Abstract
Given a map p from a space E onto a space B, we can partition the domain into disjoint sets F b = p ā1 (b), for b ā B. (Recall that p ā1(b) is the inverse image of b, that is, the set of points of E that are mapped to b.) We say that p defines a fibration if all the sets F b are homeomorphic to one another. In this case F b is called the fiber over b; the space B is called the base space of the fibration, E is the total space, and p is the projection. If the fibers of a fibration are homeomorphic to a space F, we say that F is the model fiber, or simply the fiber. A fibration with total space E, base space B, fiber F and projection p is denoted by (E,B,F,p), or simply by (E,B,F).
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Ā© 1994 Springer-Verlag Berlin Heidelberg
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Schwarz, A.S. (1994). Fibered Spaces. In: Topology for Physicists. Grundlehren der mathematischen Wissenschaften, vol 308. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-02998-5_10
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DOI: https://doi.org/10.1007/978-3-662-02998-5_10
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-642-08131-6
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