An -simplex is the smallest conves set containing points, in general position, and is denoted by .
The standard -simplex is the set
The order of the vertices is important. By convention, the edges of a simplex is oriented so that points to if .
It is easily seen that all -simplices are (linearly) homeomorphic to the standard -simplex, and such a homeomorphism is determined by the vertices. As such, we often simply call any -simplex .
The -simplex is a face of the -simplex. The union of all faces form the boundary, and is denoted . The open simplex is . (The open simplex for the -simplex is defined to be the point itself.)
A -complex structure on a topological space is a collection of maps such that:
For a space with a -complex structure, we define to be the free abelian group generated by its -simplices. Elements in has the form where and . Elements in are called the -chains.
We define the boundary map as follows. For an -simplex , , i.e. maps a simplex to its (signed) boundary. It’s easy to see that .
The groups and maps together makes a chain complex (i.e. ), called the simplicial chain complex of . The homology groups of a chain complex is defined as , which are called the simplicial homology groups of :
Singular homology groups are obviously topological invariants. It’s also easier to study its properties.
The homology groups of is the direct sum of the homology groups of its path-connected components.
If is non-empty and path-connected, then .
If is a single point, then for all .
We can attach an additional to the end of the chain complex:
to eliminate the at . The homology groups of this extended chain complex are called the reduced homology groups . For , ; for , .
To prove this, we need some algebra. A chain map between chain complexes is such a map that ; i.e. the following diagram commutes.
It’s easy to deduce that a chain map can induce a homomorphism between the homology groups: . A continuous map induces a chain map between the singular chain complexes of and (just by composing), so it in turn induces a homomorphism between their singular homology groups.
The algebraic counterpart is as follows. A chain homotopy between two chain maps is a map such that . Then by some algebraic manipulations,
Actually, the (topological) homotopy between (continuous) maps induces a chain homotopy between their induced chain maps.
For any subspace of , we can define to get another chain complex . The boundary map is inherited from the singular chain complex of , and the cycles are called the relative cycles (because they are relative to : the boundary of a relative cycle lies in ). Its homology groups, , are called the relative homology groups.
Relative homology groups also have functoriality and homotopy invariance. Also, if is path-connected and is a point in , then .
A short exact sequence (s.e.s.) of chain complexes induces a long exact sequence (l.e.s.) of their homology groups:
In particular, there is a l.e.s. about the relative homology groups:
Suppose such that the closure of is contained inside the interior of . Then
A pair of a topological space and a subspace is called a good pair, if is closed, non-empty, and is a deformation retract of a neighbourhood of itself. Using the excision theorem and the l.e.s. of a pair, we can deduce that, for a good pair ,
Therefore:
For a good pair , there is a l.e.s. of the homology groups:
This sequence calculates the homology of space using a subspace and its quotient . There is another sequence, called the Mayer-Vietoris sequence, that calculates by covering it with two subspaces.
Suppose such that the interior of and cover . Then there is a l.e.s.
where and , is the (quotiented) boundary map.
With the tool of l.e.s. of a pair and excision, we can finally prove the equivalence of singular and simplicial homology:
Suppose () is a continuous map. Then induces a homomorphism . is isomorphic to , so must be of the form where is a generator of and . This is called the degree of the map , .
Below we list some properties of the degree:
For some applications of the degree, we mention:
If has no fixed point, then .
(Hairy ball theorem) A non-vanishing continuous vector field exists on , only if is odd.
If is even, then is the only non-trivial group that can act freely on .
A powerful tool to calculate degree is the ontion of local degree. We need an additional (very weak) condition for : there is a point with finitely many preimages . Suppose are disjoint neighbourhoods of , a neighbourhood of , such that . Then , and we have a diagram
Where , and are induced by inclusions, so that the diagram commutes. The upper two isomorphisms are from excision, and the lower two isomorphisms are from the l.e.s. Focus on the top map . By the isomorphisms, this is also a map , and therefore has the form . This is called the local degree of at , denoted .
The degree of is equal to the sum of local degrees at each . In symbols
A CW complex is a space built inductively as follows: start from , a set of discrete set. To build from , we attach some disks onto , by a family of attaching maps . The attached disks are called the -cells, and the maps are called the characteristic maps. We thus get a chain of spaces . We then define , and give it the weak topology, i.e. is closed if and only if is closed in for every . is called the -skeleton of the CW complex .
An important property of CW complexes is
A compact set in a CW complex only intersects with finitely many cells.
In particular a compact set in a CW complex is always contained in a finite skeleton.
We first state some preliminary facts:
Suppose is a CW complex.
Now we can fit portions of the three l.e.s. of pairs , and into a diagram
where is just the “relativized” boundary map (note that , which is the free abelian group generated by the -cells). The carries information about how -cells are attached to the -cells of . Using relative chains, we can ignore “holes” that comes from an earlier stage of construction, and only focus on -cycles added in the -skeleton.
