4.2. Integral representation
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OperatorRidgelet.IsTemperedFunction[complete] -
OperatorRidgelet.temperedTestFilter[complete] -
OperatorRidgelet.temperedAdmissibilityConst[complete]
This is the activation and distributional-pairing setup for Theorem 4.5(iii).
A tempered distribution \beta\in\mathcal S'(\mathbb R) that is a continuous function of
polynomial growth is the pair of \beta and a continuous b:\mathbb R\to\mathbb R with
|b(t)|\le C(1+|t|)^p and \langle\beta,\varphi\rangle=\int b\varphi. For a band-pass
\rho the test filter \omega\mapsto\rho^\sharp(-\omega)|\omega|^{-\alpha} is a Schwartz
function, and the distributional admissibility constant is
C_{\beta,\rho}^{(\alpha)}=\frac1{2\pi}\langle\beta^\sharp,\rho^\sharp(-\,\cdot\,)|\cdot|^{-\alpha}\rangle.
Lean code for DefinitionAux.5●3 definitions
Associated Lean declarations
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OperatorRidgelet.IsTemperedFunction[complete]
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OperatorRidgelet.temperedTestFilter[complete]
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OperatorRidgelet.temperedAdmissibilityConst[complete]
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OperatorRidgelet.IsTemperedFunction[complete] -
OperatorRidgelet.temperedTestFilter[complete] -
OperatorRidgelet.temperedAdmissibilityConst[complete]
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structuredefined in OperatorRidgelet/Reconstruction/Defs.leancomplete
structure OperatorRidgelet.IsTemperedFunction (β : TemperedDistribution ℝ ℂ) (b : ℝ → ℝ) : Prop
structure OperatorRidgelet.IsTemperedFunction (β : TemperedDistribution ℝ ℂ) (b : ℝ → ℝ) : Prop
`β ∈ 𝒮'(ℝ)` is the continuous function `b` of polynomial growth: `b` is continuous, `|b(t)| ≤ C (1+|t|)^p`, and `β` acts on test functions by integration against `b`.
Fields
continuous : Continuous b
`b` is continuous.
polynomialGrowth : OperatorRidgelet.HasPolynomialGrowth b
`b` has polynomial growth.
apply_eq : ∀ (φ : SchwartzMap ℝ ℂ), β φ = ∫ (t : ℝ), ↑(b t) * φ t
`β` is integration against `b`.
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defdefined in OperatorRidgelet/Tempered/Const.leancomplete
def OperatorRidgelet.temperedTestFilter (α : ℝ) (ρ : SchwartzMap ℝ ℝ) : SchwartzMap ℝ ℂ
def OperatorRidgelet.temperedTestFilter (α : ℝ) (ρ : SchwartzMap ℝ ℝ) : SchwartzMap ℝ ℂ
The test filter `ω ↦ ρ♯(-ω) |ω|^{-α}` as a Schwartz function, when one with these values exists (in particular when `ρ` is band-pass); `0` otherwise. -
defdefined in OperatorRidgelet/Tempered/Const.leancomplete
def OperatorRidgelet.temperedAdmissibilityConst (α : ℝ) (β : TemperedDistribution ℝ ℂ) (ρ : SchwartzMap ℝ ℝ) : ℂ
def OperatorRidgelet.temperedAdmissibilityConst (α : ℝ) (β : TemperedDistribution ℝ ℂ) (ρ : SchwartzMap ℝ ℝ) : ℂ
The distributional admissibility constant `C^{(α)}_{β,ρ} = (2π)⁻¹ ⟨β♯, ρ♯(-·) |·|^{-α}⟩` of a tempered activation `β` and a filter `ρ`.
