (0cm, 3cm);
2279 % β-conversion between a and b
2280 ncarc.a(a)(b) "name(bred)";
2281 ObjLabel.a(btex $\xrightarrow[normal]{}{β}$ etex) "labpathname(bred)", "labdir(rt)";
2282 ncarc.b(b)(a) "name(bexp)", "linestyle(dashed withdots)";
2283 ObjLabel.b(btex $\xleftarrow[normal]{}{β}$ etex) "labpathname(bexp)", "labdir(lft)";
2285 % η-conversion between a and c
2286 ncarc.a(a)(c) "name(ered)";
2287 ObjLabel.a(btex $\xrightarrow[normal]{}{η}$ etex) "labpathname(ered)", "labdir(rt)";
2288 ncarc.c(c)(a) "name(eexp)", "linestyle(dashed withdots)";
2289 ObjLabel.c(btex $\xleftarrow[normal]{}{η}$ etex) "labpathname(eexp)", "labdir(lft)";
2291 % η-conversion between b and d
2292 ncarc.b(b)(d) "name(ered)";
2293 ObjLabel.b(btex $\xrightarrow[normal]{}{η}$ etex) "labpathname(ered)", "labdir(rt)";
2294 ncarc.d(d)(b) "name(eexp)", "linestyle(dashed withdots)";
2295 ObjLabel.d(btex $\xleftarrow[normal]{}{η}$ etex) "labpathname(eexp)", "labdir(lft)";
2297 % β-conversion between c and d
2298 ncarc.c(c)(d) "name(bred)";
2299 ObjLabel.c(btex $\xrightarrow[normal]{}{β}$ etex) "labpathname(bred)", "labdir(rt)";
2300 ncarc.d(d)(c) "name(bexp)", "linestyle(dashed withdots)";
2301 ObjLabel.d(btex $\xleftarrow[normal]{}{β}$ etex) "labpathname(bexp)", "labdir(lft)";
2303 % Draw objects and lines
2304 drawObj(a, b, c, d);
2307 \placeexample[right][ex:TransformGraph]{Partial graph of a lambda calculus
2308 system with β and η reduction (solid lines) and expansion (dotted lines).}
2309 \boxedgraphic{TransformGraph}
2311 Of course the graph for Cλash is unbounded, since we can construct an
2312 infinite amount of Core expressions. Also, there might potentially be
2313 multiple edges between two given nodes (with different labels), though
2314 this seems unlikely to actually happen in our system.
2316 See \in{example}[ex:TransformGraph] for the graph representation of a very
2317 simple lambda calculus that contains just the expressions \lam{(λx.λy. (+) x
2318 y) 1}, \lam{λy. (+) 1 y}, \lam{(λx.(+) x) 1} and \lam{(+) 1}. The
2319 transformation system consists of β-reduction and η-reduction (solid edges) or
2320 β-expansion and η-expansion (dotted edges).
2322 \todo{Define β-reduction and η-reduction?}
2324 Note that the normal form of such a system consists of the set of nodes
2325 (expressions) without outgoing edges, since those are the expressions to which
2326 no transformation applies anymore. We call this set of nodes the \emph{normal
2327 set}. The set of nodes containing expressions in intended normal
2328 form \refdef{intended normal form} is called the \emph{intended
2331 From such a graph, we can derive some properties easily:
2333 \item A system will \emph{terminate} if there is no walk (sequence of
2334 edges, or transformations) of infinite length in the graph (this
2335 includes cycles, but can also happen without cycles).
2336 \item Soundness is not easily represented in the graph.
2337 \item A system is \emph{complete} if all of the nodes in the normal set have
2338 the intended normal form. The inverse (that all of the nodes outside of
2339 the normal set are \emph{not} in the intended normal form) is not
2340 strictly required. In other words, our normal set must be a
2341 subset of the intended normal form, but they do not need to be
2344 \item A system is deterministic if all paths starting at a particular
2345 node, which end in a node in the normal set, end at the same node.
2348 When looking at the \in{example}[ex:TransformGraph], we see that the system
2349 terminates for both the reduction and expansion systems (but note that, for
2350 expansion, this is only true because we have limited the possible
2351 expressions. In complete lambda calculus, there would be a path from
2352 \lam{(λx.λy. (+) x y) 1} to \lam{(λx.λy.(λz.(+) z) x y) 1} to
2353 \lam{(λx.λy.(λz.(λq.(+) q) z) x y) 1} etc.)
2355 If we would consider the system with both expansion and reduction, there
2356 would no longer be termination either, since there would be cycles all
2359 The reduction and expansion systems have a normal set of containing just
2360 \lam{(+) 1} or \lam{(λx.λy. (+) x y) 1} respectively. Since all paths in
2361 either system end up in these normal forms, both systems are \emph{complete}.
