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Fibration

Concept in algebraic topology

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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:E→B satisfies the homotopy lifting property for a space X if:

  • for every homotopy h:X×[0,1]→B and
  • for every mapping (also called lift) h~0:X→E lifting h|X×0=h0 (i.e. h0=p∘h~0)

there exists a (not necessarily unique) homotopy h~:X×[0,1]→E lifting h (i.e. h=p∘h~) with h~0=h~|X×0.

The following commutative diagram shows the situation:

Fibration

A fibration (also called Hurewicz fibration) is a mapping p:E→B satisfying the homotopy lifting property for all spaces X. The space B is called the base space and the space E is called the total space. The fiber over b∈B is the subspace Fb=p−1(b)⊆E.

Serre fibration

A Serre fibration (also called weak fibration) is a mapping p:E→B satisfying the homotopy lifting property for all CW-complexes.

Every Hurewicz fibration is a Serre fibration.

Quasifibration

A mapping p:E→B is called quasifibration, if for every b∈B, e∈p−1(b) and i≥0 holds that the induced mapping p∗:πi(E,p−1(b),e)→πi(B,b) is an isomorphism.

Every Serre fibration is a quasifibration.

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