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OperatorRidgelet.Paper.thm_4_5_i_a[complete] -
OperatorRidgelet.Paper.thm_4_5_i_b[complete] -
OperatorRidgelet.Paper.thm_4_5_i_c[complete] -
OperatorRidgelet.Paper.thm_4_5_ii_a[complete] -
OperatorRidgelet.Paper.thm_4_5_ii_b[complete] -
OperatorRidgelet.Paper.thm_4_5_ii_c[complete] -
OperatorRidgelet.Paper.thm_4_5_iii_a[complete] -
OperatorRidgelet.Paper.thm_4_5_iii_b[complete] -
OperatorRidgelet.Paper.thm_4_5_iii_c[complete] -
OperatorRidgelet.Paper.thm_4_5_iii_d[complete] -
OperatorRidgelet.Paper.thm_4_5_iii_e[complete]
Let \alpha>0. Part (ii) assumes an \alpha-admissible Schwartz filter \rho; part
(iii) assumes a band-pass filter. (i) For G\in L^1(\nu_\alpha), the function g_G is
bounded with \|g_G\|_\infty\le\|G\|_{L^1(\nu_\alpha)} and continuous,
and g_G=0 only if G=0 \nu_\alpha-almost everywhere. (ii) For
G\in L^1(\nu_\alpha)\cap L^2(\nu_\alpha) and every x, the iterated integral
\int_H[\int_{\mathbb R}\gamma_G(a,c)\rho(\langle a,x\rangle+c)\,\mathrm dc]\,\nu_\alpha(\mathrm da)=(\!(\rho,\rho)\!)_\alpha g_G(x)
converges absolutely, and if \gamma_G\in L^1(\lambda_\alpha) its left side is the integral
network S_\rho[\gamma_G\lambda_\alpha](x). (iii) For a tempered \beta that is a
continuous function of polynomial growth and G satisfying Definition 4.2, the integrand
\gamma_G(a,c)\beta(\langle a,x\rangle+c) is absolutely integrable on the product space.
Its integral is the ordinary network with finite coefficient measure \gamma_G\lambda_\alpha
and equals C_{\beta,\rho}^{(\alpha)}g_G(x). This identity allows a zero constant.
Non-polynomiality is needed separately to choose a band-pass filter with a nonzero constant,
then normalize it for reconstruction or universality. A polynomial activation has zero
band-pass pairing.
Lean code for Theorem4.5●11 theorems
Associated Lean declarations
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OperatorRidgelet.Paper.thm_4_5_i_a[complete]
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OperatorRidgelet.Paper.thm_4_5_i_b[complete]
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OperatorRidgelet.Paper.thm_4_5_i_c[complete]
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OperatorRidgelet.Paper.thm_4_5_ii_a[complete]
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OperatorRidgelet.Paper.thm_4_5_ii_b[complete]
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OperatorRidgelet.Paper.thm_4_5_ii_c[complete]
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OperatorRidgelet.Paper.thm_4_5_iii_a[complete]
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OperatorRidgelet.Paper.thm_4_5_iii_b[complete]
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OperatorRidgelet.Paper.thm_4_5_iii_c[complete]
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OperatorRidgelet.Paper.thm_4_5_iii_d[complete]
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OperatorRidgelet.Paper.thm_4_5_iii_e[complete]
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OperatorRidgelet.Paper.thm_4_5_i_a[complete] -
OperatorRidgelet.Paper.thm_4_5_i_b[complete] -
OperatorRidgelet.Paper.thm_4_5_i_c[complete] -
OperatorRidgelet.Paper.thm_4_5_ii_a[complete] -
OperatorRidgelet.Paper.thm_4_5_ii_b[complete] -
OperatorRidgelet.Paper.thm_4_5_ii_c[complete] -
OperatorRidgelet.Paper.thm_4_5_iii_a[complete] -
OperatorRidgelet.Paper.thm_4_5_iii_b[complete] -
OperatorRidgelet.Paper.thm_4_5_iii_c[complete] -
OperatorRidgelet.Paper.thm_4_5_iii_d[complete] -
OperatorRidgelet.Paper.thm_4_5_iii_e[complete]
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theoremdefined in OperatorRidgelet/Paper/Reconstruction.leancomplete
theorem OperatorRidgelet.Paper.thm_4_5_i_a.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [MeasurableSpace H] (ν : MeasureTheory.Measure H) (G : H → ℂ) (hG : Measurable G) (hG₁ : MeasureTheory.Integrable G ν) (x : H) : ‖OperatorRidgelet.spectralTarget ν G x‖ ≤ ∫ (ξ : H), ‖G ξ‖ ∂ν
theorem OperatorRidgelet.Paper.thm_4_5_i_a.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [MeasurableSpace H] (ν : MeasureTheory.Measure H) (G : H → ℂ) (hG : Measurable G) (hG₁ : MeasureTheory.Integrable G ν) (x : H) : ‖OperatorRidgelet.spectralTarget ν G x‖ ≤ ∫ (ξ : H), ‖G ξ‖ ∂ν
**Theorem [thm:4.5]** Integral representation of targets with a spectral density. For `G ∈ L¹(ν_α)` the target `g_G` is bounded by `‖G‖_{L¹(ν_α)}`. -
theoremdefined in OperatorRidgelet/Paper/Reconstruction.leancomplete
theorem OperatorRidgelet.Paper.thm_4_5_i_b.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) (G : H → ℂ) (hG : Measurable G) (hG₁ : MeasureTheory.Integrable G ν) : Continuous (OperatorRidgelet.spectralTarget ν G)
theorem OperatorRidgelet.Paper.thm_4_5_i_b.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) (G : H → ℂ) (hG : Measurable G) (hG₁ : MeasureTheory.Integrable G ν) : Continuous (OperatorRidgelet.spectralTarget ν G)
**Theorem [thm:4.5]** Integral representation of targets with a spectral density. For `G ∈ L¹(ν_α)` the target `g_G` is continuous.