The chain together with makes a chain complex, the cellular chain complex, denoted , and its homology groups are called the cellular homology groups .
A diagram chasing shows that the cellular homology group is isomorphic to the singular homology group:
This has some implications:
To compute the cellular homology we need a more precise formula for :
Suppose is an -cell of , are all -cells of and is the attaching map for , i.e. . By identifying everything except (the interior of) in , we will obtain with boundary identified, i.e. . We therefore get a map
and this is a map from to . Denote the degree of this map by . Then
Intuitively, counts how many times the boundary of traversed through .
Here is a minor technicality, that the orientation of the two -spheres may not be aligned (i.e. the choice for the generator of may not be consistent). We can do this by fixing an orientation for and suspend it to get a fixed set of generators for each .
As an application of cellular homology, let’s define the Euler characteristic for a finite CW complex :
Notice that the number of -cells is equal to . Using the short exact sequences
we deduce that the rank of the central term is the sum of the rank of the other two terms. Therefore, by some arithmetics,
Therefore,
This shows that the Euler characteristic is a topological invariant, independent of the CW structure given.
The above algebraic calculations can be generalized. Using exactly the same ideas, we can deduce the
Suppose is a finite chain complex, such that every is a free abelian group of finite rank. Suppose is a chain map from to itself. Then for every , we can write down the matrix of , and compute its trace . Also, will induce maps ; if we ignore the torsion and consider only the free part, then we can also calculate the trace . Then
This, together with the simplicial approximation theorem, has an important implication, a generalization of Brouwer’s fixed point theorem:
Suppose is a finite simplicial complex, and . We define the Lefschetz number
where we ignore the torsion part when calculating trace. actually, the requirement of finite simplicial complex is not substantial. Three conditions are needed: compact, locally contractible, and can be embedded into some Euclidean space.
If , then must have a fixed point.
When defining the chain groups, we can replace by any abelian group , and define . The homology groups of this chain complex, , is called the homology with coefficients in . Theorems like excision, l.e.s. of a pair, Mayer-Vietoris sequences, etc. also apply to this homology group.
However, there should be care when dealing with degrees. Because is generally not generated by one element, we can no longer talk about the degree of a map. There are exceptional cases, that is, when is a field. In this case, actually .
To answer the general question about the relation of and , we need to use the universal coefficients theorem, introduced in Section 2.2.
We now present five axioms, the Eilenberg-Steenrod axioms, that defines the behaviour of homology groups.
A homology theory is a sequence of functors from the category of pairs of topological spaces to the category abelian groups, together with a natural transformation , satisfying the following axioms:
homotopy invariance: Theorem 1.5, holds.
excision: Theorem 1.7 holds.
l.e.s. of a pair: Proposition 1.6 holds.
additivity: .
dimension:
The important theorem is,
This is just a recap of what we’ve learned; we can first use 4 and 5 to calculate , then by 1, 2 and 3 calculate , then by 3 calculate the cellular homology groups. We will use the notion of weak equivalence to prove the final step that the calculation of the homology of any space reduces to that of some CW complex.
Suppose is an abelian group. If we apply a contravariant Hom functor to the chain complex of , , we get another chain of maps, but reversed by contravariance:
where and . We also have in this case.
This chain of maps is called the cochain complex of , and its homology groups
is then called the cohomology groups of .
Cohomology groups share many properties with homology groups. To name a few:
A natural question to ask is: how are homology groups and cohomology groups related? It turns out that there is a completely algebraic answer, relating and .
A guess might be that . This turns out to be a good guess in some cases, but it’s generally not true. Actually, is always a direct summand of .
Another natural question to ask is to relate with . Unsurprisingly, it turns out that is always a direct summand of .
The precise relation is written in the following form, called the universal coefficient theorems for and :
Suppose is a chain complex of free abelian groups and is an abelian group. Then there are natural s.e.s’s
such that these s.e.s’s split, although not naturally.
We next illustrate how to calculate and .
Calculating
Calculating
We will not go deeper into the detailed definition of and here.
The universal coefficient theorems has a powerful generalization, called the Künneth formula:
Let be a principal ideal domain, and are chain complexes of -modules and are all free modules. Then there are natural s.e.s’s
that splits, although not naturally.
The differential on is defined as where ; the differential on is defined as , where .
Let us return to topology. Recall that the product of two CW complexes is still a CW complex, but the CW topology and the product topology might be different. Nonetheless, they are equal in finite dimensions, so they are equal on any compact subset, so it doesn’t matter the homology groups. Notice that , therefore we have split s.e.s.
The same holds for any PID as the coefficient ring.
