Parallel Haskell Digest 4

Fri, 22 Jul 2011 15:46:17 GMT, by nick.
Filed under parallel, ph-digest.

Hello Haskellers!

It's time for the fourth edition of the Parallel Haskell Digest, bringing you a summary of the news and discussions of parallelism and concurrency in Haskell. The digest is made possible by the Parallel GHC Project.


Word of the Month

In this issue we have two words of the month: par and pseq.

Haskell provides two annotations, par and pseq, that allow the programmer to give hints to the compiler about where there are opportunities to exploit parallelism. While these annotations are not typically used directly by programmers, it is useful to understand them because they are the underlying mechanism for higher level tools such as "parallel strategies" and the Eval monad.

The two combinators have the following signatures:

par  :: a -> b -> b
pseq :: a -> b -> b

While their signatures are the same, they are used to annotate different things. The par combinator hints to the Haskell implementation that it might be beneficial to evaluate the first argument in parallel. However, since Haskell does not impose an evaluation order, we also need pseq, which instructs the compiler to ensure that its first argument is evaluated before the second.

Let's take a look at an example inspired by Parallel Performance Tuning for Haskell by Jones, Marlow, and Singh, which illustrates this nicely. Suppose you're interested in the sum of two expensive computations. To keep things simple, we'll use a naive implementation of fib (the point here isn't to have an efficient computation, I'm trying to show an expensive one):

fib :: Int -> Int
fib 0 = 0
fib 1 = 1
fib n = fib (n-1) + fib (n-2)

For a second expensive computation, we'll calculate the negafibonacci number, which works on negative numbers:

negafib :: Int -> Int
negafib 0 = 0
negafib (-1) = 1
negafib n = nfib (n+2) - nfib (n+1)

The sum of these two can be calculated by the following sequential function:

sumfib :: Int -> Int
sumfib n = x + y
  x = fib n
  y = negafib (-n)

There's obvious room for improvement here when we have two cores: we simply calculate the expensive computations on separate cores. Annotating the code above is a fairly simple process. We first use par to annotate the fact that x must be calculated in parallel with the rest of the computation. Second, we ensure that y gets computed before x + y by annotating with pseq. The result is as follows:

import Control.Parallel (par, pseq)

psumfib :: Int -> Int
psumfib n = x `par` (y `pseq` x + y)
  x = fib n
  y = negafib (-n)

We can write a simple program that outputs the result of running this computation with the following main function:

main :: IO ()
main = putStrLn . show . sumfib $ 37

We should hope for the parallel version to work twice as fast, since the two expensive functions should take about the same time to compute. Here's the output of compiling and running the sequential version of the program:

$ ghc -rtsopts Main.hs
[1 of 1] Compiling Main             ( Main.hs, Main.o )
Linking Main ...
$ time ./Main

real        0m6.113s
user        0m6.090s
sys         0m0.010s

Now replacing sumfib with psumfib produces the following results:

$ ghc -rtsopts -threaded Main.hs
[1 of 1] Compiling Main             ( Main.hs, Main.o )
Linking Main ...
$ time ./Main +RTS -N2

real        0m3.402s
user        0m6.660s
sys         0m0.040s

This is obviously a very trivial example, but the point is that annotations provide a powerful way of expressing parallel algorithms. It's interesting to note that for this simple program, the timings for the parallel version on a single core performs as well as the single core version compiled without threading.

While annotations are a simple mechanism for expressing where parallelism might be exploited in a program, beware that there are a number of pitfalls to using this technique: all that glitters is not gold! The main difficulty in using par and pseq directly is that you really need to have a clear understanding of evaluation order. In particular, unless you understand what laziness is doing to the evaluation order, then you might find that the computations you're sparking off with par might not occur when you expected they should.

Then there are all the general difficulties that you face with parallel programming, like getting the right granularity of work to do in parallel. Using par is quite lightweight so can be used to exploit reasonably fine grained parallelism, but it is certainly not free. Finally, parallel performance suffers when there are too many garbage collections, so keeping this to a minimum by either using more efficient data structures or increasing available memory, becomes an important factor.

Nevertheless, it's well worth having a play with par and pseq. The next step after that is to look at parallel strategies. Strategies is a layer of abstraction on top of par and pseq. You might like to to read Seq no more: Better Strategies for Parallel Haskell, by Simon Marlow et al. which describes Strategies and the Eval monad. It's all available in the parallel library on Hackage. More recently, the Par monad has also been introduced as yet another way of describing parallel evaluations. These key topics will no doubt feature in a future word of the month, so stay tuned!

