Fibration Explained

The notion of a fibration generalizes the notion of a fiber bundle and plays an important role in algebraic topology, a branch of mathematics.

Fibrations are used, for example, in Postnikov systems or obstruction theory.

In this article, all mappings are continuous mappings between topological spaces.

Formal definitions

Homotopy lifting property

A mapping

p\colonE\toB

satisfies the homotopy lifting property for a space

X

if:

h\colonX x [0,1]\toB

and

\tildeh0\colonX\toE

lifting

h|X=h0

(i.e.

h0=p\circ\tildeh0

)

there exists a (not necessarily unique) homotopy

\tildeh\colonX x [0,1]\toE

lifting

h

(i.e.

h=p\circ\tildeh

) with

\tildeh0=\tildeh|X.

The following commutative diagram shows the situation:

Fibration

A fibration (also called Hurewicz fibration) is a mapping

p\colonE\toB

satisfying the homotopy lifting property for all spaces

X.

The space

B

is called base space and the space

E

is called total space. The fiber over

b\inB

is the subspace

Fb=p-1(b)\subseteqE.

Serre fibration

A Serre fibration (also called weak fibration) is a mapping

p\colonE\toB

satisfying the homotopy lifting property for all CW-complexes.

Every Hurewicz fibration is a Serre fibration.

Quasifibration

A mapping

p\colonE\toB

is called quasifibration, if for every

b\inB,

e\inp-1(b)

and

i\geq0

holds that the induced mapping

p*\colon\pii(E,p-1(b),e)\to\pii(B,b)

is an isomorphism.

Every Serre fibration is a quasifibration.

Examples

p\colonB x F\toB

is a fibration. That is, trivial bundles are fibrations.

p\colonE\toB

is a fibration. Specifically, for every homotopy

h\colonX x [0,1]\toB

and every lift

\tildeh0\colonX\toE

there exists a uniquely defined lift

\tildeh\colonX x [0,1]\toE

with

p\circ\tildeh=h.

p\colonE\toB

satisfies the homotopy lifting property for every CW-complex.

i*\colon

Ik
X

\to

\partialIk
X
induced by the inclusion

i\colon\partialIk\toIk

where

k\in\N,

X

a topological space and

XA=\{f\colonA\toX\}

is the space of all continuous mappings with the compact-open topology.

S1\toS3\toS2

is a non-trivial fiber bundle and, specifically, a Serre fibration.

Basic concepts

Fiber homotopy equivalence

A mapping

f\colonE1\toE2

between total spaces of two fibrations

p1\colonE1\toB

and

p2\colonE2\toB

with the same base space is a fibration homomorphism if the following diagram commutes:The mapping

f

is a fiber homotopy equivalence if in addition a fibration homomorphism

g\colonE2\toE1

exists, such that the mappings

f\circg

and

g\circf

are homotopic, by fibration homomorphisms, to the identities
\operatorname{Id}
E2
and
\operatorname{Id}
E1

.

Pullback fibration

Given a fibration

p\colonE\toB

and a mapping

f\colonA\toB

, the mapping

pf\colonf*(E)\toA

is a fibration, where

f*(E)=\{(a,e)\inA x E|f(a)=p(e)\}

is the pullback and the projections of

f*(E)

onto

A

and

E

yield the following commutative diagram:The fibration

pf

is called the pullback fibration or induced fibration.

Pathspace fibration

With the pathspace construction, any continuous mapping can be extended to a fibration by enlarging its domain to a homotopy equivalent space. This fibration is called pathspace fibration.

The total space

Ef

of the pathspace fibration for a continuous mapping

f\colonA\toB

between topological spaces consists of pairs

(a,\gamma)

with

a\inA

and paths

\gamma\colonI\toB

with starting point

\gamma(0)=f(a),

where

I=[0,1]

is the unit interval. The space

Ef=\{(a,\gamma)\inA x BI|\gamma(0)=f(a)\}

carries the subspace topology of

A x BI,

where

BI

describes the space of all mappings

I\toB

and carries the compact-open topology.

