import Lean.Elab.Tactic.Omega import Mathlib.Algebra.GroupWithZero.Units.Basic import Mathlib.Analysis.Calculus.FDeriv.Add import Mathlib.Analysis.Calculus.FDeriv.Congr import Mathlib.Analysis.Complex.Basic import Mathlib.Analysis.SpecialFunctions.Complex.LogDeriv namespace OAI /-! # Automorphic section spaces, Laurent recurrences, and period freeness -/ section /-! Concrete holomorphic multiplier sections on the punctured complex plane. The value at zero is fixed to zero, solely to represent functions on `ℂ*` as ordinary functions `ℂ → ℂ` without introducing an extra free coefficient. No dimension, spanning, existence, or Nagata conclusion is a structure field. -/ namespace Nagata.W08 open Filter Topology /-- Holomorphic functions on `ℂ*` with the multiplier of `D(n,γ)`. The zero extension at the omitted point is part of the representation. -/ noncomputable def automorphicSections (τ : ℂ) (n : ℤ) (γ : ℂ) : Submodule ℂ (ℂ → ℂ) where carrier := {f | f 0 = 0 ∧ (∀ z, z ≠ 0 → DifferentiableAt ℂ f z) ∧ (∀ z, z ≠ 0 → f (τ * z) = γ * z ^ (-n) * f z)} zero_mem' := by refine ⟨rfl, ?_, ?_⟩ · intro z _ exact differentiableAt_const 0 · intro z _ simp add_mem' := by intro f g hf hg refine ⟨?_, ?_, ?_⟩ · change f 0 + g 0 = 0 rw [hf.1, hg.1, add_zero] · intro z hz exact (hf.2.1 z hz).add (hg.2.1 z hz) · intro z hz change f (τ * z) + g (τ * z) = γ * z ^ (-n) * (f z + g z) rw [hf.2.2 z hz, hg.2.2 z hz, mul_add] smul_mem' := by intro a f hf refine ⟨?_, ?_, ?_⟩ · change a * f 0 = 0 rw [hf.1, mul_zero] · intro z hz exact (hf.2.1 z hz).const_smul a · intro z hz change a * f (τ * z) = γ * z ^ (-n) * (a * f z) rw [hf.2.2 z hz] ac_rfl @[simp] theorem mem_automorphicSections_iff {τ γ : ℂ} {n : ℤ} {f : ℂ → ℂ} : f ∈ automorphicSections τ n γ ↔ f 0 = 0 ∧ (∀ z, z ≠ 0 → DifferentiableAt ℂ f z) ∧ (∀ z, z ≠ 0 → f (τ * z) = γ * z ^ (-n) * f z) := Iff.rfl /-- Agreement on the genuine domain `ℂ*` determines the represented section. -/ theorem automorphicSections_ext {τ γ : ℂ} {n : ℤ} (f g : automorphicSections τ n γ) (h : ∀ z, z ≠ 0 → f.val z = g.val z) : f = g := by apply Subtype.ext funext z by_cases hz : z = 0 · subst z exact f.property.1.trans g.property.1.symm · exact h z hz /-- Forget the forced zero value and restrict to the actual punctured-plane domain. -/ def sectionRestriction (τ : ℂ) (n : ℤ) (γ : ℂ) : automorphicSections τ n γ →ₗ[ℂ] ({z : ℂ // z ≠ 0} → ℂ) where toFun f z := f.val z.val map_add' _ _ := rfl map_smul' _ _ := rfl /-- The zero-extension representation adds no sections invisible on `ℂ*`. -/ theorem sectionRestriction_injective (τ : ℂ) (n : ℤ) (γ : ℂ) : Function.Injective (sectionRestriction τ n γ) := by intro f g h apply automorphicSections_ext intro z hz exact congrFun h ⟨z, hz⟩ /-- Extend the values on `ℂ*` by zero at the omitted point. -/ noncomputable def normalizeAtZero (f : ℂ → ℂ) (z : ℂ) : ℂ := if z = 0 then 0 else f z @[simp] theorem normalizeAtZero_zero (f : ℂ → ℂ) : normalizeAtZero f 0 = 0 := by simp [normalizeAtZero] @[simp] theorem normalizeAtZero_of_ne (f : ℂ → ℂ) {z : ℂ} (hz : z ≠ 0) : normalizeAtZero f z = f z := by simp [normalizeAtZero, hz] /-- Changing the value at zero changes no germ on the punctured plane. -/ theorem normalizeAtZero_eventuallyEq (f : ℂ → ℂ) {z : ℂ} (hz : z ≠ 0) : normalizeAtZero f =ᶠ[𝓝 z] f := (eventually_ne_nhds