Fiber-homotopy equivalence explained

In algebraic topology, a fiber-homotopy equivalence is a homotopy equivalence between fibers of maps into a space B from spaces D and E (that is, a map between preimages that is bidirectionally invertible up to homotopy). It is a fiber-wise analog of a homotopy equivalence between spaces.

Given maps p: DB, q: EB, if ƒ: DE is a fiber-homotopy equivalence, then for any b in B the restriction

f:p-1(b)\toq-1(b)

is a homotopy equivalence. If p, q are fibrations, this is always the case for homotopy equivalences by the next proposition.

Proof of the proposition

The following proof is based on the proof of Proposition in Ch. 6, § 5 of . We write

\simB

for a homotopy over B.

We first note that it is enough to show that ƒ admits a left homotopy inverse over B. Indeed, if

gf\simB\operatorname{id}

with g over B, then g is in particular a homotopy equivalence. Thus, g also admits a left homotopy inverse h over B and then formally we have

h\simf

; that is,

fg\simB\operatorname{id}

.

Now, since ƒ is a homotopy equivalence, it has a homotopy inverse g. Since

fg\sim\operatorname{id}

, we have:

pg=qfg\simq

. Since p is a fibration, the homotopy

pg\simq

lifts to a homotopy from g to, say, g' that satisfies

pg'=q

. Thus, we can assume g is over B. Then it suffices to show gƒ, which is now over B, has a left homotopy inverse over B since that would imply that ƒ has such a left inverse.

Therefore, the proof reduces to the situation where ƒ: DD is over B via p and

f\sim\operatorname{id}D

. Let

ht

be a homotopy from ƒ to

\operatorname{id}D

. Then, since

ph0=p

and since p is a fibration, the homotopy

pht

lifts to a homotopy

kt:\operatorname{id}D\simk1

; explicitly, we have

pht=pkt

. Note also

k1

is over B.

We show

k1

is a left homotopy inverse of ƒ over B. Let

J:k1f\simh1=\operatorname{id}D

be the homotopy given as the composition of homotopies

k1f\simf=h0\sim\operatorname{id}D

. Then we can find a homotopy K from the homotopy pJ to the constant homotopy

pk1=ph1

. Since p is a fibration, we can lift K to, say, L. We can finish by going around the edge corresponding to J:

k1f=J0=L0,\simBL0,\simBL1,\simBL1,=J1=\operatorname{id}.

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