If are all free -modules, then
If are all finitely generated free -modules, then
by the universal coefficient theorem.
We will see later, that this holds for all topological spaces, using a product called the cross product .
Suppose is a ring and a topological space. A good thing about cohomology is that we can define a multiplication on it, making it a ring. One such definition is called the cup product.
Suppose and . This means that and . We then define the cup product , by specifying its effect on a singular -simplex :
We can check that . Therefore, the cup product of two cocycles is a cocycle, and the cup product of a coboundary and a cocycle is a coboundary. Therefore, induces a well-defined map , making a graded -algebra.
There is also a relative version: if and are open sets in , or subcomplexes of a CW complex , then we can define a cup product
Also, if is a map between topological spaces, then it induces ring homomorphisms: .
Another important property of this ring structure is its graded commutativity. That is, if and , then .
Suppose and are topological spaces and and are the projection maps. Then for any and , we can pull them back to get cochains in : and . We define the cross product . Since this cross product is clearly -bilinear, it actually induces a map
If and are CW complexes, then this is a map we have seen before: the map appeared in the Künneth formula (Proposition 2.4). In particular, if and are CW complexes and is a finitely generated free -module for every , then is an -module isomorphism.
We can make a ring homomorphism, by defining an appropriate ring structure on , as follows: .
We also have the relative version of cross product:
and the reduced version:
where is the smash product with basepoints and .
As a special case, if , we then have where . The composition of these two maps is exactly the cup product .
Poincaré duality is another fundamentally different way of relating cohomology groups with homology groups of topological manifolds. Its general form states that,
Suppose is an -dimensional compact connected manifold, then
for every ;
if we further assume that is orientable, then for every .
Our next subsections will be devoted to proving this deep result, and discussing its significance on calculating the cup product structure.
In this section and sections to follow, we mainly consider connected, closed, compact manifold.
Suppose is a subset of . We define the local homology group of , denoted by , by .
If , then . Therefore, any cycle relative to is a cycle relative to , so we have a restriction map , induced by the inclusion .
If is a point, or a contractible open neighbourhood of a point that is small enough, then by excision . Intuitively, it describes how many times a chain, with boundary in , wraps around the “hole” .
There are two choices for the generator of . A chosen generator for is called the a local orientation .
We now choose a local orientation for every . We say that they satisfy the local consistency condition, that is, for every , there is a small open set around and a local orientation of , such that for any , , i.e. the restriction map takes to .
Intuitively, we draw a small loop around every point , and the local consistency condition says that the loops goes in the same direction in the proximity of every point.
If admits a choice of the local orientations that satisfies the local consistency condition, we say that is orientable. Otherwise, say is non-orientable.
Every non-orientable manifold has a double covering . This can be constructed as follows: as a set, . Since for each , there are two choices for , so is a two-to-one map. We give a topology, generated by sets for sufficiently small sets , making a covering space of . This constructed is always orientable.
This kind of construction can be done to any manifold, not just non-orientable ones. When one do it on an orientable manifold, what one get is a trivial covering map, with being just a disjoint union of two copies of . But when one do it on a non-orientable manifold, there is some loop on that when one goes around it once the orientation reverses, as on a Möbius band. Therefore, will be a connected manifold, and there is no way to find a copy of in it. In other words, there is no section .
In light of this observation, we introduce the notion of orientability to arbitrary coefficient rings. Suppose is a ring. We similarly define a manifold, a covering space of , by , with topological basis for any chosen and some fixed . The covering map is given by , so the fiber of each is with discrete topology.
Since , we can consider a subspace , where is a generator of . If , then . If , then will be the double cover we defined before. Therefore, is the disjoint union , and each is either or . For example, is the disjoint union of one (corresponding to ) and one for each .
We have seen that is orientable if and only if we can find a copy of in , or a section . Similarly we define the notion of -orientability. An -orientation is a section , such that is a generator (equivalently, a unit) for . A manifold that admits an -orientation is called -orientable, and a manifold with a fixed -orientation is called an -oriented manifold.
If is orientable, i.e. -orientable, then it is -orientable for every ring . If is not orientable, then it’s -orientable if and only if there is a unit such that . In particular, every manifold is -orientable.
We will establish the following result:
Let be a closed, compact, connected -dimensional manifold, and a point.
If is -orientable, then the map is an (-module) isomorphism.
If is not -orientable, then the previously mentioned map is injective, with image .
For , .
The technical part is the following lemma:
Suppose is any -dimensional manifold, and a compact subset.
If is a section of , then there is a unique such that .
, for any .
Assuming this lemma is true. Denote by the -module of sections of . Consider
This is an -linear map. The Lemma tells us that is an isomorphism by taking (notice that ).