hz).mono fun point hpoint ↦ normalizeAtZero_of_ne f (z := point) hpoint /-- The zero-extension representation preserves holomorphy at every genuine point. -/ theorem normalizeAtZero_differentiableAt_iff (f : ℂ → ℂ) {z : ℂ} (hz : z ≠ 0) : DifferentiableAt ℂ (normalizeAtZero f) z ↔ DifferentiableAt ℂ f z := (normalizeAtZero_eventuallyEq f hz).differentiableAt_iff /-- Construct a concrete section from an actual holomorphic automorphic function. The assumptions state only holomorphy and the defining multiplier equation. -/ theorem normalizeAtZero_mem_automorphicSections {τ γ : ℂ} {n : ℤ} (hτ : τ ≠ 0) (f : ℂ → ℂ) (hf : ∀ z, z ≠ 0 → DifferentiableAt ℂ f z) (he : ∀ z, z ≠ 0 → f (τ * z) = γ * z ^ (-n) * f z) : normalizeAtZero f ∈ automorphicSections τ n γ := by refine ⟨normalizeAtZero_zero f, ?_, ?_⟩ · intro z hz exact (normalizeAtZero_differentiableAt_iff f hz).mpr (hf z hz) · intro z hz rw [normalizeAtZero_of_ne f (mul_ne_zero hτ hz), normalizeAtZero_of_ne f hz] exact he z hz /-- The resulting element of the genuine section space. -/ noncomputable def sectionOfFunction {τ γ : ℂ} {n : ℤ} (hτ : τ ≠ 0) (f : ℂ → ℂ) (hf : ∀ z, z ≠ 0 → DifferentiableAt ℂ f z) (he : ∀ z, z ≠ 0 → f (τ * z) = γ * z ^ (-n) * f z) : automorphicSections τ n γ := ⟨normalizeAtZero f, normalizeAtZero_mem_automorphicSections hτ f hf he⟩ @[simp] theorem sectionOfFunction_apply {τ γ : ℂ} {n : ℤ} (hτ : τ ≠ 0) (f : ℂ → ℂ) (hf : ∀ z, z ≠ 0 → DifferentiableAt ℂ f z) (he : ∀ z, z ≠ 0 → f (τ * z) = γ * z ^ (-n) * f z) {z : ℂ} (hz : z ≠ 0) : (sectionOfFunction hτ f hf he).val z = f z := normalizeAtZero_of_ne f hz end Nagata.W08 end section universe u namespace Nagata.W08 /-- The integer-valued quadratic appearing in a bi-infinite Laurent orbit. -/ def triangular (p : Int) : Int := p * (p - 1) / 2 @[simp] theorem triangular_zero : triangular 0 = 0 := by decide /-- This identity is valid also for negative `p`. -/ theorem triangular_add_one (p : Int) : triangular (p + 1) = triangular p + p := by unfold triangular have h : (p + 1) * (p + 1 - 1) = p * (p - 1) + 2 * p := by simp only [Int.add_sub_cancel, Int.add_mul, Int.one_mul, Int.mul_sub, Int.mul_one] omega rw [h] omega theorem triangular_sub_one (p : Int) : triangular (p - 1) = triangular p - (p - 1) := by have h := triangular_add_one (p - 1) have he : p - 1 + 1 = p := by omega rw [he] at h omega /-- The exact exponent, before distributing the factor `n` inside the quotient. -/ def laurentExponent (n K p : Int) : Int := p * K + n * triangular p @[simp] theorem laurentExponent_zero (n K : Int) : laurentExponent n K 0 = 0 := by simp [laurentExponent] theorem laurentExponent_add_one (n K p : Int) : laurentExponent n K (p + 1) = laurentExponent n K p + (K + n * p) := by simp only [laurentExponent, triangular_add_one, Int.add_mul, Int.one_mul, Int.mul_add] omega theorem laurentExponent_sub_one (n K p : Int) : laurentExponent n K (p - 1) = laurentExponent n K p - (K + n * (p - 1)) := by have h := laurentExponent_add_one n K (p - 1) have he : p - 1 + 1 = p := by omega rw [he] at h omega /-- A recurrence with reversible transitions is determined at every integer by its value at zero. -/ theorem biInfinite_unique {α : Type u} (step : Int → α → α) (injective_step : ∀ p x y, step p x = step p y → x = y) (a b : Int → α) (ha : ∀ p, a (p + 