openAI-math-dataset / lean /OAI /Probability /SKGap /Entropy /NormalizedWeightedMean.lean
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import Mathlib
import OAI.Probability.SKGap.Entropy.WeightedMean
namespace OAI
section
noncomputable section
open scoped BigOperators
namespace SKGapCutoff.Recipe
open Primary Static
variable {n : ℕ}
def squareMass (P : Observables n) (f : Observables n) (x : Spin n) : ℝ :=
P x*(f x)^2/(∑y,P y*(f y)^2)
def squareMean (P : Observables n) (f : Observables n) (i : Fin n) : ℝ :=
∑x,squareMass P f x*spin x i
lemma squareMass_probability (P f : Observables n) (hP : ∀x,0≤P x)
(hN : 0<∑x,P x*(f x)^2) :
(∀x,0 ≤ squareMass P f x) ∧ ∑x,squareMass P f x=1 := by
refine ⟨fun x=>div_nonneg (mul_nonneg (hP x) (sq_nonneg _)) hN.le,?_⟩
simp only [squareMass,←Finset.sum_div,div_self (ne_of_gt hN)]
lemma squareMean_centered (P f : Observables n) (t : Fin n→ℝ)
(hN : 0<∑x,P x*(f x)^2) :
squareMean P f-t=fun i=>(∑x,P x*(f x)^2*(spin x i-t i))/(∑x,P x*(f x)^2) := by
ext i
simp only [squareMean,squareMass,Pi.sub_apply,div_mul_eq_mul_div,←Finset.sum_div,
mul_sub,Finset.sum_sub_distrib,←Finset.sum_mul,sub_div]
rw [mul_div_cancel_left₀ _ (ne_of_gt hN)]
lemma normalized_square_bound (hn : 0<n) (P f : Observables n) (t : Fin n→ℝ)
(hN : 0<∑x,P x*(f x)^2) (L A : ℝ)
(H : vectorNorm (fun i=>∑x,P x*(f x)^2*(spin x i-t i))≤
L*Real.sqrt (n:ℝ)*(∑x,P x*(f x)^2)+A*starSquared P f) :
vectorNorm (squareMean P f-t)/Real.sqrt (n:ℝ)≤
L+A/Real.sqrt (n:ℝ)*(1+varianceEnergy P f/(∑x,P x*(f x)^2)) := by
have hs : 0<Real.sqrt (n:ℝ):=Real.sqrt_pos.mpr (Nat.cast_pos.mpr hn)
rw [squareMean_centered P f t hN]
have he : vectorNorm (fun i=>(∑x,P x*(f x)^2*(spin x i-t i))/(∑x,P x*(f x)^2))=
vectorNorm (fun i=>∑x,P x*(f x)^2*(spin x i-t i))/(∑x,P x*(f x)^2) := by
simp only [div_eq_mul_inv,mul_comm _ (∑x,P x*(f x)^2)⁻¹]
change SKGap.vectorNorm _ = _
rw [SKGap.vectorNorm_smul,abs_of_pos (inv_pos.mpr hN)]
rfl
rw [he]
calc
_ ≤ (L*Real.sqrt (n:ℝ)*(∑x,P x*(f x)^2)+A*starSquared P f)/(∑x,P x*(f x)^2)/Real.sqrt (n:ℝ) :=
div_le_div_of_nonneg_right (div_le_div_of_nonneg_right H hN.le) hs.le
_ = _ := by unfold starSquared;field_simp [ne_of_gt hN,ne_of_gt hs]
universe u
variable {Ω : Type u} {N : Ω→ℕ} {j R B W C ρ : ℝ}
variable {J : ∀a,Interaction (N a)} {h : ∀a,Fin (N a)→ℝ}
theorem gibbs_normalized_square_mean (m : ℕ) {c r₀ ε : ℝ}
(hj : 0≤j) (hR : 0≤R) (hc : 0<c) (hr₀ : 0<r₀) (hρ : 0<ρ) (hε : 0<ε)
(hbuffer : (R+4*j)*ρ<r₀) (hm : 2<(m:ℝ)*ρ^2/4) (he : 2*(2*m:ℕ)*ε≤1)
(hB : 0≤B) (hW : 0≤W) (hC : 0≤C)
(hn : ∀a,0<N a) (hJ : ∀a,(J a).IsSymm) (hdiag : ∀a i,J a i i=0)
(hevent : ∀a,RecipeMatrixEvent j R (residualCoefficientBudget j 2 (2*m) 0) B W C (2*m+1) (2*(2*m)) (J a))
(hH : ∀a y,vectorNorm (SKGap.tapField j (J a) (h a) y)≤r₀*Real.sqrt (N a:ℝ)→∀v,
c*SKGap.vectorSqNorm v≤SKGap.quadraticForm (SKGap.fieldHessian j (J a) y (SKGap.spinVariance y)) v) :
∃r : ∀a,Fin (N a)→ℝ,