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theoremdefined in OperatorRidgelet/Paper/Reconstruction.leancomplete
theorem OperatorRidgelet.Paper.thm_4_5_i_c.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) (G : H → ℂ) (hG : Measurable G) (hG₁ : MeasureTheory.Integrable G ν) (h : OperatorRidgelet.spectralTarget ν G = 0) : G =ᵐ[ν] 0
theorem OperatorRidgelet.Paper.thm_4_5_i_c.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) (G : H → ℂ) (hG : Measurable G) (hG₁ : MeasureTheory.Integrable G ν) (h : OperatorRidgelet.spectralTarget ν G = 0) : G =ᵐ[ν] 0
**Theorem [thm:4.5]** Integral representation of targets with a spectral density. For `G ∈ L¹(ν_α)`, `g_G = 0` only if `G = 0` `ν_α`-almost everywhere.
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theoremdefined in OperatorRidgelet/Paper/Reconstruction.leancomplete
theorem OperatorRidgelet.Paper.thm_4_5_ii_a.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) [MeasureTheory.SigmaFinite ν] [ν.IsOpenPosMeasure] {α : ℝ} (hα : 0 < α) (hν : OperatorRidgelet.IsHomogeneous α ν) (ρ : SchwartzMap ℝ ℝ) (hρ : OperatorRidgelet.IsAdmissible α ρ) (G : H → ℂ) (hG : Measurable G) (hG₁ : MeasureTheory.Integrable G ν) (hG₂ : MeasureTheory.MemLp G 2 ν) (x : H) : (∀ᵐ (a : H) ∂ν, MeasureTheory.Integrable (fun c => OperatorRidgelet.coefficientFormula (⇑ρ) G (a, c) * ↑(ρ (inner ℝ a x + c))) MeasureTheory.volume) ∧ MeasureTheory.Integrable (fun a => ∫ (c : ℝ), OperatorRidgelet.coefficientFormula (⇑ρ) G (a, c) * ↑(ρ (inner ℝ a x + c))) ν
theorem OperatorRidgelet.Paper.thm_4_5_ii_a.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) [MeasureTheory.SigmaFinite ν] [ν.IsOpenPosMeasure] {α : ℝ} (hα : 0 < α) (hν : OperatorRidgelet.IsHomogeneous α ν) (ρ : SchwartzMap ℝ ℝ) (hρ : OperatorRidgelet.IsAdmissible α ρ) (G : H → ℂ) (hG : Measurable G) (hG₁ : MeasureTheory.Integrable G ν) (hG₂ : MeasureTheory.MemLp G 2 ν) (x : H) : (∀ᵐ (a : H) ∂ν, MeasureTheory.Integrable (fun c => OperatorRidgelet.coefficientFormula (⇑ρ) G (a, c) * ↑(ρ (inner ℝ a x + c))) MeasureTheory.volume) ∧ MeasureTheory.Integrable (fun a => ∫ (c : ℝ), OperatorRidgelet.coefficientFormula (⇑ρ) G (a, c) * ↑(ρ (inner ℝ a x + c))) ν
**Theorem [thm:4.5]** Integral representation of targets with a spectral density. For `G ∈ L¹(ν_α) ∩ L²(ν_α)` and every `x`, the iterated integral `∫ [∫ γ_G(a,c) ρ(⟨a,x⟩+c) dc] ν_α(da)` converges absolutely: the inner integral converges absolutely for `ν_α`-almost every `a`, and the outer integrand is `ν_α`-integrable.
