AutoSamplingTheory.TechnicalLemmas.InformationTheory.RelativeFisher
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7 named declarations scanned from AutoSamplingTheory/TechnicalLemmas/InformationTheory/RelativeFisher.lean.
Declarations
abbrev AutoSamplingTheory.TechnicalLemmas.InformationTheory.RelativeFisher.State Partial Not mapped
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abbrev State := EuclideanSpace ℝ ι
/-- Pointwise relative-Fisher energy for a supplied density and a supplied
log-density ratio. -/
AutoSamplingTheory/TechnicalLemmas/InformationTheory/RelativeFisher.lean:38published source at 0e31a3cda412
def AutoSamplingTheory.TechnicalLemmas.InformationTheory.RelativeFisher.densityEnergy Partial Not mapped
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- Pointwise relative-Fisher energy for a supplied density and a supplied log-density ratio.
noncomputable def densityEnergy
(q logRatio : State (ι := ι) → ℝ) (x : State (ι := ι)) : ℝ :=
q x * ‖gradient logRatio x‖ ^ 2
/-- Relative Fisher information with respect to an explicit base measure.
For the usual Euclidean density representation the base measure will be
Lebesgue measure and `q` will be the density of `mu`; equivalently the integral
is `integral ||grad log(d mu / d pi)||^2 d mu` after the Radon--Nikodym bridge is
proved. -/
AutoSamplingTheory/TechnicalLemmas/InformationTheory/RelativeFisher.lean:42published source at 0e31a3cda412
def AutoSamplingTheory.TechnicalLemmas.InformationTheory.RelativeFisher.information Partial Not mapped
Read the complete mathematical statement and proof, with Lean below each
- Relative Fisher information with respect to an explicit base measure. For the usual Euclidean density representation the base measure will be Lebesgue measure and `q` will be the density of `mu`; equivalently the integral is `integral ||grad log(d mu / d pi)||^2 d mu` after the Radon--Nikodym bridge is proved.
noncomputable def information
(base : Measure (State (ι := ι)))
(q logRatio : State (ι := ι) → ℝ) : ℝ :=
∫ x, densityEnergy q logRatio x ∂base
/-- Fisher energy density is nonnegative wherever the supplied density is
nonnegative. -/
AutoSamplingTheory/TechnicalLemmas/InformationTheory/RelativeFisher.lean:52published source at 0e31a3cda412
theorem AutoSamplingTheory.TechnicalLemmas.InformationTheory.RelativeFisher.densityEnergy_nonneg Partial Not mapped
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- Fisher energy density is nonnegative wherever the supplied density is nonnegative.
theorem densityEnergy_nonneg
{q logRatio : State (ι := ι) → ℝ} {x : State (ι := ι)}
(hq : 0 ≤ q x) :
0 ≤ densityEnergy q logRatio x := by
exact mul_nonneg hq (sq_nonneg _)
/-- A vanishing relative score gives zero pointwise Fisher energy. -/
AutoSamplingTheory/TechnicalLemmas/InformationTheory/RelativeFisher.lean:59published source at 0e31a3cda412
theorem AutoSamplingTheory.TechnicalLemmas.InformationTheory.RelativeFisher.densityEnergy_eq_zero_of_gradient_eq_zero Partial Not mapped
Read the complete mathematical statement and proof, with Lean below each
- A vanishing relative score gives zero pointwise Fisher energy.
theorem densityEnergy_eq_zero_of_gradient_eq_zero
{q logRatio : State (ι := ι) → ℝ} {x : State (ι := ι)}
(hgrad : gradient logRatio x = 0) :
densityEnergy q logRatio x = 0 := by
simp [densityEnergy, hgrad]
/-- If the relative score vanishes almost everywhere, then the relative Fisher
information vanishes. This statement needs no positivity or normalization
assumption on `q`; those belong to the source-facing density bridge. -/
AutoSamplingTheory/TechnicalLemmas/InformationTheory/RelativeFisher.lean:66published source at 0e31a3cda412
theorem AutoSamplingTheory.TechnicalLemmas.InformationTheory.RelativeFisher.information_eq_zero_of_gradient_ae_eq_zero Partial Not mapped
Read the complete mathematical statement and proof, with Lean below each
- If the relative score vanishes almost everywhere, then the relative Fisher information vanishes. This statement needs no positivity or normalization assumption on `q`; those belong to the source-facing density bridge.
theorem information_eq_zero_of_gradient_ae_eq_zero
(base : Measure (State (ι := ι)))
(q logRatio : State (ι := ι) → ℝ)
(hgrad : ∀ᵐ x ∂base, gradient logRatio x = 0) :
information base q logRatio = 0 := by
rw [information]
apply integral_eq_zero_of_ae
filter_upwards [hgrad] with x hx
exact densityEnergy_eq_zero_of_gradient_eq_zero hx
/-- The Fisher functional is insensitive to changing the supplied log-ratio on
an a.e. set *provided its gradients themselves agree a.e.*. This is the exact
representative-level congruence needed after a Sobolev/Radon--Nikodym layer has
chosen versions. -/
AutoSamplingTheory/TechnicalLemmas/InformationTheory/RelativeFisher.lean:75published source at 0e31a3cda412
theorem AutoSamplingTheory.TechnicalLemmas.InformationTheory.RelativeFisher.information_congr_gradient_ae Partial Not mapped
Read the complete mathematical statement and proof, with Lean below each
- The Fisher functional is insensitive to changing the supplied log-ratio on an a.e. set *provided its gradients themselves agree a.e.*. This is the exact representative-level congruence needed after a Sobolev/Radon--Nikodym layer has chosen versions.
theorem information_congr_gradient_ae
(base : Measure (State (ι := ι)))
(q r s : State (ι := ι) → ℝ)
(hgrad : ∀ᵐ x ∂base, gradient r x = gradient s x) :
information base q r = information base q s := by
rw [information, information]
apply integral_congr_ae
filter_upwards [hgrad] with x hx
simp [densityEnergy, hx]
end
end RelativeFisher
end InformationTheory
end TechnicalLemmas
end AutoSamplingTheory
AutoSamplingTheory/TechnicalLemmas/InformationTheory/RelativeFisher.lean:89published source at 0e31a3cda412