Algebraic Gaussian moment functionals and their coefficient identities.
Linear extension from monomials of the three-coordinate Gaussian moments.
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Linear extension from monomials for two independent normalized conjugate pairs.
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@[simp]
theorem
GaussianMomentsCounterexamples.naturalMoment3_monomial
(d : Fin 3 →₀ ℕ)
(c : ℂ)
:
naturalMoment3 ((MvPolynomial.monomial d) c) = c * (pairMoment (d 0) (d 1) * ∫ (t : ℝ), ↑t ^ d 2 ∂ProbabilityTheory.gaussianReal 0 1)
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theorem
GaussianMomentsCounterexamples.naturalMoment4_monomial
(d : Fin 4 →₀ ℕ)
(c : ℂ)
:
naturalMoment4 ((MvPolynomial.monomial d) c) = c * (pairMoment (d 0) (d 1) * pairMoment (d 2) (d 3))
Embed a univariate polynomial in one specified natural coordinate.
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theorem
GaussianMomentsCounterexamples.naturalMoment3_contraction
(a b : ℕ)
(f : Polynomial ℂ)
:
naturalMoment3 (MvPolynomial.X 0 ^ a * (polyAt 1) f * MvPolynomial.X 2 ^ b) = ↑a.factorial * f.coeff a * ∫ (t : ℝ), ↑t ^ b ∂ProbabilityTheory.gaussianReal 0 1
theorem
GaussianMomentsCounterexamples.naturalMoment4_master
(A : Polynomial ℂ)
(m : ℕ)
(hm : 1 ≤ m)
:
The four-variable master identity in the natural-coordinate moment interface.
theorem
GaussianMomentsCounterexamples.naturalMoment3_power_expansion_raw
(A : Polynomial ℂ)
(m : ℕ)
:
theorem
GaussianMomentsCounterexamples.naturalMoment3_master
(A : Polynomial ℂ)
(m : ℕ)
(hm : 1 ≤ m)
:
The three-variable master identity in the natural-coordinate moment interface.
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