By uniqueness of path lifting and is connected, we know that every section in is actually uniquely determined by its value at one point in . Therefore, fix a point , consider the evaluation map
Then is injective. Therefore, considering the diagram,
Since is injective and is an isomorphism, is injective and its image is equal to the image of .
If is -orientable, then is an isomorphism since its image contains a generator, the one making -orientable.
If is not -orientable, actually, if is not -orientable, then where if , if . Since is not orientable, there is no section from to ; therefore, every section is from to some where . Therefore, .
We start from simple sets, and gradually building up to general compact set .
Step 1. We claim that, if the Lemma holds for , and , then it also holds for . This can be proved by looking into the Mayer-Vietoris sequence
Step 2. For any compact set , we can write as the union of finitely many smaller compact sets, each is contained inside a single local chart of . Using step 1 and induction on the number of smaller sets, we only need to consider the case of one compact set contained in a single local chart. And by using excision, we reduced to .
Step 3. If is a convex set then deformation retracts to any point and deformation retracts to an -sphere around . Therefore we have a map
Therefore, statement 1 holds for convex , and therefore for finite unions of convex sets .
Step 4. For general , consider , suppose where . Let , then is a compact set. Cover with finitely many closed balls disjoint from , and let be the union of these closed balls. Then, from step 1 and 3, statement 1 holds for , so . Therefore, sends to . If , then , so statement 2 holds.
Now we prove statement 1.
Existence. Take any ball . Then satisfies the conditions.
Uniqueness. The cycle defines an element , which . If is another element satisfying the Lemma, let and where defined similarly, then for every . Since is an isomorphism for every , for every since this is true for . Therefore, by the uniqueness part of step 3, , so i.e. .
This theorem has some important implications.
First, it implies that if is -orientable, then , which is the case of the Poincaré duality theorem.
Second, it shows that an -oriented manifold determines a choice of a generator . This is called a fundamental class of . Conversely, if , then a fundamental class can be chosen, and we can define an -orientation by sending to . A fundamental class of an orientable manifold determines an orientation of that manifold, and vice versa.
Finally, from the proof and the universal coefficient theorem, we can get some information about the highest two homology groups from orientability:
For the highest homology group, if we take coefficients, then if is orientable, and if is non-orientable.
For the second highest, the torsion subgroup of is trivial if is orientable, and if is non-orientable.
Our proof of the Poincaré duality follows a similar route as that of Lemma 2.7. However we will encounter a difficulty in the last step, where we reduce to the case ; Poincaré duality does not hold for non-compact manifolds like . Therefore, we need an extension of the duality theorem to non-compact manifolds.
Suppose is any space and a commutative ring. For a cochain , we say that is compactly supported if there is a compact set , such that for any chain , . Obviously if is itself compact, then any cochain is compactly supported. Let be the subgroup containing all compactly supported -cochains. It’s easy to check that the coboundary map of any compactly supported cochain is sill compactly supported. Therefore, forms a cochain complex, and its homology groups are defined as the compactly supported cohomology groups, .
The compactly supported cohomology is not natural as a functor from to ; rather, it is only natural under proper maps. A continuous map between spaces is called proper, if the preimage of any compact set is compact; a homotopy is called a proper homotopy if the map is proper. Then the compactly supported cohomology groups are natural under proper maps and are invariant under proper homotopies. As an example, but .
The compactly supported cohomology can also be defined using direct limits. Suppose is a poset, such that any two elements of has a common upper bound. Such a poset is called a directed set. Given a functor , we can define the direct limit of the groups , denoted , by , where is defined by , where and , iff there is a , such that , , and and maps to the same element under and . Intuitively, the direct limit is the “smallest group containing all groups ”.
Suppose is the union of a directed set of topological spaces ordered by inclusion, such that every compact set is contained entirely inside . Then
.
.
As a corollary, the compact subsets of form a directed set under inclusion; therefore,
The first statement about homology holds without compactness assumptions because the images of simplices are already compact by themselves.
A particular thing about compactly supported cohomology is that it can be covariant, as opposed to the normal cohomology group which is contravariant. This is because we can pushforward a compactly supported cochain, as follows. Suppose is an inclusion of open sets. Then for any , we can extend it to a cochain in , by simply defining outside of . Since the support is already inside , we get a well-defined chain. This gives us a map , and thus a map .
We can now generalize the Poincaré duality to non-compact manifolds:
To prove this we must first construct a map from to , and then verify that it is an isomorphism. This map turns out to be constructed using cap products, a product that looks much like the cup product.
Let be any space and be a commutative ring. We define the cap product
The cap product satisfies that ; so the cap product induces a well defined map on (co)homology groups . Moreover, like the cup product, the cap product is a natural map.
