space such that the value at any given location is a random variable p(f ) is a Gaussian Process if: For any finite subset of locations x = [x1, x2, x3, ...xn ], the set f = [f (x1 ), f (x2 ), ..f (xn )] has a multivariate Gaussian distribution. p(f|x) = N(µ, C) pdf [f (x1 ), f (x2 ), ...f (xn )] = 1 (2π)k |C| exp − 1 2 (f − µ)C−1(f − µ)T Vikrant Kamble Gaussian Random Fields September 28, 2017 6 / 13
function µ(x) and a Kernel K(xi , xj ) that allows us to construct the Covariance matrix C. p(f |X) = N(0, K) A Kernel is a function that takes a pair of vectors and maps them to a scalar quantity K(xi , xj ) : Rn × Rn → R Let’s simulate!!! Vikrant Kamble Gaussian Random Fields September 28, 2017 7 / 13
), ...δ(xn )] = 1 (2π)k |C| exp − 1 2 δ C−1δT The kernel K is nothing but the correlation function ξ(r). Assuming that the Universe is homogeneous, isotropic and all n > 2-point correlation functions vanish, the only quantity we need to fully capture all the information of the Universe is ξ(r). Redshift Space Distortions (RSD) - ξ(r) → ξ(r, θ). Non-gaussianity → finite (n > 2)-point correlation functions Vikrant Kamble Gaussian Random Fields September 28, 2017 11 / 13
Remember, the probability distribution is over the scalar field value at these chosen locations, and not the location themselves. Create the mean vector of the perturbations µ = [g(x1 ), g(x2 ), ..., g(xn )] At early Universe, µ = 0 Create the Covariance matrix using the kernel. For the perturbation field K(xi , xj ; θ) = K(|xi − xj |; θ) = ξ(r; θ) What we have is f ∼ N(g(x)N , CN×N ) Sample once to get one realization of the function Vikrant Kamble Gaussian Random Fields September 28, 2017 13 / 13