1) = step p (a p)) (hb : ∀ p, b (p + 1) = step p (b p)) (hzero : a 0 = b 0) : a = b := by have hnat : ∀ k : Nat, a (k : Int) = b (k : Int) := by intro k induction k with | zero => exact hzero | succ k ih => have hindex : ((k + 1 : Nat) : Int) = (k : Int) + 1 := by omega rw [hindex, ha, hb, ih] have hneg : ∀ k : Nat, a (-(k : Int)) = b (-(k : Int)) := by intro k induction k with | zero => exact hzero | succ k ih => apply injective_step (-((k + 1 : Nat) : Int)) rw [← ha, ← hb] have hindex : -((k + 1 : Nat) : Int) + 1 = -(k : Int) := by omega rw [hindex] exact ih funext p cases p with | ofNat k => exact hnat k | negSucc k => have hindex : Int.negSucc k = -((k + 1 : Nat) : Int) := by omega rw [hindex] exact hneg (k + 1) /-- The division in the triangular exponent is exact, for every integer. -/ theorem two_mul_triangular (p : Int) : 2 * triangular p = p * (p - 1) := by have heq : (fun p : Int => 2 * triangular p) = (fun p : Int => p * (p - 1)) := by apply biInfinite_unique (fun p x => x + 2 * p) · intro p x y h omega · intro p rw [triangular_add_one, Int.mul_add] · intro p simp only [Int.add_sub_cancel, Int.add_mul, Int.one_mul, Int.mul_sub, Int.mul_one] omega · decide exact congrFun heq p theorem two_dvd_mul_pred (p : Int) : (2 : Int) ∣ p * (p - 1) := ⟨triangular p, (two_mul_triangular p).symm⟩ /-- Moves `n` through the exact integer quotient in the manuscript exponent. -/ theorem laurentExponent_eq_source (n K p : Int) : laurentExponent n K p = p * K + n * p * (p - 1) / 2 := by unfold laurentExponent triangular rw [← Int.mul_ediv_assoc n (two_dvd_mul_pred p), Int.mul_assoc] end Nagata.W08 end section /-! Freeness of the source's multiplicative period action. -/ namespace Nagata.W08 /-- A complex period strictly inside the unit circle has no nontrivial integral period. -/ theorem period_zpow_eq_one {τ : ℂ} (hτ : ‖τ‖ < 1) {k : ℤ} (hk : τ ^ k = 1) : k = 0 := by have hnorm := congrArg norm hk rw [norm_zpow, norm_one] at hnorm exact (zpow_eq_one_iff_right₀ (norm_nonneg τ) (ne_of_lt hτ)).mp hnorm /-- The period acts freely on every nonzero point. -/ theorem period_zpow_mul_eq_self {τ z : ℂ} (hτ : ‖τ‖ < 1) (hz : z ≠ 0) {k : ℤ} (hk : τ ^ k * z = z) : k = 0 := by apply period_zpow_eq_one hτ exact mul_right_cancel₀ hz (hk.trans (one_mul z).symm) /-- The unit-valued form used by the genuine torus and multiplier quotients. -/ theorem unitPeriod_free (τ : ℂˣ) (hτ : ‖(τ : ℂ)‖ < 1) (k : ℤ) (hk : τ ^ k = 1) : k = 0 := by apply period_zpow_eq_one hτ simpa only [Units.val_zpow_eq_zpow_val, Units.val_one] using congrArg (fun u : ℂˣ ↦ (u : ℂ)) hk end Nagata.W08 end section /-! Global gluing across the principal-logarithm branch cut. An entire function invariant under the actual exponential deck transformations descends to a holomorphic function on all of the punctured complex plane. -/ noncomputable section namespace Nagata.W08 open Filter Topology /-- Equality of exponential images identifies values of a deck-invariant function. -/ theorem periodic_eq_of_exp_eq (F : ℂ → ℂ) (hperiod : ∀ x (k : ℤ), F (x + (k : ℂ) * (2 * (Real.pi : ℂ) * Complex.I)) = F x) {x y : ℂ} (hxy : Complex.exp x = Complex.exp y) : F x = F y := by obtain ⟨k, hk⟩ := Complex.exp_eq_exp_iff_exists_int.mp hxy rw [hk, hperiod] /-- Use any local logarithm about `z₀`; the value agrees with the