Endpoint cones in a planar slit disk avoid the deleted ray
ProvedPlanarSlitDiskEndpointConesAvoidRaycrossing-consequencesgeometrypolygonal
Let be a point, let be a direction, and let . Remove from the open disk the positive ray from in direction and the point itself. The resulting slit disk is open and connected, and it contains two small endpoint cones on the two sides of the slit. More precisely, in the orthogonal chart
there are positive and for which the lower and upper wedges are contained in the slit disk.
This supplies the connected local terminal neighborhood and the two cone inclusions used by the terminal-slit-disk construction.
Preamble
import Definitions.Def_PlanarRot90 open Classical noncomputable section
Formal statement
lemma PlanarSlitDiskEndpointConesAvoidRay
(p base : EuclideanSpace ℝ (Fin 2)) (rho : ℝ)
(hrho : 0 < rho) (hbase : base ≠ 0) :
let ray : Set (EuclideanSpace ℝ (Fin 2)) :=
{q | ∃ t : ℝ, 0 < t ∧ q = p + t • base}
let slit : Set (EuclideanSpace ℝ (Fin 2)) :=
Metric.ball p rho \ (ray ∪ ({p} : Set (EuclideanSpace ℝ (Fin 2))))
let chart : EuclideanSpace ℝ (Fin 2) → EuclideanSpace ℝ (Fin 2) :=
fun z => p + z 0 • base + z 1 • PlanarRot90 base
IsOpen slit ∧ IsConnected slit ∧
∃ r K : ℝ, 0 < r ∧ 0 < K ∧
chart ''
{z | 0 < z 0 ∧ z 0 ^ 2 + z 1 ^ 2 < (r / ‖base‖) ^ 2 ∧
-K * z 0 < z 1 ∧ z 1 < 0} ⊆ slit ∧
chart ''
{z | 0 < z 0 ∧ z 0 ^ 2 + z 1 ^ 2 < (r / ‖base‖) ^ 2 ∧
0 < z 1 ∧ z 1 < K * z 0} ⊆ slit := by sorrySource