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Path space fibration

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In algebraic topology, the path space fibration over a based space (X, *) is a fibration of the form

where

  • is the space called the path space of X.
  • is the fiber of over the base point of X; thus it is the loop space of X.

The space consists of all maps from I to X that may not preserve the base points; it is called the free path space of X and the fibration given by, say, , is called the free path space fibration.

Mapping path space

If ƒ:XY is any map, then the mapping path space Pƒ of ƒ is the pullback of along ƒ. Since a fibration pullbacks to a fibration, if Y is based, one has the fibration

where and is the homotopy fiber, the pullback of along ƒ.

Note also ƒ is the composition

where the first map φ sends x to , the constant path with value ƒ(x). Clearly, φ is a homotopy equivalence; thus, the above decomposition says that any map is a fibration up to homotopy equivalence.

If ƒ is a fibration to begin with, then is a fiber-homotopy equivalence and, consequently,[1] the fibers of f over the path-component of the base point are homotopy equivalent to the homotopy fiber of ƒ.

Moore's path space

By definition, a path in a space X is a map from the unit interval I to X. Again by definition, the product of two paths α, β such that α(1) = β(0) is the path β · α: IX given by:

.

This product, in general, fails to be associative on the nose: (γ · β) · αγ · (β · α), as seen directly. One solution to this failure is to pass to homotopy classes: one has [(γ · β) · α ] = [γ · (β · α)]. Another solution is to work with paths of varying length, leading to the notion of Moore's path space and Moore's path space fibration.[2]

Given a based space (X, *), we let

An element f of this set has the unique extension to the interval such that . Thus, the set can be identified as a subspace of . The resulting space is called Moore's path space of X. Then, just as before, there is a fibration, Moore's path space fibration:

where p sends each f: [0, r] → X to f(r) and is the fiber. It turns out that and are homotopy equivalent.

Now, we define the product map:

by: for and ,

.

This product is manifestly associative. In particular, with μ restricted to Ω'X × Ω'X, we have that Ω'X is a topological monoid (in the category of all spaces). Moreover, this monoid Ω'X acts on P'X through the original μ.

Notes

  1. ^ using the change of fiber
  2. ^ Whitehead 1979, Ch. III, § 2.

References

  • James F. Davis, Paul Kirk, Lecture Notes in Algebraic Topology
  • May, J. A Concise Course in Algebraic Topology
  • George William Whitehead (1978). Elements of homotopy theory. Graduate Texts in Mathematics. Vol. 61 (3rd ed.). New York-Berlin: Springer-Verlag. pp. xxi+744. ISBN 978-0-387-90336-1. MR 0516508. Retrieved September 6, 2011.