principal-log formula. -/ theorem periodic_log_eq_localLog (F : ℂ → ℂ) (hperiod : ∀ x (k : ℤ), F (x + (k : ℂ) * (2 * (Real.pi : ℂ) * Complex.I)) = F x) {z z₀ : ℂ} (hz : z ≠ 0) (hz₀ : z₀ ≠ 0) : F (Complex.log z) = F (Complex.log (z / z₀) + Complex.log z₀) := by apply periodic_eq_of_exp_eq F hperiod rw [Complex.exp_log hz, Complex.exp_add, Complex.exp_log (div_ne_zero hz hz₀), Complex.exp_log hz₀, div_mul_cancel₀ _ hz₀] /-- The expression using principal log is holomorphic even at its branch cut, because locally it agrees with a holomorphic choice centered at the point. -/ theorem periodic_log_differentiableAt (F : ℂ → ℂ) (hF : Differentiable ℂ F) (hperiod : ∀ x (k : ℤ), F (x + (k : ℂ) * (2 * (Real.pi : ℂ) * Complex.I)) = F x) {z₀ : ℂ} (hz₀ : z₀ ≠ 0) : DifferentiableAt ℂ (fun z ↦ F (Complex.log z)) z₀ := by have hdiv : DifferentiableAt ℂ (fun z : ℂ ↦ z / z₀) z₀ := by simp only [div_eq_mul_inv] exact differentiableAt_id.mul_const _ have hslit : z₀ / z₀ ∈ Complex.slitPlane := by simp [div_self hz₀] have hlocal : DifferentiableAt ℂ (fun z : ℂ ↦ Complex.log (z / z₀) + Complex.log z₀) z₀ := ((Complex.differentiableAt_log hslit).comp z₀ (f := fun z : ℂ ↦ z / z₀) hdiv).add (differentiableAt_const (Complex.log z₀)) have hg := (hF (Complex.log (z₀ / z₀) + Complex.log z₀)).comp z₀ hlocal apply hg.congr_of_eventuallyEq exact (eventually_ne_nhds hz₀).mono fun z hz ↦ periodic_log_eq_localLog F hperiod hz hz₀ /-- A shift law on the exponential cover gives the actual multiplicative law on `ℂ*`. -/ theorem periodic_log_automorphy (F : ℂ → ℂ) (hperiod : ∀ x (k : ℤ), F (x + (k : ℂ) * (2 * (Real.pi : ℂ) * Complex.I)) = F x) {τ γ : ℂ} {n : ℤ} (hτ : τ ≠ 0) (hshift : ∀ x, F (x + Complex.log τ) = γ * Complex.exp (((-n : ℤ) : ℂ) * x) * F x) {z : ℂ} (hz : z ≠ 0) : F (Complex.log (τ * z)) = γ * z ^ (-n) * F (Complex.log z) := by have heq : F (Complex.log (τ * z)) = F (Complex.log z + Complex.log τ) := by apply periodic_eq_of_exp_eq F hperiod rw [Complex.exp_log (mul_ne_zero hτ hz), Complex.exp_add, Complex.exp_log hz, Complex.exp_log hτ, mul_comm] rw [heq, hshift, Complex.exp_int_mul, Complex.exp_log hz] /-- Package the descended actual function as a genuine holomorphic multiplier section. Entire holomorphy, deck invariance and the scalar shift law remain explicit inputs. -/ def automorphicSectionOfPeriodicFunction (F : ℂ → ℂ) (hF : Differentiable ℂ F) (hperiod : ∀ x (k : ℤ), F (x + (k : ℂ) * (2 * (Real.pi : ℂ) * Complex.I)) = F x) {τ γ : ℂ} {n : ℤ} (hτ : τ ≠ 0) (hshift : ∀ x, F (x + Complex.log τ) = γ * Complex.exp (((-n : ℤ) : ℂ) * x) * F x) : automorphicSections τ n γ := sectionOfFunction hτ (fun z ↦ F (Complex.log z)) (fun _ hz ↦ periodic_log_differentiableAt F hF hperiod hz) (fun _ hz ↦ periodic_log_automorphy F hperiod hτ hshift hz) /-- Every exponential-cover value is recovered exactly, independently of branch choices. -/ theorem automorphicSectionOfPeriodicFunction_exp (F : ℂ → ℂ) (hF : Differentiable ℂ F) (hperiod : ∀ x (k : ℤ), F (x + (k : ℂ) * (2 * (Real.pi : ℂ) * Complex.I)) = F x) {τ γ : ℂ} {n : ℤ} (hτ : τ ≠ 0) (hshift : ∀ x, F (x + Complex.log τ) = γ * Complex.exp (((-n : ℤ) : ℂ) * x) * F x) (x : ℂ) : (automorphicSectionOfPeriodicFunction F hF hperiod hτ hshift).val (Complex.exp x) = F x := by change normalizeAtZero (fun z ↦ F (Complex.log z)) (Complex.exp