Beautiful differentiation

Lately I’ve been playing again with parametric surfaces in Haskell. Surface rendering requires normals, which can be constructed from partial derivatives, which brings up automatic differentiation (AD). Playing with some refactoring, I’ve stumbled across a terser, lovelier formulation for the derivative rules than I’ve seen before.

Edits:

Automatic differentiation

The idea of AD is to simultaneously manipulate values and derivatives. Overloading of the standard numerical operations (and literals) makes this combined manipulation as simple and pretty as manipulating values without derivatives.

In Functional Differentiation of Computer Programs, Jerzy Karczmarczuk extended the usual trick to a “lazy tower of derivatives”. He exploited Haskell’s laziness to carry infinitely many derivatives, rather than just one. Lennart Augustsson’s AD post contains a summary of Jerzy’s idea and an application. I’ll use some of the details from Lennart’s version, for simplicity.

For some perspectives on the mathematical structuure under AD, see sigfpe’s AD post, and Non-standard analysis, automatic differentiation, Haskell, and other stories.

Representation and overloadings

The tower of derivatives can be represented as an infinite list. Since we’ll use operator overloadings that are not meaningful for lists in general, let’s instead define a new data type:

data Dif a = D a (Dif a)

Given a function f :: a -> Dif b, f a has the form D x (D x' (D x'' ...)), where x is the value at a, and x', x'' …, are the derivatives (first, second, …) at a.

Constant functions have all derivatives equal to zero.

dConst :: Num a => a -> Dif a
dConst x = D x dZero
 
dZero :: Num a => Dif a
dZero = D 0 dZero

Numeric overloadings then are simple. For instance,

instance Num a => Num (Dif a) where
  fromInteger a           = dConst (fromInteger a)
  D x x’ + D y y’         = D (x + y) (x’ + y’)
  D x x’ - D y y’         = D (x - y) (x’ - y’)
  p@(D x x’) * q@(D y y’) = D (x * y) (x’ * q + p * y’)

In each of the right-hand sides of these last three definitions, the first argument to D is constructed using Num a, while the second argument is recursively constructed using Num (Dif a).

Jerzy’s paper uses a function to provide all of the derivatives of a given function (called dlift from Section 3.3):

lift :: Num a => [a -> a] -> Dif a -> Dif a
lift (f : f’) p@(D x x’) = D (f x) (x’ * lift f’ p)

The given list of functions are all of the derivatives of a given function. Then, derivative towers can be constructed by definitions like the following:

instance Floating a => Floating (Dif a) where
  pi               = dConst pi
  exp (D x x’)     = r where r = D (exp x) (x’ * r)
  log p@(D x x’)   = D (log x) (x’ / p)
  sqrt (D x x’)    = r where r = D (sqrt x) (x’ / (2 * r))
  sin              = lift (cycle [sin, cos, negate . sin, negate . cos])
  cos              = lift (cycle [cos, negate . sin, negate . cos, sin])
  asin p@(D x x’)  = D (asin x) ( x’ / sqrt(1 - sqr p))
  acos p@(D x x’)  = D (acos x) (-x’ / sqrt(1 - sqr p))
  atan p@(D x x’)  = D (atan x) ( x’ / (sqr p - 1))
 
sqr :: Num a => a -> a
sqr x = x*x

Reintroducing the chain rule

The code above, which corresponds to section 3 of Jerzy’s paper, is fairly compact. It can be made prettier, however, which is the point of this blog post.

First, let’s simplify the lift so that it expresses the chain rule directly. In fact, this definition is just like dlift from Section 2 (not Section 3) of Jerzy’s paper. It’s the same code, but at a different type, here being used to manipulate infinite derivative towers instead of just value and derivative.

dlift :: Num a => (a -> a) -> (Dif a -> Dif a) -> Dif a -> Dif a
dlift f d = \ p@(D u u’) -> D (f u) (d p * u’)

This operator lets us write simpler definitions.

instance Floating a => Floating (Dif a) where
  pi    = dConst pi
  exp   = dlift exp exp
  log   = dlift log recip
  sqrt  = dlift sqrt (recip . (2*) . sqrt)
  sin   = dlift sin cos
  cos   = dlift cos (negate . sin)
  asin  = dlift asin (\ x -> recip (sqrt (1 - sqr x)))
  acos  = dlift acos (\ x -> - recip (sqrt (1 - sqr x)))
  atan  = dlift atan (\ x -> recip (sqr x + 1))
  sinh  = dlift sinh cosh
  cosh  = dlift cosh sinh
  asinh = dlift asinh (\ x -> recip (sqrt (sqr x + 1)))
  acosh = dlift acosh (\ x -> - recip (sqrt (sqr x - 1)))
  atanh = dlift atanh (\ x -> recip (1 - sqr x))

The necessary recursion has moved out of the lifting function into the class instance (second argument to dlift).