There is also a relative version:
Let be an -orientable -dimensional manifold, and fix an orientation . Consider compact subsets . Then the inclusion induces and on (co)homology groups. Consider the following diagram:
Using Lemma 2.7, there is a unique , such that for any ; we have the same for . Uniqueness implies that . Then naturality of the cap product implies that, for any , . Therefore, the map is natural under inclusion of ; therefore, it induces a well-defined map on the direct limit . This gives a map .
Suppose and are open subsets. We have two Mayer-Vietoris sequences
Notice the first row is different from the Mayer-Vietoris sequence of normal cohomology groups, because we can make compactly supported cohomology groups covariant. By the five lemma, if , and are all isomorphisms, then so if .
We clain that, if where , and are all isomorphisms, then is also an isomorphism. This is seem by
We can check that is an isomorphism; since every manifold is second countable, we finished the proof.
In the case of a closed (compact) manifold , this is given by .
The cap product is closely related to the cup product. Some basic identities involving both are
for , and ;
, which makes the homology group into a right module of the cohomology ring.
Recall that by the universal coefficient theorem there is a surjective homomorphism , but this is in general not an isomorphism. If we fix a , then we get a commutative diagram
In particular, when is an isomorphism, the cap product and the cup product are dual to each other.
From this relation we can state the Poincaré duality for cup products. A bilinear pairing on two -modules and is a bilinear map , or equivalently a map . A bilinear pairing is called non-singular, if the induced maps and are isomorphisms.
For an -oriented manifold , we can define the Poincaré pairing:
By graded commutativity of the cup product, this Poincaré pairing is also graded commutative. In particular, as an application, if , then the pairing on is anti-symmetric, showing that must have even dimension. Therefore, if is a -dimensional oriented compact manifold, then is even.
Poincaré duality also allows us to understand cup products in a geometrical way. Suppose is an -oriented closed connected -dimensional manifold. We fix the coefficient ring , and denote the duality map. Poincaré duality tells us that is an isomorphism, so an inverse exists: . For a homology class , the dual cohomology class will frequently be denoted by .
We define the intersection product :
In formula, is defined by
This formula can be simplified to .
The name “intersection product” can be justified as follows. Suppose that is moreover a smooth manifold, and and are embedded oriented closed connected submanifolds of , with dimensions and respectively. We say that and intersect transversely, if at any point , . In this case, is a -dimensional embedded submanifold, and inherits an orientation from and .
We spend some time here to explain how exactly we orient . An orientation on a smooth manifold can be described by bases of tangent spaces; a basis of the tangent space at is a local orientation at , and two orientations are consistent if one can transform one to another using a linear transformation with positive determinant. We can relate the tangent spaces of , and using a natural s.e.s.
This gives local orientations of through local orientations of , and .
Inclusion gives and , and we denote, by abuse of notation, the images of the fundamental classes in by and . The main theorem is:
For embedded oriented closed connected manifolds and of an oriented closed manifold ,
Equivalently, in cup products,
where is the Poincaré dual of .
In general, however, cup products are more general than intersection products, as not every homology class of is represented as the fundamental class of some submanifold.
As a corollary, since of a connected manifold is always and can only take one of the two orientations, if two submanifolds intersects at an odd number of points, then they cannot cancel out in ; therefore, if and intersects at an odd number of points, then is not zero, and therefore and are non-zero.
For an application, we can show using this corollary that non-orientable surfaces cannot be embedded in , because we can otherwise find a loop in that only intersect it once, but . (As depicted in the following graph; connecting the two ends of the red arc gives such a curve.)
For an application, all hyperplanes in (i.e. the zero set of for , and not all zero) shares a same homology class where , and . We can use this to imply the Bézout theorem for : if two smooth algebraic curves of degees and intersects transversally, then they intersect at points.
Suppose is a based space, and .
The -th homotopy group is defined, as a set, by
The group structure can be defined for , as
In particular, is the familiar fundamental group.
An interesting property of higher homotopy groups is that
For an intuition about why this is right, see the following diagram:
Similar to the case of fundamental groups,
In particular, this gives us a group action . If this action is trivial, we say that is -simple, and write , omitting the basepoint.
Since , he group can also be described as the set , modulo homotopy . The addition can then be described as
As is the case for , higher homotopy groups are functors
and homotopy equivalences induces isomorphisms.
Homotopy groups behave particularly well under covering maps:
In particular, if has a contractible universal cover, then for .
The homotopy groups of products are simple to compute:
We can also define the relative homotopy groups for . Let be the closure of the union of all but one faces of the -cube . Then consists of all maps , modulo homotopy through such maps. Group multiplication is defined similarly. In terms of spheres, this is the set of maps , modulo homotopy through such maps. The relative homotopy group is indeed a group only when , and is abelian when . The intuition is that, in the diagram for Proposition 3.2, this time we need that the rectangles and be “rooted” in , and in dimension two, there is no enough place for the two rooted rectangles to swap positions, while in dimension three there is enough place.
