nLab
homotopy coequalizer

Contents

Context

Limits and colimits

(,1)(\infty,1)-Category theory

Contents

Idea

Homotopy coequalizers are a special case of homotopy colimits, when the indexing diagram is the walking parallel pair, consisting of a pair of parallel morphisms, i.e., two objects, 0 and 1, and exactly two nonidentity morphisms, both of the form 010\to 1.

Homotopy coequalizers can be defined in any relative category, just like homotopy colimits, but practical computations are typically carried out in presence of additional structures such as model structures.

Computation

In any model category, the homotopy coequalizer of a pair of arrows f,g:ABf,g\colon A\to B can be computed as follows. First, if AA is not cofibrant and the model category is not left proper, construct a cofibrant replacement q:QAAq\colon QA\to A and replace (f,g)(f,g) with (fq,gq)(f q,g q).

Assume now that AA is cofibrant or the model category is left proper.

In the special case when the map

[f,g]:AAB[f,g]\colon A\sqcup A\to B

happens to be a cofibration, we can compute the ordinary coequalizer of ff and gg, which is a homotopy coequalizer.

In the general case, factor the codiagonal map :AAA\nabla\colon A\sqcup A\to A as a cofibration AACAA\sqcup A\to C A followed by a weak equivalence CAACA\to A, then compute the (ordinary) pushout of

CAAAB.CA\leftarrow A\sqcup A \to B.

This is the homotopy coequalizer of ff and gg.

Examples

In simplicial sets with simplicial weak equivalences, the homotopy coequalizer of f,g:ABf,g\colon A\to B can be computed as the pushout

Δ 1×A AAB.\Delta^1\times A\sqcup_{A\sqcup A} B.

The same formula works for topological spaces with weak homotopy equivalences, using Δ=[0,1]\Delta=[0,1].

For chain complexes with quasi-isomorphisms, the homotopy coequalizer can be computed (expanding the analogous formula with CA=NZ[Δ 1]AC A =\mathrm{N} \mathbf{Z} [\Delta^1]\otimes A) as

BA[1],B\oplus A[1],

where

d(ba)=db+f(a)g(a)da.d(b\oplus a)=d b+f(a)-g(a)\oplus d a.

Last revised on January 31, 2021 at 16:58:36. See the history of this page for a list of all contributions to it.