Appendix A. A kernel interpretation of the frame operator
This appendix computes a regularized characteristic functional of the infinite Gaussian mixture and explains a formal kernel interpretation of the frame operator. These optional observations are not prerequisites for the main proofs.
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OperatorRidgelet.Paper.lem_A_1_i[complete] -
OperatorRidgelet.Paper.lem_A_1_ii[complete] -
OperatorRidgelet.Paper.lem_A_1_iii[complete] -
OperatorRidgelet.Paper.lem_A_1_iv[complete]
For z\ne0 put q=\langle Pz,z\rangle>0 (i) and
\nu_\alpha^{\varepsilon,M}=\int_\varepsilon^M\mathcal N(0,2sP)s^{\alpha/2-1}\mathrm ds.
Then \lim_{\varepsilon\downarrow0,M\uparrow\infty}\int_He^{i\langle z,\xi\rangle}\,\nu_\alpha^{\varepsilon,M}(\mathrm d\xi)=\Gamma(\alpha/2)q^{-\alpha/2}
(ii), where \int_0^\infty e^{-sq}s^{\alpha/2-1}\mathrm ds=\Gamma(\alpha/2)q^{-\alpha/2}
(iii). In contrast \int_H|e^{i\langle z,\xi\rangle}|\,\nu_\alpha(\mathrm d\xi)=\infty
(iv), so the limit is not a Lebesgue integral against \nu_\alpha.
Lean code for LemmaA.1●4 theorems
Associated Lean declarations
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OperatorRidgelet.Paper.lem_A_1_i[complete]
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OperatorRidgelet.Paper.lem_A_1_ii[complete]
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OperatorRidgelet.Paper.lem_A_1_iii[complete]
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OperatorRidgelet.Paper.lem_A_1_iv[complete]
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OperatorRidgelet.Paper.lem_A_1_i[complete] -
OperatorRidgelet.Paper.lem_A_1_ii[complete] -
OperatorRidgelet.Paper.lem_A_1_iii[complete] -
OperatorRidgelet.Paper.lem_A_1_iv[complete]
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theoremdefined in OperatorRidgelet/Paper/Transform.leancomplete
theorem OperatorRidgelet.Paper.lem_A_1_i.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] {P : H →L[ℝ] H} (hP : OperatorRidgelet.IsTraceClassCovariance P) (z : H) (hz : z ≠ 0) : 0 < inner ℝ (P z) z
theorem OperatorRidgelet.Paper.lem_A_1_i.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] {P : H →L[ℝ] H} (hP : OperatorRidgelet.IsTraceClassCovariance P) (z : H) (hz : z ≠ 0) : 0 < inner ℝ (P z) z
**Lemma [lem:A.1]** Truncation of the scale integral. For `z ≠ 0` the quadratic form `q = ⟨Pz,z⟩` is positive.
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theoremdefined in OperatorRidgelet/Paper/Transform.leancomplete
theorem OperatorRidgelet.Paper.lem_A_1_ii.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] {P : H →L[ℝ] H} (hP : OperatorRidgelet.IsTraceClassCovariance P) {N : ℝ → MeasureTheory.Measure H} (hN : OperatorRidgelet.IsCenteredGaussianLayers P N) {α : ℝ} (hα : 0 < α) (z : H) (hz : z ≠ 0) : Filter.Tendsto (fun εM => MeasureTheory.charFun (OperatorRidgelet.gaussianMixtureOn N α (Set.Ioo εM.1 εM.2)) z) (nhdsWithin 0 (Set.Ioi 0) ×ˢ Filter.atTop) (nhds ↑(Real.Gamma (α / 2) * inner ℝ (P z) z ^ (-(α / 2))))