The pathspace fibration is given by the mapping

p\colonEf\toB

with

p(a,\gamma)=\gamma(1).

The fiber

Ff

is also called the homotopy fiber of

f

and consists of the pairs

(a,\gamma)

with

a\inA

and paths

\gamma\colon[0,1]\toB,

where

\gamma(0)=f(a)

and

\gamma(1)=b0\inB

holds.

For the special case of the inclusion of the base point

i\colonb0\toB

, an important example of the pathspace fibration emerges. The total space

Ei

consists of all paths in

B

which starts at

b0.

This space is denoted by

PB

and is called path space. The pathspace fibration

p\colonPB\toB

maps each path to its endpoint, hence the fiber

p-1(b0)

consists of all closed paths. The fiber is denoted by

\OmegaB

and is called loop space.

Properties

p-1(b)

over

b\inB

are homotopy equivalent for each path component of

B.

f\colon[0,1] x A\toB

the pullback fibrations
*
f
0(E)

\toA

and
*
f
1(E)

\toA

are fiber homotopy equivalent.

B

is contractible, then the fibration

p\colonE\toB

is fiber homotopy equivalent to the product fibration

B x F\toB.

p\colonE\toB

is very similar to itself. More precisely, the inclusion

E\hookrightarrowEp

is a fiber homotopy equivalence.

p\colonE\toB

with fiber

F

and contractible total space, there is a weak homotopy equivalence

F\to\OmegaB.

Puppe sequence

For a fibration

p\colonE\toB

with fiber

F

and base point

b0\inB

the inclusion

F\hookrightarrowFp

of the fiber into the homotopy fiber is a homotopy equivalence. The mapping

i\colonFp\toE

with

i(e,\gamma)=e

, where

e\inE

and

\gamma\colonI\toB

is a path from

p(e)

to

b0

in the base space, is a fibration. Specifically it is the pullback fibration of the pathspace fibration

PB\toB

along

p

. This procedure can now be applied again to the fibration

i

and so on. This leads to a long sequence:

\toFj\toFi\xrightarrow{j}Fp\xrightarrowiE\xrightarrowpB.

The fiber of

i

over a point

e0\inp-1(b0)

consists of the pairs

(e0,\gamma)

where

\gamma

is a path from

p(e0)=b0

to

b0

, i.e. the loop space

\OmegaB

. The inclusion

\OmegaB\hookrightarrowFi

of the fiber of

i

into the homotopy fiber of

i

is again a homotopy equivalence and iteration yields the sequence:

\Omega2B\to\OmegaF\to\OmegaE\to\OmegaB\toF\toE\toB.

Due to the duality of fibration and cofibration, there also exists a sequence of cofibrations. These two sequences are known as the Puppe sequences or the sequences of fibrations and cofibrations.

Principal fibration

A fibration

p\colonE\toB

with fiber

F

is called principal, if there exists a commutative diagram:The bottom row is a sequence of fibrations and the vertical mappings are weak homotopy equivalences. Principal fibrations play an important role in Postnikov towers.

Long exact sequence of homotopy groups

For a Serre fibration

p\colonE\toB

there exists a long exact sequence of homotopy groups. For base points

b0\inB

and

x0\inF=p-1(b0)

this is given by:

\pin(F,x0)\pin(E,x0)\pin(B,b0)\pin(F,x0)

\pi0(F,x0)\pi0(E,x0).

The homomorphisms

\pin(F,x0)\pin(E,x0)

and

\pin(E,x0)\pin(B,b0)

are the induced homomorphisms of the inclusion

i\colonF\hookrightarrowE

and the projection

p\colonEB.

Hopf fibration

Hopf fibrations are a family of fiber bundles whose fiber, total space and base space are spheres:

S0\hookrightarrowS1S1,

S1\hookrightarrowS3S2,

S3\hookrightarrowS7S4,

S7\hookrightarrowS15S8.

