OAI/Analysis/SignedDisk/DiskGeometry1.lean
22 declarations, 0 contain sorry, 0 declared as axioms
- theorem
OAI.SignedDisk.DiskGeometry.monotone_increment_intervalline 19Source documentation
Cancellation of translated monotone integrals on a finite interval.
theorem monotone_increment_interval {G : ℝ → ℝ} (hG : Monotone G) {C v : ℝ} (h0 : ∀ x, 0 ≤ G x) (hC : ∀ x, G x ≤ C) (hv : 0 ≤ v) (a b : ℝ) : (∫ l in a..b, (G (l + v) - G (l - v))) ≤ 2 * v * C := by … - theorem
OAI.SignedDisk.DiskGeometry.monotone_increment_integrableline 42 - theorem
OAI.SignedDisk.DiskGeometry.monotone_jump_window_measureline 65Source documentation
The permitted jump times have uniformly bounded length, independent of the size of the original positive measure. Only its truncated distribution is used.
theorem monotone_jump_window_measure {H : ℝ → ℝ} (hH : Monotone H) (hH0 : ∀ l, 0 ≤ H l) {T U v : ℝ} (hT : 0 ≤ T) (hU : 0 < U) (hv : 0 ≤ v) : volume {l | H (l - v) ≤ T ∧ U ≤ H (l + v) - H (l - v)} ≤ ENNReal.ofReal (2 * v * (1 + T / U)) := by … - theorem
OAI.SignedDisk.DiskGeometry.volume_le_radial_sectionsline 98Source documentation
A polar-coordinate area bound from uniform lengths of radial sections.
theorem volume_le_radial_sections {s : Set ℂ} (hs : MeasurableSet s) (z : ℂ) {R : ℝ} (hR : 0 ≤ R) {B : ℝ≥0∞} (hbound : ∀ x ∈ s, ‖x - z‖ ≤ R) (hsections : ∀ θ : ℝ, volume {r : ℝ | 0 < r ∧ z + (r : ℂ) * ((Real.cos θ : ℂ) + (Real.sin θ : ℂ) * Complex.I) ∈ s} ≤ B) : volume s ≤ ENNReal.ofReal (2 * Real.pi * R) * B := by … - def
OAI.SignedDisk.DiskGeometry.tangentMassline 162Source documentation
Mass in the increasing family of tangent disks, away from its tangency cap.
def tangentMass (S : Measure ℂ) (ρ : ℝ) (z θ : ℂ) (L : ℝ) : ℝ := …
- theorem
OAI.SignedDisk.DiskGeometry.tangentMass_nonnegline 165 - theorem
OAI.SignedDisk.DiskGeometry.tangentMass_monoline 168 - theorem
OAI.SignedDisk.DiskGeometry.measurable_tangentMassline 178 - def
OAI.SignedDisk.DiskGeometry.rayConditionline 190Source documentation
The measurable condition whose planar cost is bounded by the ray-length estimate.
def rayCondition (S : Measure ℂ) (ρ T U v : ℝ) (x z : ℂ) : Prop := …
- theorem
OAI.SignedDisk.DiskGeometry.measurableSet_rayConditionline 196 - theorem
OAI.SignedDisk.DiskGeometry.volume_rayConditionline 207Source documentation
Full two-dimensional ray-condition estimate, independent of the chosen radius.
theorem volume_rayCondition (S : Measure ℂ) [IsFiniteMeasure S] (ρ : ℝ) {T U v : ℝ} (hT : 0 ≤ T) (hU : 0 < U) (hv : 0 ≤ v) (z : ℂ) : volume {x : ℂ | rayCondition S ρ T U v x z} ≤ ENNReal.ofReal (6 * Real.pi) * ENNReal.ofReal (2 * v * (1 + T / U)) := by …Mentions: OAI.SignedDisk.DiskGeometry.rayCondition
- def
OAI.SignedDisk.DiskGeometry.thinShellline 239 - theorem
OAI.SignedDisk.DiskGeometry.measurableSet_thinShellline 241 - theorem
OAI.SignedDisk.DiskGeometry.shell_center_boundsline 244 - theorem
OAI.SignedDisk.DiskGeometry.shell_pair_closeline 252 - theorem
OAI.SignedDisk.DiskGeometry.shell_subset_tangent_differenceline 263Source documentation
Every distant point of the thin shell crosses the tangent disks in the short window.