theorem OperatorRidgelet.Paper.lem_A_1_ii.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] {P : H →L[ℝ] H} (hP : OperatorRidgelet.IsTraceClassCovariance P) {N : ℝ → MeasureTheory.Measure H} (hN : OperatorRidgelet.IsCenteredGaussianLayers P N) {α : ℝ} (hα : 0 < α) (z : H) (hz : z ≠ 0) : Filter.Tendsto (fun εM => MeasureTheory.charFun (OperatorRidgelet.gaussianMixtureOn N α (Set.Ioo εM.1 εM.2)) z) (nhdsWithin 0 (Set.Ioi 0) ×ˢ Filter.atTop) (nhds ↑(Real.Gamma (α / 2) * inner ℝ (P z) z ^ (-(α / 2))))
**Lemma [lem:A.1]** Truncation of the scale integral. The characteristic functionals of the truncated mixtures `ν_α^{ε,M} = ∫_ε^M 𝒩(0,2sP) s^{α/2-1} ds` converge, as `ε ↓ 0` and `M ↑ ∞`, to `Γ(α/2) q^{-α/2}`. -
theoremdefined in OperatorRidgelet/Paper/Transform.leancomplete
theorem OperatorRidgelet.Paper.lem_A_1_iii.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] {P : H →L[ℝ] H} (hP : OperatorRidgelet.IsTraceClassCovariance P) {α : ℝ} (hα : 0 < α) (z : H) (hz : z ≠ 0) : ∫ (s : ℝ) in Set.Ioi 0, Real.exp (-s * inner ℝ (P z) z) * s ^ (α / 2 - 1) = Real.Gamma (α / 2) * inner ℝ (P z) z ^ (-(α / 2))
theorem OperatorRidgelet.Paper.lem_A_1_iii.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] {P : H →L[ℝ] H} (hP : OperatorRidgelet.IsTraceClassCovariance P) {α : ℝ} (hα : 0 < α) (z : H) (hz : z ≠ 0) : ∫ (s : ℝ) in Set.Ioi 0, Real.exp (-s * inner ℝ (P z) z) * s ^ (α / 2 - 1) = Real.Gamma (α / 2) * inner ℝ (P z) z ^ (-(α / 2))
**Lemma [lem:A.1]** Truncation of the scale integral. The limit is the Gamma integral `∫₀^∞ e^{-sq} s^{α/2-1} ds = Γ(α/2) q^{-α/2}`. -
theoremdefined in OperatorRidgelet/Paper/Transform.leancomplete
theorem OperatorRidgelet.Paper.lem_A_1_iv.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (hH : ¬FiniteDimensional ℝ H) {P : H →L[ℝ] H} (hP : OperatorRidgelet.IsTraceClassCovariance P) {N : ℝ → MeasureTheory.Measure H} (hN : OperatorRidgelet.IsCenteredGaussianLayers P N) {α : ℝ} (hα : 0 < α) (z : H) (hz : z ≠ 0) : ¬MeasureTheory.Integrable (fun ξ => Complex.exp (↑(inner ℝ z ξ) * Complex.I)) (OperatorRidgelet.gaussianMixture N α)
theorem OperatorRidgelet.Paper.lem_A_1_iv.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (hH : ¬FiniteDimensional ℝ H) {P : H →L[ℝ] H} (hP : OperatorRidgelet.IsTraceClassCovariance P) {N : ℝ → MeasureTheory.Measure H} (hN : OperatorRidgelet.IsCenteredGaussianLayers P N) {α : ℝ} (hα : 0 < α) (z : H) (hz : z ≠ 0) : ¬MeasureTheory.Integrable (fun ξ => Complex.exp (↑(inner ℝ z ξ) * Complex.I)) (OperatorRidgelet.gaussianMixture N α)
**Lemma [lem:A.1]** Truncation of the scale integral. In contrast, the character `ξ ↦ e^{i⟨z,ξ⟩}` is not integrable against `ν_α`, so the limit is not a Lebesgue integral.
The truncated mixture is finite, so Fubini and the characteristic functional of
\mathcal N(0,2sP) reduce the integral to
\int_\varepsilon^Me^{-sq}s^{\alpha/2-1}\mathrm ds; monotone convergence and the
substitution u=sq finish the proof.
Remark A.2 (A Riesz-type kernel for the frame operator).
The regularized characteristic functional in Lemma A.1 suggests
the kernel \Gamma(\alpha/2)\langle P(x-y),x-y\rangle^{-\alpha/2} for the frame
operator. This is only a formal interchange against an infinite oscillatory measure and is
not used as an identity. In finite dimension, with P=I and 0<\alpha<m, it agrees
with the Riesz-potential interpretation of Corollary D.2.