The Mayer–Vietoris recursive step for sphere homology #
For n ≥ 1 we prove Hₙ₊₁(Sⁿ⁺¹; ℤ) ≅ Hₙ(Sⁿ; ℤ) (sphereTopHomologyStepMV),
the recursive step of SphereSuspensionTower.
Cover Sⁿ⁺¹ by the two punctured spheres U = Sⁿ⁺¹ \ {north} and
V = Sⁿ⁺¹ \ {south}. Both are contractible (stereographic projection), so their
positive homology vanishes, and the Mayer–Vietoris connecting isomorphism
(mvHomologyIsoSucc) gives Hₙ₊₁(Sⁿ⁺¹) ≅ Hₙ(U ∩ V). The intersection
U ∩ V is the equatorial band, homotopy equivalent to Sⁿ; the subspace bridge
(subspaceHomologyIsoℤ) and homotopy invariance then identify its homology with
Hₙ(Sⁿ).
The north pole of Sⁿ⁺¹ as a unit vector e₀.
Equations
- SphereOddDegree.northVec n = PiLp.single 2 0 1
Instances For
The north pole of Sⁿ⁺¹.
Equations
Instances For
The south pole of Sⁿ⁺¹, the antipode of the north pole.
Equations
Instances For
The upper punctured sphere Sⁿ⁺¹ \ {north}.
Equations
Instances For
The lower punctured sphere Sⁿ⁺¹ \ {south}.
Equations
Instances For
The equatorial band Sⁿ⁺¹ \ {north, south}.
Equations
Instances For
Contractibility of the punctured spheres #
The equatorial band is homotopy equivalent to Sⁿ #
Construction of the band ≃ Sⁿ homotopy equivalence #
The equatorial-projection map underlying band → Sⁿ: drop coordinate 0 and
normalize.
Equations
- SphereOddDegree.fFun n x = (WithLp.equiv 2 (Fin (n + 1) → ℝ)).symm fun (i : Fin (n + 1)) => (↑x).ofLp i.succ / √(SphereOddDegree.eqNormSq n x)
Instances For
The continuous map band → Sⁿ.
Equations
- SphereOddDegree.bandToSphere n = { toFun := fun (x : ↑(SphereOddDegree.sphereBand n)) => ⟨SphereOddDegree.fFun n ↑x, ⋯⟩, continuous_toFun := ⋯ }
Instances For
The inclusion map underlying Sⁿ → band: prepend a 0 coordinate.
Equations
Instances For
The continuous map Sⁿ → band.
Equations
- SphereOddDegree.sphereToBand n = { toFun := fun (y : SphereOddDegree.Sphere n) => ⟨⟨SphereOddDegree.gFun n y, ⋯⟩, ⋯⟩, continuous_toFun := ⋯ }
Instances For
The straight-line-on-the-sphere homotopy from sphereToBand ∘ bandToSphere to the
identity of the band.
Equations
- SphereOddDegree.bandHomotopyFun n p = (1 - ↑p.1) • ↑↑((SphereOddDegree.sphereToBand n) ((SphereOddDegree.bandToSphere n) p.2)) + ↑p.1 • ↑↑p.2
Instances For
The homotopy sphereToBand ∘ bandToSphere ≃ id.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The equatorial band Sⁿ⁺¹ \ {north, south} is homotopy equivalent to Sⁿ.
Equations
- SphereOddDegree.sphereBandHomotopyEquiv n = { toFun := SphereOddDegree.bandToSphere n, invFun := SphereOddDegree.sphereToBand n, left_inv := ⋯, right_inv := ⋯ }
Instances For
Assembly of the Mayer–Vietoris step #
The categorical space Sⁿ⁺¹ realized as a TopCat from the library model.
Equations
- SphereOddDegree.sphereSpace n = ↧(SphereOddDegree.Sphere (n + 1))
Instances For
The upper punctured sphere as an open set of Sⁿ⁺¹.
Equations
- SphereOddDegree.upperOpens n = { carrier := SphereOddDegree.upperPunctured n, is_open' := ⋯ }
Instances For
The lower punctured sphere as an open set of Sⁿ⁺¹.
Equations
- SphereOddDegree.lowerOpens n = { carrier := SphereOddDegree.lowerPunctured n, is_open' := ⋯ }
Instances For
The integral homology of the band is isomorphic to Hₙ(Sⁿ; ℤ), via the
subspace bridge and homotopy invariance.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The Mayer–Vietoris recursive step. For n ≥ 1,
Hₙ₊₁(Sⁿ⁺¹; ℤ) ≅ Hₙ(Sⁿ; ℤ).
Equations
- One or more equations did not get rendered due to their size.