module Homotopy.Space.Sphere where
The -1 and 0 spheres🔗
In classical topology, the topological space is typically defined as the subspace of consisting of all points at unit distance from the origin. We see from this definition that the is the discrete two point space and that the sphere is the empty subspace We will recycle existing types and define:
S⁻¹ : Type S⁻¹ = ⊥ S⁰ : Type S⁰ = Bool
We note that S⁰
may be identified with
Susp S⁻¹
. Since the pattern matching checker can prove that
merid x i
is impossible when x : ⊥
, the case
for this constructor does not need to be written, this makes the proof
look rather tautologous.
open is-iso SuspS⁻¹≃S⁰ : Susp S⁻¹ ≡ S⁰ SuspS⁻¹≃S⁰ = ua (SuspS⁻¹→S⁰ , is-iso→is-equiv iso-pf) where SuspS⁻¹→S⁰ : Susp S⁻¹ → S⁰ SuspS⁻¹→S⁰ N = true SuspS⁻¹→S⁰ S = false S⁰→SuspS⁻¹ : S⁰ → Susp S⁻¹ S⁰→SuspS⁻¹ true = N S⁰→SuspS⁻¹ false = S iso-pf : is-iso SuspS⁻¹→S⁰ iso-pf .inv = S⁰→SuspS⁻¹ iso-pf .rinv false = refl iso-pf .rinv true = refl iso-pf .linv N = refl iso-pf .linv S = refl
n-Spheres🔗
The spheres of higher dimension can be defined inductively: that is, suspending the constructs the
The spheres are essentially indexed by the natural numbers, except that we want to start at instead of To remind ourselves of this, we name our spheres with a superscript
Sⁿ⁻¹ : Nat → Type Sⁿ⁻¹ zero = S⁻¹ Sⁿ⁻¹ (suc n) = Susp (Sⁿ⁻¹ n)
A slightly less trivial example of definitions lining up is the
verification that Sⁿ⁻¹ 2
is equivalent to our previous
definition of S¹
:
SuspS⁰≡S¹ : Sⁿ⁻¹ 2 ≡ S¹ SuspS⁰≡S¹ = ua (SuspS⁰→S¹ , is-iso→is-equiv iso-pf) where
In Sⁿ⁻¹ 2
, we have two point constructors joined by two
paths, while in S¹
we have a single point constructor and a
loop. Geometrically, we can picture morphing Sⁿ⁻¹ 2
into
S¹
by squashing one of the meridians down to a point, thus
bringing N
and S
together. This intuition
leads to a definition:
SuspS⁰→S¹ : Sⁿ⁻¹ 2 → S¹ SuspS⁰→S¹ N = base SuspS⁰→S¹ S = base SuspS⁰→S¹ (merid N i) = base SuspS⁰→S¹ (merid S i) = loop i
In the other direction, we send base
to N
,
and then need to send loop
to some path N ≡ N
.
Since this map should define an equivalence, we make it such that loop
wraps around the space Sⁿ 2
by way of traversing both
meridians.
S¹→SuspS⁰ : S¹ → Sⁿ⁻¹ 2 S¹→SuspS⁰ base = N S¹→SuspS⁰ (loop i) = (merid S ∙ sym (merid N)) i
We then verify that these maps are inverse equivalences. One of the
steps involves a slightly tricky hcomp
, although this can
be avoided by working with transports instead of dependent paths, and
then by using lemmas on transport in pathspaces.
iso-pf : is-iso SuspS⁰→S¹ iso-pf .inv = S¹→SuspS⁰ iso-pf .rinv base = refl iso-pf .rinv (loop i) = ap (λ p → p i) (ap SuspS⁰→S¹ (merid S ∙ sym (merid N)) ≡⟨ ap-∙ SuspS⁰→S¹ (merid S) (sym (merid N))⟩≡ loop ∙ refl ≡⟨ ∙-idr _ ⟩≡ loop ∎) iso-pf .linv N = refl iso-pf .linv S = merid N iso-pf .linv (merid N i) j = merid N (i ∧ j) iso-pf .linv (merid S i) j = hcomp (∂ i ∨ ∂ j) λ where k (k = i0) → merid S i k (i = i0) → N k (i = i1) → merid N (j ∨ ~ k) k (j = i0) → ∙-filler (merid S) (sym (merid N)) k i k (j = i1) → merid S i