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theoremdefined in OperatorRidgelet/Paper/Reconstruction.leancomplete
theorem OperatorRidgelet.Paper.thm_4_5_ii_b.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) [MeasureTheory.SigmaFinite ν] [ν.IsOpenPosMeasure] {α : ℝ} (hα : 0 < α) (hν : OperatorRidgelet.IsHomogeneous α ν) (ρ : SchwartzMap ℝ ℝ) (hρ : OperatorRidgelet.IsAdmissible α ρ) (G : H → ℂ) (hG : Measurable G) (hG₁ : MeasureTheory.Integrable G ν) (hG₂ : MeasureTheory.MemLp G 2 ν) (x : H) : ∫ (a : H), ∫ (c : ℝ), OperatorRidgelet.coefficientFormula (⇑ρ) G (a, c) * ↑(ρ (inner ℝ a x + c)) ∂ν = ↑(OperatorRidgelet.admissibilityConst α ⇑ρ) * OperatorRidgelet.spectralTarget ν G x
theorem OperatorRidgelet.Paper.thm_4_5_ii_b.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) [MeasureTheory.SigmaFinite ν] [ν.IsOpenPosMeasure] {α : ℝ} (hα : 0 < α) (hν : OperatorRidgelet.IsHomogeneous α ν) (ρ : SchwartzMap ℝ ℝ) (hρ : OperatorRidgelet.IsAdmissible α ρ) (G : H → ℂ) (hG : Measurable G) (hG₁ : MeasureTheory.Integrable G ν) (hG₂ : MeasureTheory.MemLp G 2 ν) (x : H) : ∫ (a : H), ∫ (c : ℝ), OperatorRidgelet.coefficientFormula (⇑ρ) G (a, c) * ↑(ρ (inner ℝ a x + c)) ∂ν = ↑(OperatorRidgelet.admissibilityConst α ⇑ρ) * OperatorRidgelet.spectralTarget ν G x
**Theorem [thm:4.5]** Integral representation of targets with a spectral density. For `G ∈ L¹(ν_α) ∩ L²(ν_α)` the spectral synthesis identity `∫ [∫ γ_G(a,c) ρ(⟨a,x⟩+c) dc] ν_α(da) = C^{(α)}_ρ g_G(x)` holds for every `x`. -
theoremdefined in OperatorRidgelet/Paper/Reconstruction.leancomplete
theorem OperatorRidgelet.Paper.thm_4_5_ii_c.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) [MeasureTheory.SigmaFinite ν] [ν.IsOpenPosMeasure] {α : ℝ} (hα : 0 < α) (hν : OperatorRidgelet.IsHomogeneous α ν) (ρ : SchwartzMap ℝ ℝ) (hρ : OperatorRidgelet.IsAdmissible α ρ) (G : H → ℂ) (hG : Measurable G) (hG₁ : MeasureTheory.Integrable G ν) (hG₂ : MeasureTheory.MemLp G 2 ν) (hγ : MeasureTheory.Integrable (OperatorRidgelet.coefficientFormula (⇑ρ) G) (OperatorRidgelet.parameterMeasure ν)) (x : H) : ∫ (a : H), ∫ (c : ℝ), OperatorRidgelet.coefficientFormula (⇑ρ) G (a, c) * ↑(ρ (inner ℝ a x + c)) ∂ν = OperatorRidgelet.integralNetworkDensity (fun t => ↑(ρ t)) (OperatorRidgelet.parameterMeasure ν) (OperatorRidgelet.coefficientFormula (⇑ρ) G) x
theorem OperatorRidgelet.Paper.thm_4_5_ii_c.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) [MeasureTheory.SigmaFinite ν] [ν.IsOpenPosMeasure] {α : ℝ} (hα : 0 < α) (hν : OperatorRidgelet.IsHomogeneous α ν) (ρ : SchwartzMap ℝ ℝ) (hρ : OperatorRidgelet.IsAdmissible α ρ) (G : H → ℂ) (hG : Measurable G) (hG₁ : MeasureTheory.Integrable G ν) (hG₂ : MeasureTheory.MemLp G 2 ν) (hγ : MeasureTheory.Integrable (OperatorRidgelet.coefficientFormula (⇑ρ) G) (OperatorRidgelet.parameterMeasure ν)) (x : H) : ∫ (a : H), ∫ (c : ℝ), OperatorRidgelet.coefficientFormula (⇑ρ) G (a, c) * ↑(ρ (inner ℝ a x + c)) ∂ν = OperatorRidgelet.integralNetworkDensity (fun t => ↑(ρ t)) (OperatorRidgelet.parameterMeasure ν) (OperatorRidgelet.coefficientFormula (⇑ρ) G) x
**Theorem [thm:4.5]** Integral representation of targets with a spectral density. If moreover `γ_G ∈ L¹(λ_α)`, the left side of the spectral synthesis identity is the integral network `S_ρ[γ_G λ_α](x)`.
