Homotopy colimit and limit

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In mathematics, especially in algebraic topology, the homotopy limit and colimit[1]pg 52 are variants of the notions of limit and colimit extended to the homotopy category

Ho(Top)

. The main idea is this: if we have a diagram

F:ITop

considered as an object in the homotopy category of diagrams

FHo(TopI)

, (where the homotopy equivalence of diagrams is considered pointwise), then the homotopy limit and colimits then correspond to the cone and cocone

HolimI(F):*TopHocolimI(F):*Top

which are objects in the homotopy category

Ho(Top*)

, where

*

is the category with one object and one morphism. Note this category is equivalent to the standard homotopy category

Ho(Top)

since the latter homotopy functor category has functors which picks out an object in

Top

and a natural transformation corresponds to a continuous function of topological spaces. Note this construction can be generalized to model categories, which give techniques for constructing homotopy limits and colimits in terms of other homotopy categories, such as derived categories. Another perspective formalizing these kinds of constructions are derivators[2]pg 193 which are a new framework for homotopical algebra.

Introductory examples

Homotopy pushout

The concept of homotopy colimit[1]pg 4-8 is a generalization of homotopy pushouts, such as the mapping cylinder used to define a cofibration. This notion is motivated by the following observation: the (ordinary) pushout

DnSn1pt

is the space obtained by contracting the (n−1)-sphere (which is the boundary of the n-dimensional disk) to a single point. This space is homeomorphic to the n-sphere Sn. On the other hand, the pushout

ptSn1pt

is a point. Therefore, even though the (contractible) disk Dn was replaced by a point, (which is homotopy equivalent to the disk), the two pushouts are not homotopy (or weakly) equivalent.

Therefore, the pushout is not well-aligned with a principle of homotopy theory, which considers weakly equivalent spaces as carrying the same information: if one (or more) of the spaces used to form the pushout is replaced by a weakly equivalent space, the pushout is not guaranteed to stay weakly equivalent. The homotopy pushout rectifies this defect.

The homotopy pushout of two maps ABC of topological spaces is defined as

A1B×[0,1]0B1B×[0,1]0C,

i.e., instead of glueing B in both A and C, two copies of a cylinder on B are glued together and their ends are glued to A and C. For example, the homotopy colimit of the diagram (whose maps are projections)

X0X0×X1X1

is the join X0*X1.

It can be shown that the homotopy pushout does not share the defect of the ordinary pushout: replacing A, B and / or C by a homotopic space, the homotopy pushout will also be homotopic. In this sense, the homotopy pushouts treats homotopic spaces as well as the (ordinary) pushout does with homeomorphic spaces.

Composition of maps

Another useful and motivating examples of a homotopy colimit is constructing models for the homotopy colimit of the diagram

AfXgY

of topological spaces. There are a number of ways to model this colimit: the first is to consider the space

[(A×I)(X×I)Y]/

where

is the equivalence relation identifying

(a,1)(f(a),0)(x,1)g(x)

which can pictorially be described as the picture

Because we can similarly interpret the diagram above as the commutative diagram, from properties of categories, we get a commutative diagram

giving a homotopy colimit. We could guess this looks like

but notice we have introduced a new cycle to fill in the new data of the composition. This creates a technical problem which can be solved using simplicial techniques: giving a method for constructing a model for homotopy colimits. The new diagram, forming the homotopy colimit of the composition diagram pictorially is represented as

giving another model of the homotopy colimit which is homotopy equivalent to the original diagram (without the composition of

gf

) given above.

Mapping telescope

The homotopy colimit of a sequence of spaces

X1X2,

is the mapping telescope.[3] One example computation is taking the homotopy colimit of a sequence of cofibrations. The colimit of [1]pg 62 this diagram gives a homotopy colimit. This implies we could compute the homotopy colimit of any mapping telescope by replacing the maps with cofibrations.

General definition

Homotopy limit

Treating examples such as the mapping telescope and the homotopy pushout on an equal footing can be achieved by considering an Template:Mvar-diagram of spaces, where Template:Mvar is some "indexing" category. This is a functor

X:ISpaces,

i.e., to each object Template:Mvar in Template:Mvar, one assigns a space Template:Math and maps between them, according to the maps in Template:Mvar. The category of such diagrams is denoted Template:Math.

There is a natural functor called the diagonal,

Δ0:SpacesSpacesI

which sends any space Template:Mvar to the diagram which consists of Template:Mvar everywhere (and the identity of Template:Mvar as maps between them). In (ordinary) category theory, the right adjoint to this functor is the limit. The homotopy limit is defined by altering this situation: it is the right adjoint to

Δ:SpacesSpacesI

which sends a space Template:Mvar to the Template:Mvar-diagram which at some object Template:Mvar gives

X×|N(I/i)|

Here Template:Math is the slice category (its objects are arrows Template:Math, where Template:Mvar is any object of Template:Mvar), Template:Mvar is the nerve of this category and |-| is the topological realization of this simplicial set.[4]

Homotopy colimit

Similarly, one can define a colimit as the left adjoint to the diagonal functor Template:Math given above. To define a homotopy colimit, we must modify Template:Math in a different way. A homotopy colimit can be defined as the left adjoint to a functor Template:Math where

Template:Math,

where Template:Math is the opposite category of Template:Mvar. Although this is not the same as the functor Template:Math above, it does share the property that if the geometric realization of the nerve category (Template:Math) is replaced with a point space, we recover the original functor Template:Math.

Examples

A homotopy pullback (or homotopy fiber-product) is the dual concept of a homotopy pushout.Template:Citation needed span Concretely, given f:XZ and g:YZ, it can be constructed as

X×ZhY:=X×ZZI×ZY={(x,γ,y)|f(x)=γ(0),g(y)=γ(1)}.[5]

For example, the homotopy fiber of f:XY over a point y is the homotopy pullback of f along yY.[5] The homotopy pullback of f along the identity is nothing but the mapping path space of f.

The universal property of a homotopy pullback yields the natural map X×ZYX×ZhY, a special case of a natural map from a limit to a homotopy limit. In the case of a homotopy fiber, this map is an inclusion of a fiber to a homotopy fiber.

Construction of colimits with simplicial replacements

Given a small category

I

and a diagram

D:ITop

, we can construct the homotopy colimit using a simplicial replacement of the diagram. This is a simplicial space,

srep(D)

given by the diagram[1]pg 16-17

where

srep(D)n=i0i1inD(in)

given by chains of composable maps in the indexing category

I

. Then, the homotopy colimit of

D

can be constructed as the geometric realization of this simplicial space, so

hocolimD=|srep(D)|

Notice that this agrees with the picture given above for the composition diagram of

AXY

.

Relation to the (ordinary) colimit and limit

There is always a map

hocolimXicolimXi.

Typically, this map is not a weak equivalence. For example, the homotopy pushout encountered above always maps to the ordinary pushout. This map is not typically a weak equivalence, for example the join is not weakly equivalent to the pushout of X0X0×X1X1, which is a point.

Further examples and applications

Just as limit is used to complete a ring, holim is used to complete a spectrum.

See also

References

Template:Reflist

Further reading

  1. 1.0 1.1 1.2 1.3 Template:Cite web
  2. Template:Cite web
  3. Hatcher's Algebraic Topology, 4.G.
  4. Bousfield & Kan: Homotopy limits, Completions and Localizations, Springer, LNM 304. Section XI.3.3
  5. 5.0 5.1 Math 527 - Homotopy Theory Homotopy pullbacks