For clarification, we begin our exposition with a motivating example. A tangent bundle over an -dimensional manifold is a collection of all the tangent spaces of :

The manifold over which is defined is called the base space. Let be an open covering of . If is the coordinate on , an element of

is specified by a point and a vector . Noting that is homeomorphic to an open subset of and each is homeomorphic to , we find that is identified with a direct product (figure 9.1). If , the identification is given by . is a 2m-dimensional differentiable manifold. What is more, is decomposed into a direct product . If we pick up a point of , we can systematically decompose the information contains into a point and a vector . Thus, we are naturally led to the concept of projection (figure 9.1). For any point , is a point at which the vector is defined. The information about the vector

Figure 9.1. A local piece of a tangent bundle . The projection projects a vector to .

is completely lost under the projection. Observe that . In the context of the theory of fibre bundles, is called the fibre at .

It is obvious by construction that if , the tangent bundle itself is expressed as a direct product . However, this is not always the case and the non-trivial structure of the tangent bundle measures the topological nontriviality of . To see this, we have to look not only at a single chart but also at other charts. Let be a chart such that and let be the coordinates on . Take a vector where . has two coordinate presentations,

It is easy to see that they are related as

For and to be good coordinate systems, the matrix must be non-singular: . Thus, fibre coordinates are rotated by an element of whenever we change the coordinates. The group is called the structure group of . In this way fibres are interwoven together to form a tangent bundle, which consequently may have quite a complicated topological structure.

We note en passant that the projection can be defined globally on . It is obvious that does not depend on a special coordinate chosen. Thus, is defined globally with no reference to local charts.

Let be a vector field on . assigns a vector at each point . From our viewpoint, is looked upon as a smooth map . This map is not utterly arbitrary since a point must be mapped to a point such that . We define a section (or a cross section) of as a smooth map such that . If a section is defined only on a chart , it is called a local section.

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正文:英文 · OCR 机器稿 · 待校对

核对状态:OCR 机器稿 · 待校对

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来源版本:second-edition-local

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