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theoremdefined in OperatorRidgelet/Paper/Reconstruction.leancomplete
theorem OperatorRidgelet.Paper.thm_4_5_iii_a.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) [MeasureTheory.SigmaFinite ν] [ν.IsOpenPosMeasure] {α : ℝ} (hα : 0 < α) (hν : OperatorRidgelet.IsHomogeneous α ν) (ρ : SchwartzMap ℝ ℝ) (hρ : OperatorRidgelet.IsBandPass ρ) (I : Set ℝ) (hI : OperatorRidgelet.IsFrequencyWindow (⇑ρ) I) (β : TemperedDistribution ℝ ℂ) (b : ℝ → ℝ) (hβ : OperatorRidgelet.IsTemperedFunction β b) (G : H → ℂ) (hG : OperatorRidgelet.IsRegularAlongRays ν I G) (x : H) : ∀ᵐ (a : H) ∂ν, MeasureTheory.Integrable (fun c => OperatorRidgelet.coefficientFormula (⇑ρ) G (a, c) * ↑(b (inner ℝ a x + c))) MeasureTheory.volume
theorem OperatorRidgelet.Paper.thm_4_5_iii_a.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) [MeasureTheory.SigmaFinite ν] [ν.IsOpenPosMeasure] {α : ℝ} (hα : 0 < α) (hν : OperatorRidgelet.IsHomogeneous α ν) (ρ : SchwartzMap ℝ ℝ) (hρ : OperatorRidgelet.IsBandPass ρ) (I : Set ℝ) (hI : OperatorRidgelet.IsFrequencyWindow (⇑ρ) I) (β : TemperedDistribution ℝ ℂ) (b : ℝ → ℝ) (hβ : OperatorRidgelet.IsTemperedFunction β b) (G : H → ℂ) (hG : OperatorRidgelet.IsRegularAlongRays ν I G) (x : H) : ∀ᵐ (a : H) ∂ν, MeasureTheory.Integrable (fun c => OperatorRidgelet.coefficientFormula (⇑ρ) G (a, c) * ↑(b (inner ℝ a x + c))) MeasureTheory.volume
**Theorem [thm:4.5]** Integral representation of targets with a spectral density. For a tempered `β` that is a continuous function `b` of polynomial growth, and `G` regular along rays, the inner integral `∫ γ_G(a,c) β(⟨a,x⟩+c) dc` converges absolutely for `ν_α`-almost every `a`.