Parallel GHC Project Update

The Parallel GHC Project is an MSR-funded project to push the real-world use of parallel Haskell. The aim is to demonstrate that parallel Haskell can be employed successfully in industrial projects. This month we're having a guest column from the team over at Los Alamos National Laboratory, one of the partners involved in the project (you can see the full details in report LA-UR 11-0341). They have been working on writing Monte Carlo physics simulations in Haskell, which has given them high levels of parallelism, along with useful tools for abstraction. So, without further ado, over to Michael Buksas from LANL:

Our goal is to build highly efficient Monte Carlo physics simulations using parallel Haskell. We're focusing on SMP performance though some combination of explicit threading and pure parallel annotations.

The Monte Carlo approach involves randomly sampling the space of solutions to generate data which contributes to the solution. For these physical problems, our samples are the tracks of particles as they move through space, interacting with a physical material as they go. Data collected from each particle trajectory is then combined into information needed to compute the solution. For example, the detailed information about the particle's interaction with the material is collected into a collective effect on the material properties.

To date, we have a code base which includes two approaches to the problem. One is a specific and parallel-tuned application code targeting relativistic neutrino transport in stellar atmospheres. The other is building a more general environment for creating specific applications, such as this one.

We recently presented to our colleagues in LANL some preliminary results on the parallel performance of the targeted application code.

To give a sense of the approach to parallelization in this code, consider these high-level functions from an earlier serial version:

main :: IO ()
main = do
  (n, rest) <- parseCL
  let tally = runMany infMesh simpleMat n
  writeTally &quot;tally&quot; tally

runMany :: Mesh -> Material -> Word32 -> RNG -> Tally
runMany msh mat ntot rng = let
  ps = genParticles ntot msh rng
  tallies = map (runParticle msh mat) $ ps
  in foldl' merge emptyTally tallies

And consider the following changes for the parallel version:

main :: IO ()
main = do
  (n,sz) <- parseCL
  let tally = feed infMesh simpleMat n sz prand
  writeTally &quot;tally&quot; tally

feed :: Mesh -> Material -> Word32 -> Word32 -> RNG -> Tally
feed msh mat ntot chunkSz rng
    | ntot <= chunkSz = runMany msh mat ntot rng
    | otherwise       = t `par` (ts `pseq` (merge t ts))
    where t  = runMany msh mat chunkSz g1
          ts = feed msh mat (ntot - chunkSz) chunkSz g2
          (g1,g2) = split g

We've wrapped function runMany in feed, which partitions the collection of generated particles into groups of size chunkSz, and issues these particles to runMany in parallel.

With this simple change, we seeing upwards of 80% utilization of up to 8 cores, for a performance improvement greater than a factor of 6. We believe that performance can be further improved with different strategies for breaking down the work, and looking for additional parallelization opportunities in the collection of results.

Our other branch of development is focused on finding useful abstractions and high-level functions to support programming a variety of Monte Carlo problems of this kind. We have identified a few such useful abstractions, and implemented them as type classes and type families.

For example, Space is a general term for the physical space and imposed symmetries in which we can perform a simulation. We express this as follows:

class Space s where
  type Position s  :: *
  type Direction s :: *
  stream    :: s -> Distance -> s
  position  :: s -> Position s
  direction :: s -> Direction s
  make      :: Position s -> Direction s -> s

and implement specific spaces, such as one with the symmetry of the unit sphere:

instance Space Spherical1D where
    type Position  Spherical1D = Radius
    type Direction Spherical1D = Normalized Vector2
    stream (Vector2 x y) (Distance d) = Vector2 (x+d) y
    position s  = Radius $ vmag s
    direction s = normalize s
    make (Radius pos) dir = pos *| (normalized_value dir)

This allows the specific space data types to be used in a variety of contexts. Using ordinary parametric polymorphism is also effective:

-- | Stream a single particle:
stream :: (p -> (e,p))   -- ^ Function to produce each step. Comes from a model.
          -> (e -> Bool) -- ^ Check for terminal events to stop streaming
          -> p           -- ^ Initial particle
          -> [(e, p)]    -- ^ Resulting list of events and particle states.
stream stepper continue p = next p
  where next p =
          let (e, p') = stepper p
          in  (e, p') : if continue e then next p' else []

The above is our high-level routine function for generating a history from a single particle, recorded as a list of (event, particle) pairs, where the event and particle data types are provided for each problem.

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Help and Feedback

If you'd like to make an announcement in the next Haskell Parallel Digest, then get in touch with me, Nicolas Wu, at Please feel free to leave any comments and feedback!