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Thursday, June 7, 2018

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In differential geometry, the tensor product of vector bundles E, F is a vector bundle, denoted by E ? F, whose fiber over a point x is the tensor product of vector spaces Ex ? Fx.

Example: If O is a trivial line bundle, then E ? O = E for any E.

Example: E ? E * is canonically isomorphic to the endomorphism bundle End(E), where E * is the dual bundle of E.

Example: A line bundle L has tensor inverse: in fact, L ? L * is (isomorphic to) a trivial bundle by the previous example, as End(L) is trivial. Thus, the set of the isomorphism classes of all line bundles on some topological space X forms an abelian group called the Picard group of X.


Video Tensor product bundle



Variants

One can also define a symmetric power and an exterior power of a vector bundle in a similar way. For example, a section of ? p T * M {\displaystyle \Lambda ^{p}T^{*}M} is a differential p-form and a section of ? p T * M ? E {\displaystyle \Lambda ^{p}T^{*}M\otimes E} is a differential p-form with values in a vector bundle E.


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See also

  • tensor product of modules

Braided noncommutative join construction - MediaServer der ...
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Notes


Tensor space theory II: over a ring - Lec 11 - Frederic Schuller ...
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References

  • Hatcher, Vector Bundles and K-Theory

Source of article : Wikipedia