Like in homology groups, there is a l.e.s. of relative homotopy groups:
There is a long exact sequence
where is induced by inclusion and is induced by inclusion . comes from restricting a map to .
There should be special care to the last few terms; they are not groups. However, as sets, they have a special element, namely, the homotopy class represented by constant maps. For maps involving these sets, kernel means every element that get mapped to the homotopy class of constant maps.
A based space is called -connected if for all . Then the following statements are equivalent:
There are three key results in the study of homotopy groups: cellular approximation, Whitehead’s theorem and CW approximation.
Suppose and are CW complexes. A cellular map is such a map that maps the -skeleton of to the -skeleton of , for every .
As an example, let . For any , can be homotoped to a cellular map. If , then is a point (since the -skeleton of is just a point). Therefore, is a constant map. We have just proved that
As a corollary
A CW pair is -connected if all cells in has dimension larger than .
In particular, is -connected, where is the -skeleton of .
Therefore, the inclusion induces isomorphisms for for :
The -th homotopy groups of for is completely determined by its -skeleton.
In particular, adding -cells to does not affect or lower homotopy groups.
The following lemma is a generalization of the compression criterion:
Suppose is a pair of topological spaces such that , and is a CW pair. Suppose that, for all , whenever has an -cell, for all .
Then every map is homotopic rel to a map , i.e. can be “compressed” into .
A map is called a weak homotopy equivalence if it induces an isomorphism on all homotopy groups with respect to all basepoints. Obviously a homotopy equivalence is a weak homotopy equivalence. Whitehead’s theorem says that the converse is true for CW complexes:
For any topological space , there exists a CW complex and a weak homotopy equivalence .
Moreover, such a is unique, up to homotopy equivalence.
This is called the CW approximation of .
Weak homotopy equivalence is the best we can hope; the quasi-circle, obtained by connecting the two ends of a topologist’s sine wave with a curve, is weakly homotopy equivalent to a point, but not homotopy equivalent to any CW complex.
It turns out that no algebraic topology invariant can distinguish between weakly homotopy equivalent spaces:
A notable technique involved here is by introducing the mapping cylinder , defined for , by attaching one base for the cylinder to by . The noticable feature of this space is that the obvious inclusion map can be homotoped to the map , so in proving such statements we can assume that is an inclusion.
Let us denote the set of maps , modulo homotopy rel basepoint. Then the homotopy groups as sets can be written as . A weak homotopy equivalence then induces a bijection . Turns out that this holds not only for spheres but also for all CW complexes:
A weak homotopy equivalence induces a bijection for every CW complex :
Our goal is to calculate the homotopy groups of union of spaces, as in the Mayer-Vietoris sequence. In , we have the nice Seifert-van Kampen theorem. However this fails for . Even the homotopy groups for wedge products can be complex.
As an example, we can prove that , whether finite or countably infinite. Consider for . This is isomorphic to of its universal cover, which is with a attached on every point of . This space is homotopy equivalent to the wedge sum of countably infinite , so its is the direct sum of countably infinitely many . This shows that even finite CW complexes can have infinite homotopy groups.
We do however have the following version of the “excision” property:
This suspension theorem has the following implications. First, suppose that is -connected, then is -connected. Second, the maps is eventually an isomorphism, so this sequence of groups are eventually all isomorphic to a group. This group is called the stable homotopy group .
As an application, an Eilenberg-Mac Lane space for and an abelian group is a space such that if and if .
For any abelian group and any , there is a unique CW complex, up to homotopy equivalence, that is a . This is therefore called the .
Any group homomorphism between can be induced by a continuous map between spaces.
The Hurewicz map is a map that maps to . There is also a relative version , that maps to where is the fundamental class of .
If is -connected for some and is simply connected, then for and by .
A map between simply connected CW complexes is a homotopy equivalence, if it induces isomorphisms on all homology groups.
A map is said to have the homotopy lifting property (h.l.p.) for a space , if given any homotopy and a map lifting , there exists a homotopy lifting .
Dually, a map is said to have th homotopy extension property (h.e.p.) for a space , if given any homotopy such that extends to , we can extend to a homotopy .
A (Hurewicz) fibration is a map having the h.l.p. for all topological spaces . A cofibration is a map having the h.e.p. for all topological spaces .
The h.l.p. for all disks can imply h.l.p. for all CW complexes. A Serre fibration is a map having the h.l.p. for all CW complexes, or equivalently, all disks.
If is a Serre fibration, is the basepoint of and , then is an isomorphism for all .
Therefore, if is path-connected, there is a l.e.s.
Given a fibration , denote the fiber at : . Given a curve , view as a homotopy . Then for any , we can take a lift of to such that . This gives a map .
