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TauCeti.Topology.CWComplex.Classical.Sphere.Basic

The CW structure on a sphere #

The unit sphere Sⁿ of a Euclidean space EuclideanSpace ℝ ι of dimension n + 1 is a finite CW complex with one 0-cell, a pole, and one n-cell attached along the constant map to it (TauCeti.sphereCWComplex). The characteristic map of the n-cell collapses the boundary of the closed unit cube closedBall (0 : Fin n → ℝ) 1 to ∞ (TauCeti.unitBallToOnePoint) and then identifies the one-point compactification of Fin n → ℝ with Sⁿ (onePointEquivSphereOfFinrankEq); the pole is the image of ∞. For n = 0 the two cells are the two points of S⁰.

References #

noncomputable def TauCeti.spherePole {ι : Type u} [Fintype ι] {n : ℕ} (h : Fintype.card ι = n + 1) :

The pole of the unit sphere Sⁿ of EuclideanSpace ℝ ι, for ι of cardinality n + 1: the 0-cell of its CW structure, onto which the boundary of the n-cell is collapsed.

Instances For
    noncomputable def TauCeti.sphereTopCellMap {ι : Type u} [Fintype ι] {n : ℕ} (h : Fintype.card ι = n + 1) :

    The characteristic map of the top cell of the unit sphere Sⁿ of EuclideanSpace ℝ ι, for ι of cardinality n + 1: it maps the open unit cube of Fin n → ℝ bijectively onto the complement of TauCeti.spherePole h and collapses the boundary of the cube to the pole.

    Instances For
      @[simp]
      theorem TauCeti.sphereTopCellMap_apply {ι : Type u} [Fintype ι] {n : ℕ} (h : Fintype.card ι = n + 1) (x : Fin n → ℝ) :

      The characteristic map of the top cell of Sⁿ is the boundary collapse TauCeti.unitBallToOnePoint followed by onePointEquivSphereOfFinrankEq.

      On Sⁿ, the inverse of the characteristic map of the top cell is the inverse of onePointEquivSphereOfFinrankEq followed by the inverse of TauCeti.unitBallToOnePoint.

      theorem TauCeti.sphereTopCellMap_mem_sphere {ι : Type u} [Fintype ι] {n : ℕ} (h : Fintype.card ι = n + 1) (x : Fin n → ℝ) :
      @[simp]
      theorem TauCeti.sphereTopCellMap_apply_of_norm_eq_one {ι : Type u} [Fintype ι] {n : ℕ} (h : Fintype.card ι = n + 1) {x : Fin n → ℝ} (hx : ‖x‖ = 1) :

      The characteristic map of the top cell collapses the boundary of the cube to the pole.

      The characteristic map of the top cell of Sⁿ is continuous on the closed unit ball, as a CW characteristic map must be.

      The inverse of the characteristic map of the top cell of Sⁿ is continuous on the open cell Sⁿ \ {pole}.

      @[instance_reducible]
      noncomputable def TauCeti.sphereCWComplex {ι : Type u} [Fintype ι] {n : ℕ} (h : Fintype.card ι = n + 1) :

      The CW structure on the unit sphere Sⁿ of EuclideanSpace ℝ ι, for ι of cardinality n + 1: one 0-cell, the pole TauCeti.spherePole h, and one n-cell with characteristic map TauCeti.sphereTopCellMap h.

      Instances For

        The CW structure on Sⁿ is finite.

        theorem TauCeti.nat_card_cell_sphereCWComplex {ι : Type u} [Fintype ι] {n : ℕ} (h : Fintype.card ι = n + 1) (m : ℕ) :

        The CW structure on Sⁿ has one cell in dimension 0 and one in dimension n (two 0-cells when n = 0).

        theorem TauCeti.isEmpty_cell_sphereCWComplex {ι : Type u} [Fintype ι] {n : ℕ} (h : Fintype.card ι = n + 1) {m : ℕ} (hm : n + 1 ≤ m) :

        The CW structure on Sⁿ has no cells of dimension greater than n.

        theorem TauCeti.skeletonLT_sphereCWComplex {ι : Type u} [Fintype ι] {n : ℕ} (h : Fintype.card ι = n + 1) {k : ℕ∞} (hk : 1 ≤ k) (hkn : k ≤ ↑n) :

        For 1 ≤ k ≤ n, skeletonLT k of the CW structure on Sⁿ, the (k - 1)-skeleton (the union of the cells of dimension less than k), is the pole.

        The unit sphere of a finite-dimensional real normed space has finite CW type: it is homeomorphic to the unit sphere of EuclideanSpace ℝ (ULift (Fin (n + 1))) for n + 1 the dimension, or empty in dimension zero.

        The one-point compactification of a finite-dimensional real vector space V has finite CW type: it is homeomorphic to the unit sphere of dimension dim V. In particular the Riemann sphere OnePoint ℂ has finite CW type.