2362 Also, since there is only one node in the normal set, it must obviously be
2363 \emph{deterministic} as well.
2365 \subsection{Termination}
2366 In general, proving termination of an arbitrary program is a very
2367 hard problem. \todo{Ref about arbitrary termination} Fortunately,
2368 we only have to prove termination for our specific transformation
2371 A common approach for these kinds of proofs is to associate a
2372 measure with each possible expression in our system. If we can
2373 show that each transformation strictly decreases this measure
2374 (\ie, the expression transformed to has a lower measure than the
2375 expression transformed from). \todo{ref about measure-based
2376 termination proofs / analysis}
2378 A good measure for a system consisting of just β-reduction would
2379 be the number of lambda expressions in the expression. Since every
2380 application of β-reduction removes a lambda abstraction (and there
2381 is always a bounded number of lambda abstractions in every
2382 expression) we can easily see that a transformation system with
2383 just β-reduction will always terminate.
2385 For our complete system, this measure would be fairly complex
2386 (probably the sum of a lot of things). Since the (conditions on)
2387 our transformations are pretty complex, we would need to include
2388 both simple things like the number of let expressions as well as
2389 more complex things like the number of case expressions that are
2390 not yet in normal form.
2392 No real attempt has been made at finding a suitable measure for
2395 \subsection{Soundness}
2396 Soundness is a property that can be proven for each transformation
2397 separately. Since our system only runs separate transformations
2398 sequentially, if each of our transformations leaves the
2399 \emph{meaning} of the expression unchanged, then the entire system
2400 will of course leave the meaning unchanged and is thus
2403 The current prototype has only been verified in an ad-hoc fashion
2404 by inspecting (the code for) each transformation. A more formal
2405 verification would be more appropriate.
2407 To be able to formally show that each transformation properly
2408 preserves the meaning of every expression, we require an exact
2409 definition of the \emph{meaning} of every expression, so we can
2410 compare them. A definition of the operational semantics of \GHC's Core
2411 language is available \cite[sulzmann07], but this does not seem
2412 sufficient for our goals (but it is a good start).
2414 It should be possible to have a single formal definition of
2415 meaning for Core for both normal Core compilation by \GHC\ and for
2416 our compilation to \VHDL. The main difference seems to be that in
2417 hardware every expression is always evaluated, while in software
2418 it is only evaluated if needed, but it should be possible to
2419 assign a meaning to core expressions that assumes neither.
2421 Since each of the transformations can be applied to any
2422 subexpression as well, there is a constraint on our meaning
2423 definition: The meaning of an expression should depend only on the
2424 meaning of subexpressions, not on the expressions themselves. For
2425 example, the meaning of the application in \lam{f (let x = 4 in
2426 x)} should be the same as the meaning of the application in \lam{f
2427 4}, since the argument subexpression has the same meaning (though
2428 the actual expression is different).
2430 \subsection{Completeness}
2431 Proving completeness is probably not hard, but it could be a lot
2432 of work. We have seen above that to prove completeness, we must
2433 show that the normal set of our graph representation is a subset
2434 of the intended normal set.
2436 However, it is hard to systematically generate or reason about the
2437 normal set, since it is defined as any nodes to which no
2438 transformation applies. To determine this set, each transformation
2439 must be considered and when a transformation is added, the entire
2440 set should be re-evaluated. This means it is hard to show that
2441 each node in the normal set is also in the intended normal set.
2442 Reasoning about our intended normal set is easier, since we know
2443 how to generate it from its definition. \refdef{intended normal
2446 Fortunately, we can also prove the complement (which is
2447 equivalent, since $A \subseteq B \Leftrightarrow \overline{B}
2448 \subseteq \overline{A}$): Show that the set of nodes not in
2449 intended normal form is a subset of the set of nodes not in normal
2450 form. In other words, show that for every expression that is not
2451 in intended normal form, that there is at least one transformation
2452 that applies to it (since that means it is not in normal form
2453 either and since $A \subseteq C \Leftrightarrow \forall x (x \in A
2454 \rightarrow x \in C)$).
2456 By systematically reviewing the entire Core language definition
2457 along with the intended normal form definition (both of which have
2458 a similar structure), it should be possible to identify all
2459 possible (sets of) core expressions that are not in intended
2460 normal form and identify a transformation that applies to it.
2462 This approach is especially useful for proving completeness of our
2463 system, since if expressions exist to which none of the
2464 transformations apply (\ie\ if the system is not yet complete), it
2465 is immediately clear which expressions these are and adding
2466 (or modifying) transformations to fix this should be relatively
2469 As observed above, applying this approach is a lot of work, since
2470 we need to check every (set of) transformation(s) separately.
2472 \todo{Perhaps do a few steps of the proofs as proof-of-concept}
2474 % vim: set sw=2 sts=2 expandtab: