import Mathlib namespace OAI noncomputable section namespace Problem310 /-- The integer label of the half-open periodic grid cell containing a point. -/ def periodicGridKey (q x : ℝ) : ℤ := ⌊q * Int.fract x⌋ /-- Two points separated from each other in both directions around the circle cannot occupy the same cell of a periodic grid. -/ theorem periodicGridKey_ne_of_separated {q x y : ℝ} (hq : 2 ≤ q) (hlo : q⁻¹ ≤ y - x) (hhi : y - x ≤ 1 - q⁻¹) : periodicGridKey q x ≠ periodicGridKey q y := by have hqpos : 0 < q := by linarith have hi : 0 < q⁻¹ := inv_pos.mpr hqpos have hxy : x ≤ y := by linarith have hfloorle : ⌊x⌋ ≤ ⌊y⌋ := Int.floor_mono hxy have hfloorupper : ⌊y⌋ < ⌊x⌋ + 2 := by apply Int.floor_lt.mpr have hx := Int.lt_floor_add_one x push_cast linarith intro heq unfold periodicGridKey at heq have hxlo := Int.floor_le (q * Int.fract x) have hxhi := Int.lt_floor_add_one (q * Int.fract x) have hylo := Int.floor_le (q * Int.fract y) have hyhi := Int.lt_floor_add_one (q * Int.fract y) rw [← heq] at hylo hyhi have hdlo : q * (Int.fract y - Int.fract x) < 1 := by linarith have hdhi : q * (Int.fract x - Int.fract y) < 1 := by linarith have hmul : q * q⁻¹ = 1 := mul_inv_cancel₀ hqpos.ne' have hcase : ⌊y⌋ = ⌊x⌋ ∨ ⌊y⌋ = ⌊x⌋ + 1 := by omega rcases hcase with h | h · unfold Int.fract at hdlo rw [h] at hdlo have := mul_le_mul_of_nonneg_left hlo hqpos.le nlinarith · unfold Int.fract at hdhi rw [h] at hdhi push_cast at hdhi have := mul_le_mul_of_nonneg_left hhi hqpos.le nlinarith /-- The periodic label is the residue of the label on the real-line grid. -/ theorem periodicGridKey_eq_emod (q : ℕ) (hq : 0 < q) (x : ℝ) : periodicGridKey q x = ⌊(q : ℝ) * x⌋ % (q : ℤ) := by unfold periodicGridKey Int.fract rw [mul_sub] have hc : (q : ℝ) * (⌊x⌋ : ℝ) = (((q : ℤ) * ⌊x⌋ : ℤ) : ℝ) := by push_cast rfl rw [hc, Int.floor_sub_intCast, Int.emod_def] have hf := Int.natCast_mul_floor_div_cancel (R := ℝ) (Nat.ne_of_gt hq) x rw [hf] /-- Absence of a real-line grid boundary between ordered points preserves keys. The interval is open at its left end, so a center on a boundary is allowed. -/ theorem periodicGridKey_eq_of_no_crossing (q : ℕ) (hq : 0 < q) {x y : ℝ} (hxy : x ≤ y) (hcross : ∀ k : ℤ, (k : ℝ) / q ∉ Set.Ioc x y) : periodicGridKey q x = periodicGridKey q y := by have hqpos : (0 : ℝ) < q := by exact_mod_cast hq have hmono : ⌊(q : ℝ) * x⌋ ≤ ⌊(q : ℝ) * y⌋ := Int.floor_mono (mul_le_mul_of_nonneg_left hxy hqpos.le) have hfloors : ⌊(q : ℝ) * x⌋ = ⌊(q : ℝ) * y⌋ := by by_contra hne have hlt : ⌊(q : ℝ) * x⌋ + 1 ≤ ⌊(q : ℝ) * y⌋ := by omega apply hcross (⌊(q : ℝ) * x⌋ + 1) constructor · apply (lt_div_iff₀ hqpos).mpr have h := Int.lt_floor_add_one ((q : ℝ) * x) push_cast nlinarith · apply (div_le_iff₀ hqpos).mpr have hcast : ((⌊(q : ℝ) * x⌋ + 1 : ℤ) : ℝ) ≤ (⌊(q : ℝ) * y⌋ : ℝ) := by exact_mod_cast hlt have h := Int.floor_le ((q : ℝ) * y) nlinarith rw [periodicGridKey_eq_emod q hq, periodicGridKey_eq_emod q hq, hfloors] /-- Periodic cells used for a dyadic window with last index `b`. -/ def dyadicGridKey (b : ℕ) (x : ℝ) : ℤ := periodicGridKey ((2 : ℝ) ^ (b + 2)) x @[simp] theorem dyadicGridKey_add_one (b : ℕ) (x : ℝ) : dyadicGridKey b (x + 1) = dyadicGridKey b x := by simp [dyadicGridKey, periodicGridKey, Int.fract_add_one] theorem dyadicGridKey_nonneg (b : ℕ) (x : ℝ) : 0 ≤ dyadicGridKey b x := by unfold dyadicGridKey periodicGridKey exact Int.floor_nonneg.mpr (mul_nonneg (by positivity) (Int.fract_nonneg x)) theorem dyadicGridKey_lt (b : ℕ) (x : ℝ) : dyadicGridKey b x < (2 : ℤ) ^ (b + 2) := by unfold dyadicGridKey periodicGridKey apply Int.floor_lt.mpr push_cast nlinarith [Int.fract_lt_one x, pow_pos (by norm_num : (0 : ℝ) < 2) (b + 2)] /-- Fine dyadic grid labels determine all coarser labels by integer division. -/ theorem dyadicGridKey_nested {b B : ℕ} (hb : b ≤ B) (x : ℝ) : dyadicGridKey B x / (2 : ℤ) ^ (B - b) = dyadicGridKey b x := by have hp : (2 : ℝ) ^ (B + 2) = ((2 : ℕ) ^ (B - b) : ℝ) * (2 : ℝ) ^ (b + 2) := by push_cast rw [← pow_add] congr 1 omega unfold dyadicGridKey periodicGridKey rw [hp, mul_assoc] have h := Int.natCast_mul_floor_div_cancel (R := ℝ) (n := (2 : ℕ) ^ (B - b)) (by positivity) ((2 : ℝ) ^ (b + 2) * Int.fract x) simpa using h theorem dyadicGridKey_ne_of_coarse_ne {b B : ℕ} {x y : ℝ} (hb : b ≤ B) (h : dyadicGridKey b x ≠ dyadicGridKey b y) : dyadicGridKey B x ≠ dyadicGridKey B y := by intro hxy apply h rw [← dyadicGridKey_nested hb x, ← dyadicGridKey_nested hb y, hxy] private theorem half_pow_antitone : Antitone (fun n : ℕ ↦ ((2 : ℝ)⁻¹) ^ n) := pow_right_anti₀ (by norm_num) (by norm_num) private theorem grid_resolution_bound (b : ℕ) : 2 ≤ (2 : ℝ) ^ (b + 2) := by have := pow_le_pow_right₀ (by norm_num : (1 : ℝ) ≤ 2) (show 1 ≤ b + 2 by omega) simpa using this private theorem grid_width_eq (b : ℕ) : ((2 : ℝ) ^ (b + 2))⁻¹ = ((2 : ℝ)⁻¹) ^ (b + 2) := by simp only [inv_pow] /-- The center and any requested point in a window occupy different cells. -/ theorem dyadicGridKey_center_ne {a b n : ℕ} {x t : ℝ} (ha : 3 ≤ a) (han : a ≤ n) (hnb : n ≤ b) (ht : t ∈ Set.Icc (1 : ℝ) 2) : dyadicGridKey b x ≠ dyadicGridKey b (x + t * ((2 : ℝ)⁻¹) ^ n) := by apply periodicGridKey_ne_of_separated (grid_resolution_bound b) · rw [grid_width_eq] have hn := half_pow_antitone (show n ≤ b + 2 by omega) have hp : 0 ≤ ((2 : ℝ)⁻¹) ^ n := by positivity nlinarith [ht.1] · rw [grid_width_eq] have hn := half_pow_antitone (show 3 ≤ n by omega) have hb := half_pow_antitone (show 2 ≤ b + 2 by omega) norm_num at hn hb have hp : 0 ≤ ((2 : ℝ)⁻¹) ^ n := by positivity nlinarith [ht.2] /-- Different indices in a window supply different selector addresses. -/ theorem dyadicGridKey_pair_ne {a b n m : ℕ} {x t : ℝ} (ha : 3 ≤ a) (han : a ≤ n) (hnm : n < m) (hmb : m ≤ b) (ht : t ∈ Set.Icc (1 : ℝ) 2) : dyadicGridKey b (x + t * ((2 : ℝ)⁻¹) ^ m) ≠ dyadicGridKey b (x + t * ((2 : ℝ)⁻¹) ^ n) := by apply periodicGridKey_ne_of_separated (grid_resolution_bound b) · rw [grid_width_eq] have hm := half_pow_antitone (show m ≤ b + 2 by omega) have hnm' := half_pow_antitone (show n + 1 ≤ m by omega) dsimp only at hnm' rw [pow_succ] at hnm' norm_num at hnm' have hp : 0 ≤ ((2 : ℝ)⁻¹) ^ m := by positivity have hd : ((2 : ℝ)⁻¹) ^ m ≤ ((2 : ℝ)⁻¹) ^ n - ((2 : ℝ)⁻¹) ^ m := by linarith have hmultip := mul_le_mul_of_nonneg_right ht.1 (show 0 ≤ ((2 : ℝ)⁻¹) ^ n - ((2 : ℝ)⁻¹) ^ m by linarith) nlinarith · rw [grid_width_eq] have hn := half_pow_antitone (show 3 ≤ n by omega) have hb := half_pow_antitone (show 2 ≤ b + 2 by omega) norm_num at hn hb have hpn : 0 ≤ ((2 : ℝ)⁻¹) ^ n := by positivity have hpm : 0 ≤ t * ((2 : ℝ)⁻¹) ^ m := mul_nonneg (by linarith [ht.1]) (by positivity) nlinarith [ht.2] /-- The no-crossing stability condition for a later window preserves an earlier key. -/ theorem dyadicGridKey_eq_of_stable {a b n : ℕ} {x t : ℝ} (han : a ≤ n) (ht : t ∈ Set.Icc (1 : ℝ) 2) (hstable : ∀ k : ℤ, (k : ℝ) / (2 : ℝ) ^ (b + 2) ∉ Set.Ioc x (x + 2 * ((2 : ℝ)⁻¹) ^ a)) : dyadicGridKey b (x + t * ((2 : ℝ)⁻¹) ^ n) = dyadicGridKey b x := by have hp : 0 ≤ ((2 : ℝ)⁻¹) ^ n := by positivity have hp' : 0 ≤ ((2 : ℝ)⁻¹) ^ a := by positivity have hn := half_pow_antitone han have hstep : 0 ≤ t * ((2 : ℝ)⁻¹) ^ n := mul_nonneg (by linarith [ht.1]) hp have hbound : t * ((2 : ℝ)⁻¹) ^ n ≤ 2 * ((2 : ℝ)⁻¹) ^ a := by nlinarith [ht.2] have hkey := periodicGridKey_eq_of_no_crossing ((2 : ℕ) ^ (b + 2)) (by positivity) (show x ≤ x + t * ((2 : ℝ)⁻¹) ^ n by linarith) (fun k hk ↦ hstable k ⟨by simpa using hk.1, by have hk' : (k : ℝ) / (2 : ℝ) ^ (b + 2) ≤ x + t * ((2 : ℝ)⁻¹) ^ n := by simpa using hk.2 linarith⟩) simpa [dyadicGridKey] using hkey.symm /-- All the trial addresses in one dyadic window are distinct. -/ theorem dyadicGridKey_injOn_window {a b : ℕ} {x t : ℝ} (ha : 3 ≤ a) (ht : t ∈ Set.Icc (1 : ℝ) 2) : Set.InjOn (fun n : ℕ ↦ dyadicGridKey b (x + t * ((2 : ℝ)⁻¹) ^ n)) (Set.Icc a b) := by intro n hn m hm heq rcases lt_trichotomy n m with h | h | h · exact False.elim (dyadicGridKey_pair_ne ha hn.1 h hm.2 ht heq.symm) · exact h · exact False.elim (dyadicGridKey_pair_ne ha hm.1 h hn.2 ht heq) end Problem310 end end OAI