import OAI.Probability.InvariantIsing.Fields.FieldProductSpinAveraging import OAI.Probability.InvariantIsing.Fields.FieldCanonicalVectorMoments namespace OAI /-! The actual averaged constrained terminal loss, with constants independent of the number of Gaussian steps. -/ noncomputable section open MeasureTheory ProbabilityTheory open scoped BigOperators namespace InvariantIsing lemma magnetic_projection_distance_mean {N : ℕ} {A : Type*} [Fintype A] [DecidableEq A] (group : Fin N → A) (k : A → ℕ) (hk : ∀ a, k a ≤ spinGroupSize group a) (m : A → ℝ) (hm : ∀ a, |m a| < 1) (hcount : ∀ a, (k a : ℝ) = (spinGroupSize group a : ℝ) * ((1 + m a) / 2)) (h : FieldStep) : (∫ z, fieldProjectionDistance (spinGroupProjection group k hk) z ∂fieldCanonicalVectorLaw N h (fun i => magneticBias h (m (group i)))) ≤ ∑ a, Real.sqrt (spinGroupSize group a) := by have he := field_product_spin_average (fun i : Fin N => fieldCanonicalEndpointLaw h (magneticBias h (m (group i)))) (fun σ => (hammingDist σ (spinGroupProjection group k hk σ) : ℝ)) simp only [← fieldCanonicalSpinLaw_endpoint] at he exact he.trans_le (magneticCanonical_projection_distance group k hk m hm hcount h) theorem magnetic_block_terminal_loss {N : ℕ} {A : Type*} [Fintype A] [DecidableEq A] (group : Fin N → A) (k : A → ℕ) (hk : ∀ a, k a ≤ spinGroupSize group a) (m : A → ℝ) (hm : ∀ a, |m a| < 1) (hcount : ∀ a, (k a : ℝ) = (spinGroupSize group a : ℝ) * ((1 + m a) / 2)) (h : FieldStep) {B H ε t : ℝ} (hB : ∀ i, |magneticBias h (m (group i))| ≤ B) (hH : h.height (Fin.last h.depth) ≤ H) (hε : 0 < ε) (ht : 0 ≤ t) : (∫ z, (∑ i, Real.log (Real.cosh (z i))) - restrictedFieldTerminal (spinGroupSlice group k) z ∂fieldCanonicalVectorLaw N h (fun i => magneticBias h (m (group i)))) ≤ ε * (N * (2 * Real.exp (2 * B + 4 * H))) + (ε⁻¹ + t) * (∑ a, Real.sqrt (spinGroupSize group a)) + N * Real.log (1 + Real.exp (-t)) := by have hl := field_projection_mean_loss (spinGroupSlice group k) (spinGroupSlice_nonempty group k hk) (spinGroupProjection group k hk) (spinGroupProjection_mem group k hk) (fieldCanonicalVectorLaw N h (fun i => magneticBias h (m (group i)))) (fieldCanonicalVectorLaw_square_integrable h (fun i => magneticBias h (m (group i)))) hε t have hM := fieldCanonicalVectorLaw_second_moment h (fun i => magneticBias h (m (group i))) hB hH have hD := magnetic_projection_distance_mean group k hk m hm hcount h exact hl.trans (add_le_add (add_le_add (mul_le_mul_of_nonneg_left hM hε.le) (mul_le_mul_of_nonneg_left hD (by positivity))) le_rfl) lemma sum_sqrt_spinGroupSize_le {N : ℕ} {A : Type*} [Fintype A] [DecidableEq A] (group : Fin N → A) : (∑ a, Real.sqrt (spinGroupSize group a)) ≤ Fintype.card A * Real.sqrt N := by calc _ ≤ ∑ _a : A, Real.sqrt (N : ℝ) := by apply Finset.sum_le_sum intro a _ apply Real.sqrt_le_sqrt exact_mod_cast (show spinGroupSize group a ≤ N from by simpa only [spinGroupSize, Finset.card_univ, Fintype.card_fin] using Finset.card_filter_le (s := (Finset.univ : Finset (Fin N))) (fun i => group i = a)) _ = _ := by simp theorem magnetic_block_terminal_loss_size {N : ℕ} {A : Type*} [Fintype A] [DecidableEq A] (group : Fin N → A) (k : A → ℕ) (hk : ∀ a, k a ≤ spinGroupSize group a) (m : A → ℝ) (hm : ∀ a, |m a| < 1) (hcount : ∀ a, (k a : ℝ) = (spinGroupSize group a : ℝ) * ((1 + m a) / 2)) (h : FieldStep) {B H ε t : ℝ} (hB : ∀ i, |magneticBias h (m (group i))| ≤ B) (hH : h.height (Fin.last h.depth) ≤ H) (hε : 0 < ε) (ht : 0 ≤ t) : (∫ z, (∑ i, Real.log (Real.cosh (z i))) - restrictedFieldTerminal (spinGroupSlice group k) z ∂fieldCanonicalVectorLaw N h (fun i => magneticBias h (m (group i)))) ≤ ε * (N * (2 * Real.exp (2 * B + 4 * H))) + (ε⁻¹ + t) * (Fintype.card A * Real.sqrt N) + N * Real.log (1 + Real.exp (-t)) := (magnetic_block_terminal_loss group k hk m hm hcount h hB hH hε ht).trans (add_le_add (add_le_add le_rfl (mul_le_mul_of_nonneg_left (sum_sqrt_spinGroupSize_le group) (by positivity))) le_rfl) end InvariantIsing end end OAI