theorem shell_subset_tangent_difference {z θ : ℂ} (hθ : ‖θ‖ = 1) {l ρ δ : ℝ} (hl : 1 / 2 ≤ l) (hl3 : l ≤ 3) (hρ : 0 < ρ) (hρ1 : ρ ≤ 1) (hδ : 0 < δ) (hδρ : δ ≤ ρ ^ 2 / 1600) : {y : ℂ | ρ ≤ ‖y - z‖ ∧ |‖y - (z + l • θ)‖ - l| ≤ 2 * δ} ⊆ ({y : ℂ | ρ ≤ ‖y - z‖} ∩ Metric.ball (z + (l + 200 * δ / ρ ^ 2) • θ) (l + 200 * δ / ρ ^ 2)) \ ({y : ℂ | ρ ≤ ‖y - z‖} ∩ Metric.ball (z + (l - 200 * δ / ρ ^ 2) • θ) (l - 200 * δ / ρ ^ 2)) := by … - theorem
OAI.SignedDisk.DiskGeometry.shell_mass_le_jumpline 295Source documentation
The shell mass away from a cap is bounded by the one-dimensional tangent-mass jump.
theorem shell_mass_le_jump (S : Measure ℂ) [IsFiniteMeasure S] {x z : ℂ} {r ρ δ : ℝ} (hr : r ∈ Icc (1 : ℝ) 2) (hρ : 0 < ρ) (hρ1 : ρ ≤ 1) (hδ : 0 < δ) (hδρ : δ ≤ ρ ^ 2 / 1600) (hz : z ∈ thinShell x r δ) : (S (thinShell x r δ \ Metric.ball z ρ)).toReal ≤ tangentMass S ρ z (‖x - z‖⁻¹ • (x - z)) (‖x - z‖ + 200 * δ / ρ ^ 2) - tangentMass S ρ z (‖x - z‖⁻¹ • (x - z)) (‖x - z‖ - 200 * δ / ρ ^ 2) := by …Mentions: OAI.SignedDisk.DiskGeometry.thinShell, OAI.SignedDisk.DiskGeometry.tangentMass
- theorem
OAI.SignedDisk.DiskGeometry.earlier_mass_le_interiorline 341Source documentation
The earlier tangent-disk mass is controlled by the concentric interior mass.
theorem earlier_mass_le_interior (S : Measure ℂ) [IsFiniteMeasure S] {x z : ℂ} {r ρ δ : ℝ} (hr : r ∈ Icc (1 : ℝ) 2) (hρ : 0 < ρ) (hρ1 : ρ ≤ 1) (hδ : 0 < δ) (hδρ : δ ≤ ρ ^ 2 / 1600) (hz : z ∈ thinShell x r δ) : tangentMass S ρ z (‖x - z‖⁻¹ • (x - z)) (‖x - z‖ - 200 * δ / ρ ^ 2) ≤ (S (Metric.ball x (r - δ))).toReal := by …Mentions: OAI.SignedDisk.DiskGeometry.thinShell, OAI.SignedDisk.DiskGeometry.tangentMass
- theorem
OAI.SignedDisk.DiskGeometry.volume_interval_fibersline 372Source documentation
Area of a strip with continuously moving interval fibers.
theorem volume_interval_fibers (c : ℝ → ℝ) (hc : Continuous c) (lo hi w : ℝ) : volume {p : ℝ × ℝ | p.2 ∈ Icc lo hi ∧ p.1 ∈ Icc (c p.2 - w) (c p.2 + w)} = ENNReal.ofReal (hi - lo) * ENNReal.ofReal (2 * w) := by … - theorem
OAI.SignedDisk.DiskGeometry.volume_affine_stripline 400Source documentation
A nonvertical affine strip cut off in the second coordinate.
theorem volume_affine_strip {a : ℝ} (ha : a ≠ 0) (b c d R w : ℝ) : volume {p : ℝ × ℝ | |p.2 - d| ≤ R ∧ |a * p.1 + b * p.2 + c| ≤ w} = ENNReal.ofReal (2 * R) * ENNReal.ofReal (2 * (w / |a|)) := by … - theorem
OAI.SignedDisk.DiskGeometry.complex_coordinate_separationline 421Source documentation
At least one coordinate sees half the Euclidean separation.
theorem complex_coordinate_separation {z : ℂ} {ρ : ℝ} (hz : ρ ≤ ‖z‖) : ρ / 2 ≤ |z.re| ∨ ρ / 2 ≤ |z.im| := by … - theorem
OAI.SignedDisk.DiskGeometry.volume_two_point_stripline 430Source documentation
The centers of two separated points lying on an almost common circle form an affine strip of small area. No selected radius occurs here.
theorem volume_two_point_strip {y z : ℂ} {ρ δ : ℝ} (hρ : 0 < ρ) (hδ : 0 ≤ δ) (hyz : ρ ≤ ‖y - z‖) : volume {x : ℂ | ‖x - z‖ ≤ 3 ∧ |‖x - y‖ ^ 2 - ‖x - z‖ ^ 2| ≤ 13 * δ} ≤ ENNReal.ofReal (156 * δ / ρ) := by …