The equator of a unit sphere #
Removing from the unit sphere of a real inner product space E the points of a subspace K (with
an orthogonal projection) leaves a space homotopy equivalent to the unit sphere of the orthogonal
complement Kᗮ. One map is the inclusion of that sphere; the other is radial projection of the
orthogonal projection onto Kᗮ. Retracting the sphere of Kᗮ this way fixes it, and the
deformation of the complement normalizes the segment from a point to its orthogonal projection onto
Kᗮ, which never meets K.
For the line K = ℝ ∙ p through a unit vector p, the complement is the sphere minus p and
-p, and the sphere of Kᗮ is the equator. Together with the contractibility of a sphere minus
one point, this is the geometric input to the Mayer–Vietoris computation of the homology of
spheres. For a plane K in a four-dimensional space, the complement is that of a great circle in
the three-sphere, and the sphere of Kᗮ is the complementary great circle.
When E is two-dimensional, the equator is a zero-sphere, so the circle minus p and -p
consists of two open arcs: for any point x of it, the path components of x and of -x are
distinct and are the only two path components.
Main declarations #
TauCeti.sphereDiffHomotopyEquiv: the unit sphere minus the points ofKis homotopy equivalent to the unit sphere ofKᗮ, withTauCeti.coe_sphereDiffHomotopyEquiv_applyandTauCeti.coe_sphereDiffHomotopyEquiv_symm_applycomputing both maps.TauCeti.equatorHomotopyEquiv: the unit sphere minuspand-pis homotopy equivalent to the unit sphere of(ℝ ∙ p)ᗮ, withTauCeti.coe_equatorHomotopyEquiv_applyandTauCeti.coe_equatorHomotopyEquiv_symm_applycomputing both maps.TauCeti.zerothHomotopy_mk_neg_ne_of_finrank_eq_twoandTauCeti.zerothHomotopy_mk_eq_or_eq_neg_of_finrank_eq_two: in dimension two, the circle minuspand-phas exactly two path components, those ofxand of-x.
References #
This is the deformation retraction of Sⁿ ∖ {±p} onto the equator Sⁿ⁻¹ used in Hatcher,
Algebraic Topology, Section 2.2, to compute the homology of spheres.
The complement of a subspace in the unit sphere #
The unit sphere minus a subspace is homotopy equivalent to the unit sphere of its orthogonal
complement. For a subspace K of a real inner product space E with an orthogonal projection,
the points of the unit sphere of E outside K form a space homotopy equivalent to the unit
sphere of Kᗮ: radial projection of the orthogonal projection onto Kᗮ is a homotopy inverse of
the inclusion.
Equations
- TauCeti.sphereDiffHomotopyEquiv K = { toFun := TauCeti.toSphereOrthogonal✝ K, invFun := TauCeti.ofSphereOrthogonal✝ K, left_inv := ⋯, right_inv := ⋯ }
Instances For
The homotopy equivalence TauCeti.sphereDiffHomotopyEquiv is radial projection of the
orthogonal projection onto Kᗮ.
The homotopy inverse of TauCeti.sphereDiffHomotopyEquiv is the inclusion of the unit sphere
of Kᗮ.
The equator #
The sphere minus two antipodal points is homotopy equivalent to the equator. For a point
p of the unit sphere of a real inner product space E, the unit sphere minus p and -p is
homotopy equivalent to the unit sphere of the orthogonal complement (ℝ ∙ p)ᗮ: radial projection
of the orthogonal projection is a homotopy inverse of the inclusion.
Equations
Instances For
The homotopy equivalence TauCeti.equatorHomotopyEquiv is radial projection of the
orthogonal projection onto (ℝ ∙ p)ᗮ.
The homotopy inverse of TauCeti.equatorHomotopyEquiv is the inclusion of the equator.
The two arcs of a punctured circle are distinct. On the unit circle of a two-dimensional
real inner product space minus two antipodal points p and -p, a point x and its antipode
-x lie in distinct path components.
A punctured circle has no third arc. On the unit circle of a two-dimensional real inner
product space minus two antipodal points p and -p, every point lies in the path component of
x or in that of -x.