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Section (fiber bundle) : ウィキペディア英語版
Section (fiber bundle)

In the mathematical field of topology, a section (or cross section) of a fiber bundle \pi is a continuous right inverse of the function \pi . In other words, if E is a fiber bundle over a base space, B :
: \pi : E \mapsto B
then a section of that fiber bundle is a continuous map,
: \sigma: B \mapsto E
such that
: \pi(\sigma(x)) = x for all x \in B.
A section is an abstract characterization of what it means to be a graph. The graph of a function g: B \mapsto Y can be identified with a function taking its values in the Cartesian product E = B \times Y , of B and Y :
: \sigma(x) = (x,g(x)) \in E, \ \sigma: B\mapsto E
Let \pi: E \mapsto X be the projection onto the first factor: \pi(x,y) = x . Then a graph is any function \sigma for which \pi(\sigma(x)) = x .
The language of fibre bundles allows this notion of a section to be generalized to the case when ''E'' is not necessarily a Cartesian product. If \pi: E \mapsto B is a fibre bundle, then a section is a choice of point \sigma(x) in each of the fibres. The condition \pi(\sigma(x)) = x simply means that the section at a point x must lie over x . (See image.)
For example, when ''E'' is a vector bundle a section of ''E'' is an element of the vector space ''E''x lying over each point ''x'' ∈ ''B''. In particular, a vector field on a smooth manifold ''M'' is a choice of tangent vector at each point of ''M'': this is a ''section'' of the tangent bundle of ''M''. Likewise, a 1-form on ''M'' is a section of the cotangent bundle.
Sections, particularly of principal bundles and vector bundles, are also very important tools in differential geometry. In this setting, the base space ''B'' is a smooth manifold ''M'', and ''E'' is assumed to be a smooth fiber bundle over ''M'' (i.e., ''E'' is a smooth manifold and ''π'': ''E'' → ''M'' is a smooth map). In this case, one considers the space of smooth sections of ''E'' over an open set ''U'', denoted ''C''(''U'',''E''). It is also useful in geometric analysis to consider spaces of sections with intermediate regularity (e.g., ''C''''k'' sections, or sections with regularity in the sense of Hölder conditions or Sobolev spaces).
== Local and global sections ==

Fiber bundles do not in general have such ''global'' sections (consider, for example, the fiber bundle over ''S''1 with fiber ''F'' = ℝ − obtained by taking the Möbius bundle and removing the zero section), so it is also useful to define sections only locally. A local section of a fiber bundle is a continuous map ''s'' : ''U'' → ''E'' where ''U'' is an open set in ''B'' and ''π''(''s''(''x'')) = ''x'' for all ''x'' in ''U''. If (''U'', ''φ'') is a local trivialization of ''E'', where ''φ'' is a homeomorphism from ''π''−1(''U'') to ''U'' × ''F'' (where ''F'' is the fiber), then local sections always exist over ''U'' in bijective correspondence with continuous maps from ''U'' to ''F''. The (local) sections form a sheaf over ''B'' called the sheaf of sections of ''E''.
The space of continuous sections of a fiber bundle ''E'' over ''U'' is sometimes denoted ''C''(''U'',''E''), while the space of global sections of ''E'' is often denoted Γ(''E'') or Γ(''B'',''E'').

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