Plain-English statement
- Positive finite normalization and exact product-law identification for the actual target phase energy. Integrability and all density identities are derived internally; no normalizer or minimizer is an additional hypothesis.
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Lean statement
theorem actual_phase_gibbs_normalization
{E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E]
[FiniteDimensional ℝ E] [MeasurableSpace E] [BorelSpace E]
{V : E → ℝ} {α β : ℝ≥0} {η : ℝ}
(hα : 0 < (α : ℝ)) (hαβ : α ≤ β) (hV : ContDiff ℝ 2 V)
(hH : ∀ x v : E,
(α : ℝ) * ‖v‖ ^ 2 ≤ (fderiv ℝ (fderiv ℝ V) x v) v ∧
(fderiv ℝ (fderiv ℝ V) x v) v ≤ (β : ℝ) * ‖v‖ ^ 2)
(hη : 0 < η) (hβη : (β : ℝ) * η ≤ 1) : actual_phase_normalization_statement hα hαβ hV hH hη hβη := by
dsimp only [actual_phase_normalization_statement]
intro y
let Vy : E → ℝ := fun x => V x + ‖x - y‖ ^ 2 / (2 * η)
let U : E × E → ℝ := fun z => V z.1 + ‖z.1 - y‖ ^ 2 / (2 * η) + ‖z.2‖ ^ 2 / 2
let f : E → ℝ := fun x => Real.exp (-Vy x)
let g : E → ℝ := fun p => Real.exp (-‖p‖ ^ 2 / 2)
let C : ℝ := (Real.sqrt (2 * Real.pi)) ^ Module.finrank ℝ E
let Z : ℝ := ∫ x, f x ∂(volume : Measure E)
let ell : Measure (E × E) := (volume : Measure E).prod (volume : Measure E)
let Zp : ℝ≥0∞ := ∫⁻ z, ENNReal.ofReal (Real.exp (-U z)) ∂ell
change Integrable f volume ∧ 0 < Z ∧ Zp = ENNReal.ofReal (Z * C) ∧
0 < Zp ∧ Zp < ⊤ ∧
IsProbabilityMeasure (ell.withDensity (fun z => Zp⁻¹ * ENNReal.ofReal (Real.exp (-U z)))) ∧
ell.withDensity (fun z => Zp⁻¹ * ENNReal.ofReal (Real.exp (-U z))) =
((volume : Measure E).tilted (fun x => -Vy x)).prod (stdGaussian E)
have hsc := AutoSamplingTheory.TechnicalLemmas.Analysis.HessianStrongConvexity.strongConvexOn_univ_of_fderiv2_lower hV (fun x v => (hH x v).1)
have hbase := AutoSamplingTheory.TechnicalLemmas.Analysis.StrongConvexGibbsIntegrability.integrable_exp_neg_of_strongConvexOn hα (hV.differentiable (by norm_num)) hsc
have hVy : Continuous Vy := hV.continuous.add (((continuous_id.sub continuous_const).norm.pow 2).div_const (2 * η))
have hfc : Continuous f := Real.continuous_exp.comp hVy.neg
have hgc : Continuous g := Real.continuous_exp.comp ((continuous_norm.pow 2).neg.div_const 2)
have hf : Integrable f (volume : Measure E) := by
refine hbase.mono' hfc.aestronglyMeasurable ?_
filter_upwards with x
rw [Real.norm_eq_abs, abs_of_pos (Real.exp_pos _)]
apply Real.exp_le_exp.mpr
dsimp [Vy]
have : 0 ≤ ‖x - y‖ ^ 2 / (2 * η) := by positivity
linarith
have hZ : 0 < Z := integral_exp_pos hf
have hC : 0 < C := by dsimp [C]; positivity
have hCg : (∫⁻ p : E, ENNReal.ofReal (g p) ∂volume) = ENNReal.ofReal C := by
have h := AutoSamplingTheory.TechnicalLemmas.Analysis.Integrability.lintegral_exp_neg_mul_norm_sq_eq (E := E) (a := (1 / 2 : ℝ)) (by norm_num)
have hn : (Real.pi / (1 / 2 : ℝ)) ^ ((Module.finrank ℝ E : ℝ) / 2) = C := by
dsimp [C]
rw [Real.sqrt_eq_rpow, ← Real.rpow_mul_natCast (by positivity)]
congr 1 <;> ring
rw [hn] at h
convert h using 1
congr 1
funext p
congr 2
dsimp [g]
ring
have hw (z : E × E) : Real.exp (-U z) = f z.1 * g z.2 := by
dsimp [U, f, g, Vy]
rw [← Real.exp_add]
congr 1
ring
have hphase : Zp = ENNReal.ofReal (Z * C) := by
calc
Zp = ∫⁻ z : E × E, ENNReal.ofReal (f z.1) * ENNReal.ofReal (g z.2) ∂ell := by
apply lintegral_congr
intro z
rw [hw, ENNReal.ofReal_mul (Real.exp_nonneg _)]
_ = (∫⁻ x : E, ENNReal.ofReal (f x) ∂volume) * ∫⁻ p : E, ENNReal.ofReal (g p) ∂volume :=