This satisfies the following properties:
In particular,
Denote by the group of homotopy equivalences modulo homotopy. If is path-connected, this then gives a map , called the monodromy representation. For example, if is a covering map, then is the deck transformation.
As a special case, fiber bundles are fibrations such that the fibers are homeomorphic.
Precisely, a fiber bundle is a map such that each point has a neighbourhood and a homeomorphism such that the following diagram commutes:
This is called a local trivialization, because the product is called a trivial bundle on , and means that the bundle is locally trivial.
For any path-connected component , are all homeomorphic for all . Therefore, if is path-connected, then for all in , . is called the fiber of this fiber bundle.
Fiber bundles are Serre fibrations.
If additionally is paracompact, then it’s also a Hurewicz fibration.
Examples of fiber bundles include: all covering maps, , , etc.
projective spaces. We have fiber bundles
where is the quaternions (similar reesults hold for the octonions, up to ). In particular, we have the following Hopf fibrations on , , and respectively:
Also, taking , we proved that is a and is a .
Lie groups. Let . The fiber is . This gives a fiber bundle . The l.e.s. of this fiber bundle shows that if . Therefore, for large enough , is constant. This constant group is the stable homotopy group of the orthogonal group .
There is a Bott periodicity theorem that says the stable homotopy groups are periodic in :
Similar results hold for and .
Given fibrations (), say a map is fiber-preserving if , and is a fiber homotopy equivalence if it’s fiber-preserving, and there is some such that and through fiber-preserving maps.
Given a fibration and a map , the pullback fibration is , and defined by projection is a fibration. is also denoted , the fiber product. A pullback is represented in the commutative diagram by a symbol.
If are homotopic, then the pullback fibrations and are fiber homotopy equivalent. Therefore, if is contractible, then every fibration is fiber homotopy equivalent to the trivial fibration.
Recall the construction of the mapping cylinder: for any map , we can construct
such that is a homotopy equivalence, and is a cofibration. We now describe a dual to thie construction, justifying the slogan that “every map is a fibration”.
For any map , let . Then is a subset of , where is the set of maps with the compact-open topology. The fact is that
Therefore we have a construction
where is a homotopy equivalence, and is a fibration.
If is path-connected, the fiber of is well-defined up to homotopy equivalence. This fiber is called the homotopy fiber of the map , denoted ; explicitly, , up to homotopy equivalence.
If itself is a fibration with fiber , then is a homotopy equivalence, and the homotopy fiber is then homotopy equivalent to the “true” fiber .
As a special case, take . Then . This is called the path space of . The homotopy fiber is , called the loop space of . We therefore get a fibration . This is the loop fibration.
Observe that is contractible, by contracting every path to its starting point; therefore, by the l.e.s. of the fibration, . In particular, , where denotes weak homotopy equivalence. For example, , , and .
A non-trivial fact, proved by Milnor, is that the loop space of a CW complex is always homotopy equivalent to a CW complex.
The important fact about the path space fibration is that it is the universal fibration; that is, any fibration with fiber is a pullback of the path space fibration .
Given a fibration , we can form a fibration . This in turn gives a fibration , etc. This is called a fibration sequence
where every two consecutive maps form a fibration.
Let denote maps modulo homotopy, and denote based maps modulo homotopy rel basepoints.
The main result will be
There is a natural bijection
for all , CW complexes and abelian groups .
Let’s start by making more explicit. Let . Then by universal coefficient theorem and Hurewicz theorem, . There is a special element in , namely the identity map; its pre-image in , , is called the fundamental class of . Then can be written as .
If we forget about basepoints, we then get a map . In most cases this won’t be a problem; this is a bijection for , and if is abelian for . For we need to replace by for based maps.
Since is a bijection, we would expect that has a group structure. It turns out that there is a natural group structure when is a suspension , where multiplication is defined via as in the case of . If we also take basepoints into consideration, we need to replace suspension by reduced suspension ; therefore, forms a group for based spaces and .
For general which is not a suspension, we need the following adjoint relation
The group structure on is given by composition of loops . For large enough, is an abelian group.
Inspired by this, an -spectrum is a sequence of CW complexes wich weak homotopy equivalences .
Therefore, for the -spectrum , this theorem implies Theorem 3.27.
Theorem 3.27 allows us to prove clains about cohomology by studying the universal example, the fundamental class of .
Consider the following questions:
Extension problem. Given a CW pair and a map , does it extend to ?
Lifting problem. Given a fibration and a map , does lift to a map ?
These two questions both generalizes to the
Relative lifting problem. Given a CW pair , a fibration , a map and a partial lift , is there a global lift that extends it?
Obstruction theory will tell us that a solution to these problems won’t exist if some obstruction classes are present.
