openAI-math-dataset / lean /OAI /Probability /InvariantIsing /Magnetic /MagneticConstrainedVariationalUpper.lean
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import OAI.Probability.InvariantIsing.Magnetic.MagneticConstrainedUpper
import OAI.Probability.InvariantIsing.Core.FiniteVariationalBounds
namespace OAI
/-! The finite-spectrum pressure upper bound after taking the path infimum,
under Haar and Gaussian concentration hypotheses. -/
noncomputable section
open MeasureTheory ProbabilityTheory IsingPerceptron Set Filter
open scoped BigOperators Topology
namespace InvariantIsing
theorem finiteSpectrum_magneticPressure_variational_upper
(hhaar : HaarConcentrationInput) (hgauss : GaussianLipschitzVarianceInput)
(N : ℕ → ℕ) (hN : ∀ k, 3 ≤ N k) (hNlim : Tendsto N atTop atTop) (m : ℕ)
(μ : (k : ℕ) → Measure (SpecialOrthogonal (N k))) [∀ k, IsProbabilityMeasure (μ k)]
(hμinv : ∀ k, (μ k).IsMulLeftInvariant)
(eig : (k : ℕ) → Fin (N k) → ℝ)
(K : ℝ) (hK : 0 < K) (heig : ∀ k i, |eig k i| ≤ K)
(I : (k : ℕ) → Fin m → Finset (Fin (N k)))
(hdis : ∀ k, Set.PairwiseDisjoint (Set.univ : Set (Fin m)) (I k))
(hcover : ∀ k, Finset.univ.biUnion (I k) = Finset.univ)
(lam : Fin m → ℝ) (hlam : ∀ k a i, i ∈ I k a → eig k i = lam a)
(ρ : Fin m → ℝ) (hρpos : ∀ a, 0 < ρ a) (hρsum : ∑ a, ρ a = 1)
(hρ : Tendsto (fun k a => ((I k a).card : ℝ) / N k) atTop (𝓝 ρ))
{A : Type*} [Fintype A] [DecidableEq A]
(group : ∀ k, Fin (N k) → A) (count : ℕ → A → ℕ)
(hcount : ∀ k a, count k a ≤ spinGroupSize (group k) a)
(γ mag : A → ℝ) (hγ : ∀ a, 0 ≤ γ a) (hγsum : ∑ a, γ a=1)
(hmag : ∀ a, |mag a|<1)
(hc : ∀ k a, (count k a : ℝ)=spinGroupSize (group k) a*((1+mag a)/2))
(hgroup : ∀ k a, (spinGroupSize (group k) a : ℝ)=N k*γ a) :
∀ ε : ℝ, 0 < ε → ∀ᶠ k in atTop,
(∫ U : SpecialOrthogonal (N k),
restrictedRotatedPressure (spinGroupSlice (group k) (count k)) (eig k) (specialRotation U) (fun _ => 0) ∂μ k) ≤
(magneticVariationalFunctional (finiteR ρ lam hρpos hρsum) γ mag).toReal + ε := by
intro ε hε
obtain ⟨p, S, hS, hp⟩ := exists_finiteMagneticEntropy_trial
ρ lam hρpos hρsum γ mag hγ hγsum (fun a => (hmag a).le) (half_pos hε)
have hup := finiteSpectrum_magneticPressure_upper hhaar hgauss N hN hNlim m μ hμinv
eig K hK heig I hdis hcover lam hlam ρ hρpos hρsum hρ group count hcount γ mag hmag hc hgroup p S hS.le (ε / 2) (half_pos hε)
filter_upwards [hup] with k hk
linarith
end InvariantIsing
end
end OAI