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theoremdefined in OperatorRidgelet/Paper/Reconstruction.leancomplete
theorem OperatorRidgelet.Paper.thm_4_5_iii_b.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) [MeasureTheory.SigmaFinite ν] [ν.IsOpenPosMeasure] {α : ℝ} (hα : 0 < α) (hν : OperatorRidgelet.IsHomogeneous α ν) (ρ : SchwartzMap ℝ ℝ) (hρ : OperatorRidgelet.IsBandPass ρ) (I : Set ℝ) (hI : OperatorRidgelet.IsFrequencyWindow (⇑ρ) I) (β : TemperedDistribution ℝ ℂ) (b : ℝ → ℝ) (hβ : OperatorRidgelet.IsTemperedFunction β b) (G : H → ℂ) (hG : OperatorRidgelet.IsRegularAlongRays ν I G) (x : H) : MeasureTheory.Integrable (fun a => ∫ (c : ℝ), OperatorRidgelet.coefficientFormula (⇑ρ) G (a, c) * ↑(b (inner ℝ a x + c))) ν
theorem OperatorRidgelet.Paper.thm_4_5_iii_b.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) [MeasureTheory.SigmaFinite ν] [ν.IsOpenPosMeasure] {α : ℝ} (hα : 0 < α) (hν : OperatorRidgelet.IsHomogeneous α ν) (ρ : SchwartzMap ℝ ℝ) (hρ : OperatorRidgelet.IsBandPass ρ) (I : Set ℝ) (hI : OperatorRidgelet.IsFrequencyWindow (⇑ρ) I) (β : TemperedDistribution ℝ ℂ) (b : ℝ → ℝ) (hβ : OperatorRidgelet.IsTemperedFunction β b) (G : H → ℂ) (hG : OperatorRidgelet.IsRegularAlongRays ν I G) (x : H) : MeasureTheory.Integrable (fun a => ∫ (c : ℝ), OperatorRidgelet.coefficientFormula (⇑ρ) G (a, c) * ↑(b (inner ℝ a x + c))) ν
**Theorem [thm:4.5]** Integral representation of targets with a spectral density. For a tempered `β` that is a continuous function `b` of polynomial growth, and `G` regular along rays, the `ν_α`-integral of the inner integral converges absolutely.
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theoremdefined in OperatorRidgelet/Paper/Reconstruction.leancomplete
theorem OperatorRidgelet.Paper.thm_4_5_iii_c.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) [MeasureTheory.SigmaFinite ν] [ν.IsOpenPosMeasure] {α : ℝ} (hα : 0 < α) (hν : OperatorRidgelet.IsHomogeneous α ν) (ρ : SchwartzMap ℝ ℝ) (hρ : OperatorRidgelet.IsBandPass ρ) (I : Set ℝ) (hI : OperatorRidgelet.IsFrequencyWindow (⇑ρ) I) (β : TemperedDistribution ℝ ℂ) (b : ℝ → ℝ) (hβ : OperatorRidgelet.IsTemperedFunction β b) (G : H → ℂ) (hG : OperatorRidgelet.IsRegularAlongRays ν I G) (x : H) : ∫ (a : H), ∫ (c : ℝ), OperatorRidgelet.coefficientFormula (⇑ρ) G (a, c) * ↑(b (inner ℝ a x + c)) ∂ν = OperatorRidgelet.temperedAdmissibilityConst α β ρ * OperatorRidgelet.spectralTarget ν G x
theorem OperatorRidgelet.Paper.thm_4_5_iii_c.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [CompleteSpace H] [SecondCountableTopology H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) [MeasureTheory.SigmaFinite ν] [ν.IsOpenPosMeasure] {α : ℝ} (hα : 0 < α) (hν : OperatorRidgelet.IsHomogeneous α ν) (ρ : SchwartzMap ℝ ℝ) (hρ : OperatorRidgelet.IsBandPass ρ) (I : Set ℝ) (hI : OperatorRidgelet.IsFrequencyWindow (⇑ρ) I) (β : TemperedDistribution ℝ ℂ) (b : ℝ → ℝ) (hβ : OperatorRidgelet.IsTemperedFunction β b) (G : H → ℂ) (hG : OperatorRidgelet.IsRegularAlongRays ν I G) (x : H) : ∫ (a : H), ∫ (c : ℝ), OperatorRidgelet.coefficientFormula (⇑ρ) G (a, c) * ↑(b (inner ℝ a x + c)) ∂ν = OperatorRidgelet.temperedAdmissibilityConst α β ρ * OperatorRidgelet.spectralTarget ν G x
