The standard Gaussian measure on a finite product #
The product measure γ^ι = Measure.pi (fun _ : ι => gaussianReal 0 1) is Lebesgue measure on
ℝ^ι weighted by the joint density x ↦ ∏ i, gaussianPDFReal 0 1 (x i). That identification is
what lets a weight-in-the-measure statement about γ^ι be read as a weight-in-the-function
statement about volume^ι, via TauCeti.weightL2Isometry.
Like TauCeti.Probability.gaussianPDFReal_zero_one, these are statements about the Gaussian
distribution
alone (no orthogonal family appears), so they live here rather than with the multi-index Hermite
basis that consumes them.
Main statements #
TauCeti.Probability.prod_gaussianPDFReal_zero_one: the joint density in closed form,(2π)^(-d/2) · e^{-∑ᵢ xᵢ²/2}, wheredis the number of coordinates.TauCeti.Probability.pi_gaussianReal_eq_withDensity:γ^ι = volume^ιweighted by the joint density.TauCeti.Probability.pi_volume_absolutelyContinuous_pi_gaussianReal: the joint density never vanishes, sovolume^ι-null sets are exactlyγ^ι-null sets in the direction one needs to move an almost-everywhere statement fromγ^ιtovolume^ι.
The joint standard Gaussian density on ℝ^ι is everywhere positive.
The joint standard Gaussian density on ℝ^ι in closed form: the normalisation
(2π)^(-d/2) in the dimension d, times the exponential of minus half the sum of the squared
coordinates.
The joint standard Gaussian density on ℝ^ι is measurable.
The standard Gaussian on ℝ^ι is volume^ι weighted by the joint density. Each factor is
volume weighted by gaussianPDFReal 0 1 (ProbabilityTheory.gaussianReal_of_var_ne_zero), and
coordinatewise densities multiply (TauCeti.pi_withDensity).
volume^ι is absolutely continuous with respect to γ^ι. The joint density is everywhere
positive, so weighting by it kills no set of positive measure. This is what moves an
almost-everywhere identification of a L²(γ^ι) representative to one holding volume^ι-almost
everywhere, where the √-density envelope lives.