A Postnikov tower for a path-connected space is a commutative diagram
such that the map induces isomorphisms on all (for ), and for all .
We can additionally assume that is a fibration for all . Let be the homotopy fiber of ; then by the l.e.s. of a fibration, .
We can construct the inverse limit of all the spaces , denoted by . The inverse limit of the maps gives a map . This map is a weak homotopy equivalence: .
A fibration is called principal, if there is a commutative diagram
where the lower row is a fibration sequence.
Consider a portion of the Postnikov tower with principal fibrations:
Because the fibration is principal, according to the diagram above, we can construct a fibration .
A space is called simple if is abelian, and all actions are trivial. For such a space, we can furthur extend the Postnikov tower to have an additional term .
Let’s focus on the extension problem first. Suppose is simple. Look at its Postnikov tower with principal fibrations. The violet line is the extension we are looking for, and the red lines are the same fibrations as the one the red arrows represents in the previous diagram.
We already have a trivial map . The plan is to induct on ; by induction hypothesis we already have . We with to lift it to .
Let . Then is the fiber of the fibration . Therefore, is a pullback fibration:
The key observation is that, since is contractible, a lift can be identified with a nullhomotopic map .
Now we have a lift on , and a nullhomotopy . All these gives a map where is the cone of with base identified with . Remember that ; therefore, such a map corresponds to a cohomology class , which, by excision, is isomorphic to . This is called the obstruction class. A lifting exists, if and only if .
For the relative lifting problem for a CW pair and a fibration , one need to consider a variant of the Postnikov tower.
Suppose is a fibration with fiber . The Moore-Postnikov tower is a commutative diagram
such that
Every fibration has a Moore-Postnikov tower, unique up to homotopy equivalence. A Moore-Postnikov tower of principal fibrations exists if the action of on is trivial for any . Here is the mapping cylinder of .
Therefore, to solve the relative lifting problem for and , we first assume that the action of on is trivial for ; we need to additionally assume that the given map takes into , so that the induction basis can be constructed. We also need that is abelian where is the fiber of .
Under all these conditions, we can use a similar argument as before, to the following similar diagram:
In this case the obstruction class lies in .
Generally, depends on the choice of the lift . Therefore, even if a non-zero obstruction exists, it may not imply that a solution doesn’t exist; it may be due to an inappropriate choice of previous lifts.
However, the converse is true; if all obstruction classes are zero, then a solution do exist.
There is, however, a case where the choice of is canonical. If is -connected, then is the first possible non-zero cohomology; the obstruction class is then called the first or the primary obstruction, and does not depend on the choices of lifts in the previous steps.
suppose is a fibration and is a CW complex, and suppose that is contractible. Consider the relative lifting problem for CW pair , fibration and map . A fact is that the Moore-Postnikov tower of principal fibrations always exists for such a fibration. Also, because . Therefore, obstruction theory applies; since is contractible, all obstruction classes are zero, so a lift exists. This lift is a section .
Therefore, if is a fibration with contractible, then there is a section .
there are various applications of the previous example.
We prove that every closed -dimensional manifold has a Riemannian metric. Let be all positive definite bilinear maps . A Riemannian metric is then a section . is a fiber bundle, with fiber the set of positive definite bilinear forms on . This is a convex subspace of , so it’s contractible. Therefore, a section does exist.
When does a closed orientable -dimensional manifold has a nowhere vanishing vector field?
Let . Then a nowhere vanishing vector field is a section . The fiber bundle has fiber , so the obstruction class lies in . This is zero for . Since is -dimensional, it’s also zero for . So the only possible obstruction is .
A fact is that the Poincaré pairing is equal to . Therefore, a nowhere vanishing vector field exists if and only if .
a particularly important application is the principal bundle.
If is a fiber bundle, is a topological group, acts on preserving fibers, such that act on every fiber freely and transitively (so that by orbit-stabilizer), and , say this fiber bundle a principal -bundle. Examples include: if is a closed Lie subgroup of then is a principal -bundle.
A theorem by Milnor says that, for any topological group , there is a principal -bundle such that is contractible. This is called the classifying space of .
This principal bundle is universal, in the sense that every other principal -bundle is a pullback of it. To see this, let be the quotient of by action of . Then we have two fiber bundles
Since is contractible, there is a section , which gives a map . This map then gives a principal fibration
showing that . This is actually the origin of the notion of principal fibration.
The cohomology of fiber bundles is generally hard to compute. Even for the trivial bundle , we already need the Künneth formula. The general computation requires the notion of Serre spectral sequences. However, there is an important special case where spectral sequences are not required:
Suppose is a commutative ring, is a fiber bundle, such that
is a finitely generated free -module for all ;
is surjective.
Let () such that forms a basis of .
Then the map
is an isomorphism of -modules. Actually, is a free -module generated by .