**Theorem [thm:4.5]** Integral representation of targets with a spectral density. For a tempered `β` that is a continuous function `b` of polynomial growth, and `G` regular along rays, the tempered spectral synthesis identity `∫ [∫ γ_G(a,c) β(⟨a,x⟩+c) dc] ν_α(da) = C^{(α)}_{β,ρ} g_G(x)` holds. -
theoremdefined in OperatorRidgelet/Paper/Reconstruction.leancomplete
theorem OperatorRidgelet.Paper.thm_4_5_iii_d {α : ℝ} (hα : 0 < α) (β : TemperedDistribution ℝ ℂ) (b : ℝ → ℝ) (hβ : OperatorRidgelet.IsTemperedFunction β b) (hb : ¬OperatorRidgelet.IsPolynomialFun b) : ∃ ρ, OperatorRidgelet.IsBandPass ρ ∧ OperatorRidgelet.temperedAdmissibilityConst α β ρ ≠ 0
theorem OperatorRidgelet.Paper.thm_4_5_iii_d {α : ℝ} (hα : 0 < α) (β : TemperedDistribution ℝ ℂ) (b : ℝ → ℝ) (hβ : OperatorRidgelet.IsTemperedFunction β b) (hb : ¬OperatorRidgelet.IsPolynomialFun b) : ∃ ρ, OperatorRidgelet.IsBandPass ρ ∧ OperatorRidgelet.temperedAdmissibilityConst α β ρ ≠ 0
**Theorem [thm:4.5]** Integral representation of targets with a spectral density. For every tempered `β` that is a continuous function of polynomial growth and not a polynomial, there is a band-pass filter `ρ` with `C^{(α)}_{β,ρ} ≠ 0`. -
theoremdefined in OperatorRidgelet/Paper/Revision.leancomplete
theorem OperatorRidgelet.Paper.thm_4_5_iii_e.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) [MeasureTheory.SigmaFinite ν] (ρ : SchwartzMap ℝ ℝ) (hρ : OperatorRidgelet.IsBandPass ρ) (I : Set ℝ) (hI : OperatorRidgelet.IsFrequencyWindow (⇑ρ) I) (β : TemperedDistribution ℝ ℂ) (b : ℝ → ℝ) (hβ : OperatorRidgelet.IsTemperedFunction β b) (G : H → ℂ) (hG : OperatorRidgelet.IsRegularAlongRays ν I G) (x : H) : MeasureTheory.Integrable (fun θ => OperatorRidgelet.coefficientFormula (⇑ρ) G θ * ↑(b (inner ℝ θ.1 x + θ.2))) (OperatorRidgelet.parameterMeasure ν)
theorem OperatorRidgelet.Paper.thm_4_5_iii_e.{u_1} {H : Type u_1} [NormedAddCommGroup H] [InnerProductSpace ℝ H] [MeasurableSpace H] [BorelSpace H] (ν : MeasureTheory.Measure H) [MeasureTheory.SigmaFinite ν] (ρ : SchwartzMap ℝ ℝ) (hρ : OperatorRidgelet.IsBandPass ρ) (I : Set ℝ) (hI : OperatorRidgelet.IsFrequencyWindow (⇑ρ) I) (β : TemperedDistribution ℝ ℂ) (b : ℝ → ℝ) (hβ : OperatorRidgelet.IsTemperedFunction β b) (G : H → ℂ) (hG : OperatorRidgelet.IsRegularAlongRays ν I G) (x : H) : MeasureTheory.Integrable (fun θ => OperatorRidgelet.coefficientFormula (⇑ρ) G θ * ↑(b (inner ℝ θ.1 x + θ.2))) (OperatorRidgelet.parameterMeasure ν)
**Theorem [thm:4.5]** The network integrand is jointly absolutely integrable.
Part (i) is Lemma 4.1. Parseval in the bias turns the inner
integral into a frequency integral of
\rho^\sharp(\omega)G(-\omega a) against \rho^\sharp(-\omega)e^{-i\omega\langle a,x\rangle},
and the homogeneous substitution \xi=-\omega a separates the admissibility constant from
g_G(x). For a tempered \beta the bias integral is a distributional pairing with a test
function supported in -\operatorname{supp}\rho^\sharp; Definition 4.2 makes
a\mapsto (test function) Bochner integrable in a C^m norm, so the pairing commutes with
the direction integral. Joint absolute integrability follows independently from
Lemma 4.3, choosing a moment at least as large as the
activation's polynomial growth order. If every band-pass test function paired to zero with
\beta^\sharp, its support would be \{0\} and \beta a polynomial.