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caec230 | 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100 101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120 121 122 123 124 125 126 127 128 129 130 131 132 133 134 135 136 137 138 139 140 141 142 143 144 145 146 147 148 149 150 151 152 153 154 155 156 157 158 159 160 161 162 163 164 165 166 167 168 169 170 171 172 173 174 175 176 177 178 179 180 181 182 183 184 185 186 187 188 189 190 191 192 193 194 195 196 197 198 199 200 201 202 203 204 205 206 207 208 209 210 211 212 213 | 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
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