Simplicial Structures in Topology
Simplicial Structures in Topology
Simplicial Structures in Topology
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I.2 Categories 31<br />
If conditions 2. and 3. are replaced by<br />
2’. (∀ f ∈ C(A,B)) F( f ) ∈ C ′ (F(B),F(A))<br />
3’. (∀ f ∈ C(A,B))(∀g ∈ C(B,C)) F(gf)=F( f )F(g)<br />
we have a contravariant functor.<br />
A very simple example of a (covariant) functor is the forgetful functor D: Top →<br />
Set that merely “forgets” the topological space structure. Here is another example:<br />
Let (X,x0) ∈ Top ∗ be a based space and let F : Top ∗ → Set∗ be the function that<br />
takes each based space (Y,y0) <strong>in</strong>to the set [X,Y]∗ of all homotopy classes of based<br />
maps g: X → Y ; for each morphism f : Y → Z, wedef<strong>in</strong>eF( f ): [X,Y]∗ → [X,Z]∗<br />
as the function that takes any homotopy class [g] ∈ [X,Y ]∗ <strong>in</strong>to [ fg].<br />
We now give an example of contravariant functor. Given a based space (Y,y0),<br />
we def<strong>in</strong>e F : Top ∗ → Set∗ with the condition F(X,x0)=[X,Y]∗ for every (X,x0);<br />
here, for every f ∈ Top ∗((X,x0),(Z,z0)), the function F( f ) may only be def<strong>in</strong>ed<br />
as F( f )([g]) = [gf] for every based map g: X → Z; notice that, if f ∈<br />
Top ∗((X,x0),(Z,z0)), the arrow F( f ) has the opposite direction to that of f .<br />
We now look <strong>in</strong>to some less simple examples.<br />
The suspension functor<br />
Σ : Top ∗ → Top ∗<br />
is def<strong>in</strong>ed on based spaces (X,x0) as the quotient<br />
ΣX =<br />
I × X<br />
I ×{x0}∪∂I × X<br />
where ∂I is the set {0,1}. We shall write either [t,x] or t ∧ x when <strong>in</strong>dicat<strong>in</strong>g a<br />
generic element of ΣX; then,<br />
(∀ f ∈ Top ∗(X,Y))(∀t ∧ x ∈ ΣX) Σ( f )(t ∧ x)=t ∧ f (x).<br />
The base po<strong>in</strong>t of ΣX is t ∧ x0 = 0 ∧ x = 1 ∧ x.<br />
The behavior of the suspension functor is particularly <strong>in</strong>terest<strong>in</strong>g on spheres; <strong>in</strong><br />
fact, the suspension of an n-dimensional sphere is an (n + 1)-dimensional sphere.<br />
This fact will be better understood after study<strong>in</strong>g some maps, which will be useful<br />
also later on. For every n ≥ 0, let S n be the unit n-sphere (it is the boundary ∂D n+1<br />
of the unit (n + 1)-disk D n+1 ⊂ R n+1 ). Let us take the po<strong>in</strong>t e0 =(1,0,...,0) as the<br />
base po<strong>in</strong>t for both S n and D n+1 . Let us now def<strong>in</strong>e the maps<br />
cn : I × S n → D n+1 , (t,x) ↦→ (1 − t)e0 + tx,<br />
i+ : D n+1 → S n+1 � �<br />
, x ↦→ x, 1 −�x�2 �<br />
,<br />
i− : D n+1 → S n+1 � �<br />
, x ↦→ x,− 1 −�x�2 �<br />
and<br />
˙kn+1 : I × S n → S n+1<br />
�<br />
˙kn+1(t,x)=<br />
i+cn(2t,x) , 0 ≤ t ≤ 1<br />
2<br />
i−cn(2 − 2t,x) , 1<br />
2 ≤ t ≤ 1.