{-# LANGUAGE NoImplicitPrelude #-} {- We represent a Gaussian bell curve in terms of the reciprocal of its variance and its value at the origin. We could do some projective geometry in the exponent in order to also have zero variance, which corresponds to the dirac impulse. -} module MathObj.Gaussian.Variance where import qualified MathObj.Polynomial as Poly import qualified Algebra.Transcendental as Trans import qualified Algebra.Algebraic as Algebraic import qualified Algebra.Field as Field import qualified Algebra.Real as Real import qualified Algebra.Ring as Ring import qualified Algebra.Additive as Additive {- import Algebra.Transcendental (pi, ) import Algebra.Ring ((*), (^), ) import Algebra.Additive ((+)) -} import Test.QuickCheck (Arbitrary, arbitrary, ) import Control.Monad (liftM2, ) -- import Prelude (($)) import NumericPrelude import PreludeBase data T a = Cons {amp, c :: a} deriving (Eq, Show) instance (Real.C a, Arbitrary a) => Arbitrary (T a) where arbitrary = liftM2 Cons arbitrary (fmap ((1+) . abs) arbitrary) constant :: Ring.C a => T a constant = Cons one zero {-# INLINE evaluate #-} evaluate :: (Trans.C a) => T a -> a -> a evaluate f x = sqrt (amp f) * exp (-pi * c f * x^2) exponentPolynomial :: (Additive.C a) => T a -> Poly.T a exponentPolynomial f = Poly.fromCoeffs [zero, zero, c f] norm1 :: (Algebraic.C a, Real.C a) => T a -> a norm1 f = sqrt $ abs (amp f) / c f norm2 :: (Algebraic.C a, Real.C a) => T a -> a norm2 f = sqrt $ abs (amp f) / (sqrt $ 2 * c f) normP :: (Trans.C a, Real.C a) => a -> T a -> a normP p f = sqrt (abs (amp f)) * (p * c f) ^? (- recip (2*p)) variance :: (Trans.C a) => T a -> a variance f = recip $ c f * 2*pi multiply :: (Ring.C a) => T a -> T a -> T a multiply f g = Cons (amp f * amp g) (c f + c g) {- | > convolve x y t = > integrate $ \s -> x s * y(t-s) -} convolve :: (Field.C a) => T a -> T a -> T a convolve f g = Cons (amp f * amp g / (c f + c g)) (recip $ recip (c f) + recip (c g)) {- | > fourier x f = > integrate $ \t -> x t * cis (-2*pi*t*f) -} fourier :: (Field.C a) => T a -> T a fourier f = Cons (amp f / c f) (recip $ c f) {- fourier (t -> exp(-(a*t)^2)) -} dilate :: (Field.C a) => a -> T a -> T a dilate k f = Cons (amp f) $ c f / k^2 shrink :: (Ring.C a) => a -> T a -> T a shrink k f = Cons (amp f) $ c f * k^2 amplify :: (Ring.C a) => a -> T a -> T a amplify k f = Cons (k^2 * amp f) $ c f {- laws fourier (convolve f g) = multiply (fourier f) (fourier g) dilate k (dilate m f) = dilate (k*m) f dilate k (shrink k f) = f variance (dilate k f) = k^2 * variance f variance (convolve f g) = variance f + variance g -}