(∀a,SKGap.tapField j (J a) (h a) (r a)=0 ∧
∀y,SKGap.tapField j (J a) (h a) y=0→y=r a) ∧
∃A:ℝ,0≤A ∧ ∀a (f:Observables (N a)),
0<(∑x,fieldGibbs (J a) (h a) x*(f x)^2)→
vectorNorm (squareMean (fieldGibbs (J a) (h a)) f-SKGap.magnetization (r a))/Real.sqrt (N a:ℝ)≤
((1+(R+3*j)/c)*(R+4*j))*ρ+A/Real.sqrt (N a:ℝ)*
(1+varianceEnergy (fieldGibbs (J a) (h a)) f/(∑x,fieldGibbs (J a) (h a) x*(f x)^2)) := by
obtain ⟨r,hr,A,hA,hb⟩:=gibbs_square_mean (h:=h) m hj hR hc hr₀ hρ hε hbuffer hm he hB hW hC hn hJ hdiag hevent hH
exact ⟨r,hr,A,hA,fun a f hN=>normalized_square_bound (hn a) _ f _ hN _ A (hb a f)⟩
end SKGapCutoff.Recipe
end
end
section
noncomputable section
open scoped BigOperators
namespace SKGapCutoff.Recipe
open Primary Static
structure StableRecipeInstance (j R B W C c r₀ : ℝ) (m : ℕ) where
n : ℕ
positive : 0<n
J : Interaction n
field : Fin n→ℝ
symmetric : J.IsSymm
diagonal : ∀i,J i i=0
event : RecipeMatrixEvent j R (residualCoefficientBudget j 2 (2*m) 0) B W C (2*m+1) (2*(2*m)) J
stability : ∀y,vectorNorm (SKGap.tapField j J field y)≤r₀*Real.sqrt (n:ℝ)→∀v,
c*SKGap.vectorSqNorm v≤SKGap.quadraticForm (SKGap.fieldHessian j J y (SKGap.spinVariance y)) v
theorem uniform_stable_square_mean {j R B W C c r₀ ρ ε : ℝ} (m : ℕ)
(hj : 0≤j) (hR : 0≤R) (hc : 0<c) (hr₀ : 0<r₀) (hρ : 0<ρ) (hε : 0<ε)
(hbuffer : (R+4*j)*ρ<r₀) (hm : 2<(m:ℝ)*ρ^2/4) (he : 2*(2*m:ℕ)*ε≤1)
(hB : 0≤B) (hW : 0≤W) (hC : 0≤C) :
∃A:ℝ,0≤A ∧ ∀{n:ℕ},0<n→∀(J:Interaction n) (h:Fin n→ℝ),
J.IsSymm→(∀i,J i i=0)→
RecipeMatrixEvent j R (residualCoefficientBudget j 2 (2*m) 0) B W C (2*m+1) (2*(2*m)) J→
(∀y,vectorNorm (SKGap.tapField j J h y)≤r₀*Real.sqrt (n:ℝ)→∀v,
c*SKGap.vectorSqNorm v≤SKGap.quadraticForm (SKGap.fieldHessian j J y (SKGap.spinVariance y)) v)→
∃r:Fin n→ℝ,SKGap.tapField j J h r=0 ∧ (∀y,SKGap.tapField j J h y=0→y=r) ∧
∀f:Observables n,0<(∑x,fieldGibbs J h x*(f x)^2)→
vectorNorm (squareMean (fieldGibbs J h) f-SKGap.magnetization r)/Real.sqrt (n:ℝ)≤
((1+(R+3*j)/c)*(R+4*j))*ρ+A/Real.sqrt (n:ℝ)*
(1+varianceEnergy (fieldGibbs J h) f/(∑x,fieldGibbs J h x*(f x)^2)) := by
let Ω:=StableRecipeInstance j R B W C c r₀ m
obtain ⟨r,hr,A,hA,hb⟩:=gibbs_normalized_square_mean (Ω:=Ω) (N:=fun a=>a.n)
(J:=fun a=>a.J) (h:=fun a=>a.field) m hj hR hc hr₀ hρ hε hbuffer hm he hB hW hC
(fun a=>a.positive) (fun a=>a.symmetric) (fun a=>a.diagonal) (fun a=>a.event) (fun a=>a.stability)
refine ⟨A,hA,?_⟩
intro n hn J h hJ hd hev hst
let a:Ω:=⟨n,hn,J,h,hJ,hd,hev,hst⟩
exact ⟨r a,(hr a).1,(hr a).2,hb a⟩
lemma choose_selection_depth {ρ : ℝ} (hρ : 0<ρ) :
∃m:ℕ,∃ε:ℝ,0<ε ∧ 2<(m:ℝ)*ρ^2/4 ∧ 2*(2*m:ℕ)*ε≤1 := by
obtain ⟨m,hm⟩:=exists_nat_gt (8/ρ^2)
have hρ2 : 0<ρ^2:=sq_pos_of_pos hρ
have hm' : 2<(m:ℝ)*ρ^2/4 := by
have H:8<(m:ℝ)*ρ^2:=(div_lt_iff₀ hρ2).mp hm
linarith
refine ⟨m,1/(2*(2*m:ℕ)+1),by positivity,hm',?_⟩
have hp : 0≤(2*(2*m:ℕ):ℝ):=by positivity
rw [mul_one_div]
exact (div_le_one (by positivity)).mpr (by linarith)
end SKGapCutoff.Recipe
end
end
end OAI