Notice that dlift and the Floating instance are the same code (with minor variations) as in Jerzy’s section two. In that section, however, the code computes only first derivatives, while here, we’re computing all of them.

Prettier still, with function-level overloading

The last steps are cosmetic. The goal is to make the derivative functions used with lift easier to read and write.

Just as we’ve overloaded numeric operations for derivative towers (Dif), let’s also overload them for functions. This trick is often used informally in math. For instance, given functions f and g, one might write f + g to mean \ x -> f x + g x. Using applicative functor notation makes these instances a breeze to define:

instance Num b => Num (a->b) where
  fromInteger = pure . fromInteger
  (+)         = liftA2 (+)
  (*)         = liftA2 (*)
  negate      = fmap negate
  abs         = fmap abs
  signum      = fmap signum

The other numeric class instances are analogous. (Any applicative functor can be given these same instance definitions.)

As a final touch, define an infix operator to replace the name “dlift“:

infix 0 >-<
(>-<) = dlift

Now the complete code:

instance Num a => Num (Dif a) where
  fromInteger             = dConst . fromInteger
  D x x’ + D y y’         = D (x + y) (x’ + y’)
  D x x’ - D y y’         = D (x - y) (x’ - y’)
  p@(D x x’) * q@(D y y’) = D (x * y) (x’ * q + p * y’)
 
  negate = negate >-< -1
  abs    = abs    >-< signum
  signum = signum >-< 0
 
instance Fractional a => Fractional (Dif a) where
  fromRational = dConst . fromRational
  recip        = recip >-< - sqr recip
 
instance (Fractional a, Floating a) => Floating (Dif a) where
  pi    = dConst pi
  exp   = exp   >-< exp
  log   = log   >-< recip
  sqrt  = sqrt  >-< recip (2 * sqrt)
  sin   = sin   >-< cos
  cos   = cos   >-< - sin
  sinh  = sinh  >-< cosh
  cosh  = cosh  >-< sinh
  asin  = asin  >-< recip (sqrt (1-sqr))
  acos  = acos  >-< recip (- sqrt (1-sqr))
  atan  = atan  >-< recip (1+sqr)
  asinh = asinh >-< recip (sqrt (1+sqr))
  acosh = acosh >-< recip (- sqrt (sqr-1))
  atanh = atanh >-< recip (1-sqr)

The operators and literals on the right of the (>-<) are overloaded for the type Dif a -> Dif a. For instance, in the definition of sqrt,

2     :: Dif a -> Dif a
recip :: (Dif a -> Dif a) -> (Dif a -> Dif a)
(*)   :: (Dif a -> Dif a) -> (Dif a -> Dif a)
      -> (Dif a -> Dif a)

5 Comments

  1. Punya:

    Abelson and Sussman’s Structure and Interpretation of Classical Mechanics has a Scheme implementation of this idea, which they use to implement an environment for symbolically and numerically manipulating physical systems.

  2. Jaak:

    It’s pretty and all, but either you have something missing or something wrong. Because the code doesn’t simply work (lots of complaints along the lines of “Could not deduce…” and “Couldn’t match expected type…”), something funky seems to be going on with dlift. I’d appreciate full working code.

    • Jaak
  3. Perehene:

    Very interesting post. I am a newbie in haskell and I wanted to give it a try, but I get a bunch of errors in ghci. Could you put the source code and the required options to use it in ghc? Thanks a lot!

  4. conal:

    Jaak & Perehene: I’ve added source files: NumInstances.hs and Dif.hs. Enjoy!

  5. Nikolay:

    multiplication may pull x’ and y’ while result is just requested for (D (x*y) _ _), I think

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