interpret Parigot's lambda-mu calculus in Haskell

Question

One can interpret the lambda calculus in Haskell:

data Expr = Var String | Lam String Expr | App Expr Expr

data Value a = V a | F (Value a -> Value a)

interpret :: [(String, Value a)] -> Expr -> Value a
interpret env (Var x) = case lookup x env of
  Nothing -> error "undefined variable"
  Just v -> v
interpret env (Lam x e) = F (\v -> interpret ((x, v):env) e)
interpret env (App e1 e2) = case interpret env e1 of
  V _ -> error "not a function"
  F f -> f (interpret env e2)

How could the above interpreter be extended to the lambda-mu calculus? My guess is that it should use continuations for interpreting the additional constructs in this calculus. (15) and (16) from the Bernardi&Moortgat paper are the kind of translations I expect.

It is possible since Haskell is Turing-complete, but how?

Hint: See the comment on page 197 on this research paper for the intuitive meaning of the mu binder.

Answer 1

Here's a mindless transliteration of the reduction rules from the paper, using @user2407038's representation (as you'll see, when I say mindless, I really do mean mindless):

{-# LANGUAGE DataKinds, KindSignatures, GADTs #-}
{-# LANGUAGE StandaloneDeriving #-}

import Control.Monad.Writer
import Control.Applicative
import Data.Monoid

data TermType = Named | Unnamed

type Var = String
type MuVar = String

data Expr (n :: TermType) where
  Var :: Var -> Expr Unnamed
  Lam :: Var -> Expr Unnamed -> Expr Unnamed
  App :: Expr Unnamed -> Expr Unnamed -> Expr Unnamed
  Freeze :: MuVar -> Expr Unnamed -> Expr Named
  Mu :: MuVar -> Expr Named -> Expr Unnamed
deriving instance Show (Expr n)

substU :: Var -> Expr Unnamed -> Expr n -> Expr n
substU x e = go
  where
    go :: Expr n -> Expr n
    go (Var y) = if y == x then e else Var y
    go (Lam y e) = Lam y $ if y == x then e else go e
    go (App f e) = App (go f) (go e)
    go (Freeze alpha e) = Freeze alpha (go e)
    go (Mu alpha u) = Mu alpha (go u)

renameN :: MuVar -> MuVar -> Expr n -> Expr n
renameN beta alpha = go
  where
    go :: Expr n -> Expr n
    go (Var x) = Var x
    go (Lam x e) = Lam x (go e)
    go (App f e) = App (go f) (go e)
    go (Freeze gamma e) = Freeze (if gamma == beta then alpha else gamma) (go e)
    go (Mu gamma u) = Mu gamma $ if gamma == beta then u else go u

appN :: MuVar -> Expr Unnamed -> Expr n -> Expr n
appN beta v = go
  where
    go :: Expr n -> Expr n
    go (Var x) = Var x
    go (Lam x e) = Lam x (go e)
    go (App f e) = App (go f) (go e)
    go (Freeze alpha w) = Freeze alpha $ if alpha == beta then App (go w) v else go w
    go (Mu alpha u) = Mu alpha $ if alpha /= beta then go u else u

reduceTo :: a -> Writer Any a
reduceTo x = tell (Any True) >> return x

reduce0 :: Expr n -> Writer Any (Expr n)
reduce0 (App (Lam x u) v) = reduceTo $ substU x v u
reduce0 (App (Mu beta u) v) = reduceTo $ Mu beta $ appN beta v u
reduce0 (Freeze alpha (Mu beta u)) = reduceTo $ renameN beta alpha u
reduce0 e = return e

reduce1 :: Expr n -> Writer Any (Expr n)
reduce1 (Var x) = return $ Var x
reduce1 (Lam x e) = reduce0 =<< (Lam x <$> reduce1 e)
reduce1 (App f e) = reduce0 =<< (App <$> reduce1 f <*> reduce1 e)
reduce1 (Freeze alpha e) = reduce0 =<< (Freeze alpha <$> reduce1 e)
reduce1 (Mu alpha u) = reduce0 =<< (Mu alpha <$> reduce1 u)

reduce :: Expr n -> Expr n
reduce e = case runWriter (reduce1 e) of
    (e', Any changed) -> if changed then reduce e' else e

It "works" for the example from the paper: with

example 0 = App (App t (Var "x")) (Var "y")
  where
    t = Lam "x" $ Lam "y" $ Mu "delta" $ Freeze "phi" $ App (Var "x") (Var "y")   
example n = App (example (n-1)) (Var ("z_" ++ show n))

I can reduce example n to the expected result:

*Main> reduce (example 10)
Mu "delta" (Freeze "phi" (App (Var "x") (Var "y")))

The reason I put scare quotes around "works" above is that I have no intuition about the λμ calculus so I don't know what it should do.