lintegral_prod_mul hfc.measurable.ennreal_ofReal.aemeasurable hgc.measurable.ennreal_ofReal.aemeasurable
_ = ENNReal.ofReal (Z * C) := by
rw [← ofReal_integral_eq_lintegral_ofReal hf (ae_of_all _ (fun x => Real.exp_nonneg _)), hCg, ← ENNReal.ofReal_mul hZ.le]
have hpos : 0 < Zp := by rw [hphase]; exact ENNReal.ofReal_pos.mpr (mul_pos hZ hC)
have hfin : Zp < ⊤ := by rw [hphase]; exact ENNReal.ofReal_lt_top
have hprob : IsProbabilityMeasure (ell.withDensity (fun z => Zp⁻¹ * ENNReal.ofReal (Real.exp (-U z)))) :=
AutoSamplingTheory.TechnicalLemmas.Measure.Gibbs.isProbabilityMeasure_withDensity_normalized_gibbs ell U hpos.ne' hfin.ne
refine ⟨hf, hZ, hphase, hpos, hfin, hprob, ?_⟩
have hgamma : stdGaussian E = (volume : Measure E).withDensity (fun p => ENNReal.ofReal (C⁻¹ * g p)) := by
have h := AutoSamplingTheory.TechnicalLemmas.Measure.IsotropicGaussianDensity.map_sqrt_smul_stdGaussian_eq_withDensity (E := E) 1 (by norm_num)
have hid : (fun z : E => Real.sqrt 1 • z) = id := by funext z; simp
rw [hid, Measure.map_id] at h
simpa only [mul_one, inv_pow, C, g] using h
rw [hgamma, Measure.tilted, prod_withDensity ((hfc.measurable.div_const Z).ennreal_ofReal) ((hgc.measurable.const_mul C⁻¹).ennreal_ofReal)]
apply withDensity_congr_ae
filter_upwards with z
rw [hphase, hw, ENNReal.ofReal_mul hZ.le, ENNReal.ofReal_mul (Real.exp_nonneg _), ENNReal.ofReal_div_of_pos hZ, ENNReal.ofReal_mul (inv_nonneg.mpr hC.le), ENNReal.ofReal_inv_of_pos hC]
rw [ENNReal.mul_inv (Or.inr ENNReal.ofReal_ne_top) (Or.inl ENNReal.ofReal_ne_top)]
simp only [div_eq_mul_inv, f]
ac_rfl
#print axioms actual_phase_gibbs_normalization
end
end AutoSamplingTheory.ExampleCases.ProximalBPS.ActualPhaseNormalization
Open AutoSamplingTheory/ExampleCases/ProximalBPS/ActualPhaseNormalization.lean:61published source at ed709a7f320d
Proof architecture
Actual conditional position-momentum phase law; no SALD claim
Lean proof walkthrough
- Read the quantified variables and typeclass brackets as part of the mathematical statement; inferred arguments are not missing assumptions.
- `intro` introduces quantified hypotheses into the local proof context.
- `have` creates a named intermediate mathematical fact.
- `calc` records an equality or inequality chain matching a paper calculation.
- `rw` rewrites by an established identity.
- `simp` normalizes through registered definitional and theorem rewrites.
- `apply` reduces the goal to the hypotheses of a reusable theorem.
- `refine` instantiates a reusable theorem while leaving explicit subgoals.
Why the statement has this shape
The declaration is kept at the reusable level recorded by its Registry tags and direct consumers. Explicit measures, spaces, wrappers, and regularity hypotheses expose interfaces that paper notation often infers. A theorem card explains those interfaces but never widens the compiled statement.
Hidden assumptions and non-claims
- Measurability is represented explicitly or must be supplied by a dependency.
- Integrability is an input or proved output; a displayed integral alone does not supply it.
- Totalized `fderiv` values must not be read as a differentiability theorem.
- Genuine differentiability is localized to the hypotheses shown in the Lean statement.
- Almost-everywhere hypotheses depend on the stated measure and representative.
- Density statements retain normalization and absolute-continuity prerequisites.
- A Gibbs expression is not automatically a probability law or an invariant law.