The long exact sequence of homotopy groups of the hopf fibration

S1\hookrightarrowS3S2

yields:

1,x
\pi
0)

3,
\pi
n(S

x0)

2,
\pi
n(S

b0)\pin(S1,x0)

1,
\pi
1(S

x0)

3,
\pi
1(S

x0)

2,
\pi
1(S

b0).

This sequence splits into short exact sequences, as the fiber

S1

in

S3

is contractible to a point:

0

3)
\pi
i(S

2)
\pi
i(S

\pii-1(S1)0.

This short exact sequence splits because of the suspension homomorphism

\phi\colon\pii(S1)\to

2)
\pi
i(S
and there are isomorphisms:
2)
\pi
i(S

\cong

3)
\pi
i(S

\pii(S1).

The homotopy groups

\pii(S1)

are trivial for

i\geq3,

so there exist isomorphisms between
2)
\pi
i(S
and
3)
\pi
i(S
for

i\geq3.

Analog the fibers

S3

in

S7

and

S7

in

S15

are contractible to a point. Further the short exact sequences split and there are families of isomorphisms:
4)
\pi
i(S

\cong

7)
\pi
i(S

\pii(S3)

and
8)
\pi
i(S

\cong

15
\pi
i(S

)\pii(S7).

Spectral sequence

Spectral sequences are important tools in algebraic topology for computing (co-)homology groups.

The Leray-Serre spectral sequence connects the (co-)homology of the total space and the fiber with the (co-)homology of the base space of a fibration. For a fibration

p\colonE\toB

with fiber

F,

where the base space is a path connected CW-complex, and an additive homology theory

G*

there exists a spectral sequence:

Hk(B;Gq(F))\cong

2
E
k,q

\impliesGk(E).

Fibrations do not yield long exact sequences in homology, as they do in homotopy. But under certain conditions, fibrations provide exact sequences in homology. For a fibration

p\colonE\toB

with fiber

F,

where base space and fiber are path connected, the fundamental group

\pi1(B)

acts trivially on

H*(F)

and in addition the conditions

Hp(B)=0

for

0<p<m

and

Hq(F)=0

for

0<q<n

hold, an exact sequence exists (also known under the name Serre exact sequence):

Hm+n-1(F)\xrightarrow{i*}Hm+n-1(E)\xrightarrow{f*}Hm+n-1(B)\xrightarrow\tauHm+n-2(F)\xrightarrow{i*}\xrightarrow{f*}H1(B)\to0.

This sequence can be used, for example, to prove Hurewicz's theorem or to compute the homology of loopspaces of the form

\OmegaSn:

Hk(\OmegaSn)=\begin{cases}\Z&\existq\in\Z\colonk=q(n-1)\ 0&otherwise\end{cases}.

For the special case of a fibration

p\colonE\toSn

where the base space is a

n

-sphere with fiber

F,

there exist exact sequences (also called Wang sequences) for homology and cohomology:

\toHq(F)\xrightarrow{i*}Hq(E)\toHq-n(F)\toHq-1(F)\to

\toHq(E)\xrightarrow{i*}Hq(F)\toHq-n+1(F)\toHq+1(E)\to

Orientability

For a fibration

p\colonE\toB

with fiber

F

and a fixed commutative ring

R

with a unit, there exists a contravariant functor from the fundamental groupoid of

B

to the category of graded

R

-modules, which assigns to

b\inB

the module

H*(Fb,R)

and to the path class

[\omega]

the homomorphism

h[\omega]*\colonH*(F\omega,R)\toH*(F\omega,R),

where

h[\omega]

is a homotopy class in

[F\omega(0),F\omega].

A fibration is called orientable over

R

if for any closed path

\omega

in

B

the following holds:

h[\omega]*=1.

Euler characteristic

For an orientable fibration

p\colonE\toB

over the field

K

with fiber

F

and path connected base space, the Euler characteristic of the total space is given by:

\chi(E)=\chi(B)\chi(F).

Here the Euler characteristics of the base space and the fiber are defined over the field

K

.

See also