Gaussian variance mixtures: Student-t marginals and excess kurtosis #
Marginalizing a centered Gaussian of precision β against a Gamma(a, b) law on β gives the
Student-t density, normalized by b^a. For any variance mixture X = √V · Z with Z standard
normal and independent of V ≥ 0, the kurtosis is 3 E[V²] / E[V]², so the excess kurtosis
3 Var(V) / E[V]² is nonnegative.
Main results #
Superstatistics.gaussian_gamma_mixture_studentt: the Gaussian–Gamma mixture integral.Superstatistics.std_normal_second_moment,Superstatistics.std_normal_fourth_moment:E[Z²] = 1andE[Z⁴] = 3, from the moment generating function.Superstatistics.sq_expectation_le_expectation_sq:E[V]² ≤ E[V²].Superstatistics.variance_mixture_kurtosis_identity: the kurtosis identity, given the moment factorization.Superstatistics.variance_mixture_kurtosis_identity': the same on the product spaceμV.prod (gaussianReal 0 1), with the factorization derived fromintegral_prod_mul.
References #
- C. Beck, E. G. D. Cohen, Superstatistics, Physica A 322 (2003) 267–275.
- D. F. Andrews, C. L. Mallows, Scale mixtures of normal distributions, J. Roy. Statist. Soc. Ser. B 36 (1974) 99–102.
T1 — Gaussian/Gamma scale-mixture = Student-t (pure analytic / integral form) #
Marginalising a zero-mean Gaussian of precision β against a Gamma(a,b) prior on β
yields the (unnormalised) Student-t density. In Mathlib pieces:
Real.Gamma, ProbabilityTheory.gaussianPDFReal, ProbabilityTheory.gammaPDFReal
exist, but no MIXTURE / compound / subordination identity does.
Setting a = ν/2, b = ν σ²/2 recovers Student-t_ν(scale σ) ∝ (1 + x²/(νσ²))^(−(ν+1)/2).
Proof: substitute u = β (b + x²/2), pull constants, recognise Real.Gamma (a+1/2)
via Real.Gamma_eq_integral / integral_rpow_mul_exp_neg_mul_Ioi-style Gamma integrals.
The right-hand side carries the Gamma normalization b^a; with a=ν/2, b=νσ²/2 this is the properly normalised Student-t_ν
density (b^a·(b+x²/2)^(-(a+1/2)) collapses to the standard (1+x²/(νσ²))^(-(ν+1)/2)
shape times the σ/normalisation constants).
T2 — Gaussian variance-mixture is leptokurtic (excess kurtosis ≥ 0) #
If X = √V · Z with Z ~ N(0,1) ⟂ V ≥ 0, then kurtosis(X) = 3 · E[V²]/E[V]² ≥ 3,
equality iff V a.s. constant; excess kurtosis = 3 · Var(V)/E[V]².
Mathlib DEFINES no kurtosis, so the whole claim reduces to the Jensen core
E[V]² ≤ E[V²], which is exactly variance_nonneg unfolded via variance_eq_sub
(Var V = E[V²] − E[V]²). This lemma IS the leptokurtic engine.
Explicit leptokurtic form: excess kurtosis = 3·Var(V)/E[V]² ≥ 0.
Stated as the nonnegativity of Var(V)/E[V]² (the 3· and the √V·Z
kurtosis identity are downstream). Leans on variance_nonneg.
Standard-normal moments E[Z²]=1, E[Z⁴]=3 (the leptokurtic inputs) #
Computed via the moment-generating function: with Z ~ N(0,1) the mgf is
t ↦ exp(t²/2), and E[Z^n] = (d/dt)^n mgf |₀ (iteratedDeriv_mgf_zero).
Differentiating exp(t²/2) four times gives the polynomial-times-Gaussian tower
t·e, (1+t²)·e, (3t+t³)·e, (3+6t²+t⁴)·e; evaluating at 0 yields 1 and 3.
Standard-normal second moment: E[Z²] = 1.
Standard-normal fourth moment: E[Z⁴] = 3.
Leptokurtic identity for a variance-mixture Gaussian. Writing X = √V·Z
with Z ~ N(0,1) ⟂ V ≥ 0, the independence factorisation gives
E[X²] = E[V]·E[Z²] = E[V] and E[X⁴] = E[V²]·E[Z⁴] = 3·E[V²], the
standard-normal moments E[Z²]=1, E[Z⁴]=3 being std_normal_second_moment
and std_normal_fourth_moment. Given those two moment facts (as hX2, hX4)
and E[V] > 0, the kurtosis is E[X⁴]/E[X²]² = 3·E[V²]/E[V]², the EXCESS
kurtosis equals 3·Var(V)/E[V]², and (since Var(V) ≥ 0) the kurtosis is ≥ 3:
the mixture is leptokurtic.
The independence-factorisation step E[V·Z²] = E[V]·E[Z²],
E[V²·Z⁴] = E[V²]·E[Z⁴] (which produces hX2, hX4 from X = √V·Z) is taken
as a hypothesis here; variance_mixture_kurtosis_identity' derives it on a concrete
product space.
Self-contained version: the factorisation DERIVED from a product space #
variance_mixture_kurtosis_identity above took the independence factorisation
E[X²]=E[V], E[X⁴]=3·E[V²] as hypotheses (hX2, hX4). Here we DISCHARGE them:
we build the concrete independent product space μ := μV.prod (gaussianReal 0 1) on
ℝ × ℝ, set V ω = ω.1, Z ω = ω.2, X ω = √(ω.1)·ω.2, and derive both moment
identities from Mathlib's Fubini factorisation integral_prod_mul
(∫ f(z.1)·g(z.2) ∂(μ.prod ν) = (∫f ∂μ)·(∫g ∂ν), unconditional) together with the
standard-normal moments std_normal_second_moment/std_normal_fourth_moment.
The ONLY remaining hypotheses are legitimate ones on the mixing law μV:
its second L²-integrability (MemLp (·) 2 μV, needed for the Jensen step E[V]²≤E[V²]),
V ≥ 0 a.e. (hVnn, so (√V)²=V), and E[V] > 0 (heV). No factorisation
hypothesis remains — it is now a THEOREM (via integral_prod_mul).