x) = F x rw [normalizeAtZero_of_ne _ (Complex.exp_ne_zero x)] apply periodic_eq_of_exp_eq F hperiod exact Complex.exp_log (Complex.exp_ne_zero x) end Nagata.W08 end end section /-! The algebraic iteration part of `lem:torus-sections`, equation `eq:laurent-recurrence`. This does not assume or establish existence of a holomorphic Laurent expansion, convergence, or the section-space dimension. -/ namespace Nagata.W08 variable {F : Type*} [CommGroupWithZero F] /-- Candidate values along one residue class. The starting coefficient can be zero. -/ def orbitValue (τ γ : F) (n K : ℤ) (c₀ : F) (p : ℤ) : F := γ ^ (-p) * τ ^ (laurentExponent n K p) * c₀ @[simp] theorem orbitValue_zero (τ γ : F) (n K : ℤ) (c₀ : F) : orbitValue τ γ n K c₀ 0 = c₀ := by simp [orbitValue] theorem orbitValue_add_one (τ γ : F) (hτ : τ ≠ 0) (hγ : γ ≠ 0) (n K : ℤ) (c₀ : F) (p : ℤ) : orbitValue τ γ n K c₀ (p + 1) = (γ⁻¹ * τ ^ (K + n * p)) * orbitValue τ γ n K c₀ p := by unfold orbitValue rw [show -(p + 1) = -1 + -p by omega, zpow_add₀ hγ, zpow_neg_one, laurentExponent_add_one, zpow_add₀ hτ] ac_rfl /-- The Laurent recurrence iterated through all integers, including negative ones. -/ theorem laurent_recurrence_all_int (τ γ : F) (hτ : τ ≠ 0) (hγ : γ ≠ 0) (n : ℤ) (c : ℤ → F) (hc : ∀ K, c (K + n) = γ⁻¹ * τ ^ K * c K) (K p : ℤ) : c (K + n * p) = c K * γ ^ (-p) * τ ^ (p * K + n * (p * (p - 1) / 2)) := by have horbit : (fun p : ℤ => c (K + n * p)) = orbitValue τ γ n K (c K) := by apply biInfinite_unique (fun p x => (γ⁻¹ * τ ^ (K + n * p)) * x) · intro p exact fun _ _ h => mul_left_cancel₀ (mul_ne_zero (inv_ne_zero hγ) (zpow_ne_zero _ hτ)) h · intro p have hindex : K + n * (p + 1) = K + n * p + n := by simp only [Int.mul_add, Int.mul_one] omega rw [hindex, hc] · exact orbitValue_add_one τ γ hτ hγ n K (c K) · simp have hvalue := congrFun horbit p simpa only [orbitValue, laurentExponent, triangular, mul_assoc, mul_comm, mul_left_comm] using hvalue /-- The formula exactly as printed in `eq:laurent-recurrence`. -/ theorem laurent_recurrence_source_formula (τ γ : F) (hτ : τ ≠ 0) (hγ : γ ≠ 0) (n : ℤ) (c : ℤ → F) (hc : ∀ K, c (K + n) = γ⁻¹ * τ ^ K * c K) (K p : ℤ) : c (K + n * p) = c K * γ ^ (-p) * τ ^ (p * K + n * p * (p - 1) / 2) := by have h := laurent_recurrence_all_int τ γ hτ hγ n c hc K p change c (K + n * p) = c K * γ ^ (-p) * τ ^ (laurentExponent n K p) at h rw [laurentExponent_eq_source] at h exact h /-- Rearrangement of the coefficient equality obtained from the functional equation. -/ theorem recurrence_of_coefficient_balance (τ γ : F) (hγ : γ ≠ 0) (n : ℤ) (c : ℤ → F) (hbalance : ∀ K, τ ^ K * c K = γ * c (K + n)) : ∀ K, c (K + n) = γ⁻¹ * τ ^ K * c K := by intro K calc c (K + n) = γ⁻¹ * (γ * c (K + n)) := (inv_mul_cancel_left₀ hγ _).symm _ = γ⁻¹ * (τ ^ K * c K) := by rw [← hbalance] _ = γ⁻¹ * τ ^ K * c K := (mul_assoc _ _ _).symm /-- The entire bi-infinite formula follows from the coefficient balance equation. -/ theorem laurent_formula_of_coefficient_balance (τ γ : F) (hτ : τ ≠ 0) (hγ : γ ≠ 0) (n : ℤ) (c : ℤ → F) (hbalance : ∀ K, τ ^ K * c K = γ * c (K + n)) (K p : ℤ) : c (K + n * p) = c K * γ ^ (-p) * τ ^ (p * K + n * p * (p - 1) / 2) := laurent_recurrence_source_formula τ γ hτ hγ n c (recurrence_of_coefficient_balance τ γ hγ n c hbalance) K p end Nagata.W08 end end OAI