Download lean/OAI/Probability/InvariantIsing/Core/FiniteFieldLawCoupling.lean from roseking/openAI-math-dataset: direct link, hf CLI and curl.
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| import OAI.Probability.InvariantIsing.Core.FiniteFieldAtomMass | |
| namespace OAI | |
| /-! Two positive finite representations of the same field law have a | |
| coupling supported on identical field values. -/ | |
| noncomputable section | |
| open MeasureTheory | |
| open scoped BigOperators | |
| namespace InvariantIsing | |
| def sameFieldCoupling {A B : Type*} [Fintype A] | |
| (γ c : A → ℝ) (δ d : B → ℝ) (a : A) (j : B) : ℝ := | |
| if c a=d j then γ a*δ j/fieldAtomMass γ c (c a) else 0 | |
| lemma sameFieldCoupling_nonneg {A B : Type*} [Fintype A] | |
| (γ c : A → ℝ) (δ d : B → ℝ) (hγ : ∀ a, 0 < γ a) (hδ : ∀ j, 0 ≤ δ j) (a : A) (j : B) : | |
| 0 ≤ sameFieldCoupling γ c δ d a j := by | |
| unfold sameFieldCoupling | |
| split_ifs | |
| · exact div_nonneg (mul_nonneg (hγ a).le (hδ j)) (fieldAtomMass_pos_at γ c hγ a).le | |
| · rfl | |
| lemma sameFieldCoupling_row {A B : Type*} [Fintype A] [Fintype B] | |
| (γ c : A → ℝ) (δ d : B → ℝ) (hγ : ∀ a, 0 < γ a) | |
| (he : ∀ x, fieldAtomMass γ c x=fieldAtomMass δ d x) (a : A) : | |
| ∑ j, sameFieldCoupling γ c δ d a j=γ a := by | |
| have hw j : sameFieldCoupling γ c δ d a j= | |
| (γ a/fieldAtomMass γ c (c a))*(if d j=c a then δ j else 0) := by | |
| unfold sameFieldCoupling | |
| by_cases hh : c a=d j | |
| · simp only [hh,eq_self,ite_true] | |
| ring | |
| · have hh' : ¬ d j=c a := Ne.symm hh | |
| simp only [hh,hh',ite_false,mul_zero] | |
| simp_rw [hw] | |
| rw [← Finset.mul_sum,show (∑ j, if d j=c a then δ j else 0)=fieldAtomMass δ d (c a) from rfl, | |
| ← he (c a)] | |
| exact div_mul_cancel₀ _ (fieldAtomMass_pos_at γ c hγ a).ne' | |
| lemma sameFieldCoupling_col {A B : Type*} [Fintype A] [Fintype B] | |
| (γ c : A → ℝ) (δ d : B → ℝ) (hδ : ∀ j, 0 < δ j) | |
| (he : ∀ x, fieldAtomMass γ c x=fieldAtomMass δ d x) (j : B) : | |
| ∑ a, sameFieldCoupling γ c δ d a j=δ j := by | |
| have hw a : sameFieldCoupling γ c δ d a j= | |
| (δ j/fieldAtomMass γ c (d j))*(if c a=d j then γ a else 0) := by | |
| unfold sameFieldCoupling | |
| by_cases hh : c a=d j | |
| · simp only [hh,eq_self,ite_true] | |
| ring | |
| · simp only [hh,ite_false,mul_zero] | |
| simp_rw [hw] | |
| rw [← Finset.mul_sum,show (∑ a, if c a=d j then γ a else 0)=fieldAtomMass γ c (d j) from rfl] | |
| apply div_mul_cancel₀ | |
| rw [he] | |
| exact (fieldAtomMass_pos_at δ d hδ j).ne' | |
| lemma sameFieldCoupling_cost {A B : Type*} [Fintype A] [Fintype B] | |
| (γ c : A → ℝ) (δ d : B → ℝ) : | |
| (∑ a, ∑ j, sameFieldCoupling γ c δ d a j* |c a-d j|)=0 := by | |
| apply Finset.sum_eq_zero | |
| intro a _ | |
| apply Finset.sum_eq_zero | |
| intro j _ | |
| unfold sameFieldCoupling | |
| split_ifs with h | |
| · simp only [h,sub_self,abs_zero,mul_zero] | |
| · exact zero_mul _ | |
| end InvariantIsing | |
| end | |
| end OAI | |