adjoint bundle
In mathematics, an adjoint bundle {{harvnb|Kolář|Michor|Slovák|1993||pp=161, 400}} is a vector bundle naturally associated with any smooth principal bundle. The fibers of the adjoint bundle carry a Lie algebra structure making the adjoint bundle into a (nonassociative) algebra bundle. Adjoint bundles have important applications in the theory of connections as well as in gauge theory.
Formal definition
Let G be a Lie group with Lie algebra , and let P be a principal G-bundle over a smooth manifold M. Let
:
be the (left) adjoint representation of G. The adjoint bundle of P is the associated bundle
:
The adjoint bundle is also commonly denoted by . Explicitly, elements of the adjoint bundle are equivalence classes of pairs [p, X] for p ∈ P and X ∈ such that
:
for all g ∈ G. Since the structure group of the adjoint bundle consists of Lie algebra automorphisms, the fibers naturally carry a Lie algebra structure making the adjoint bundle into a bundle of Lie algebras over M.
Restriction to a closed subgroup
Let G be any Lie group with Lie algebra , and let H be a closed subgroup of G.
Via the (left) adjoint representation of G , G becomes a topological transformation group .
By restricting the adjoint representation of G to the subgroup H,
also H acts as a topological transformation group on . For every h in H, is a Lie algebra automorphism.
Since H is a closed subgroup of Lie group G, the homogeneous space M=G/H is the base space of a principal bundle with total space G and structure group H. So the existence of H-valued transition functions is assured, where is an open covering for M, and the transition functions form a cocycle of transition function on M.
The associated fibre bundle is a bundle of Lie algebras, with typical fibre , and a continuous mapping induces on each fibre the Lie bracket.{{citation |first1=B.S. |last1=Kiranagi |title=Lie algebra bundles and Lie rings |journal=Proc. Natl. Acad. Sci. India A |volume=54 |year=1984 |pages=38–44}}
Properties
Differential forms on M with values in are in one-to-one correspondence with horizontal, G-equivariant Lie algebra-valued forms on P. A prime example is the curvature of any connection on P which may be regarded as a 2-form on M with values in .
The space of sections of the adjoint bundle is naturally an (infinite-dimensional) Lie algebra. It may be regarded as the Lie algebra of the infinite-dimensional Lie group of gauge transformations of P which can be thought of as sections of the bundle where conj is the action of G on itself by (left) conjugation.
If is the frame bundle of a vector bundle , then has fibre in the general linear group (either real or complex, depending on ) where . This structure group has Lie algebra consisting of all matrices , and these can be thought of as the endomorphisms of the vector bundle . Indeed, there is a natural isomorphism .
Notes
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References
- {{citation | last1=Kobayashi|first1=Shoshichi|last2=Nomizu|first2=Katsumi | title = Foundations of Differential Geometry|volume=1| publisher=Wiley Interscience | year=1996 |isbn=0-471-15733-3}}
- {{citation|last1=Kolář|first1=Ivan|last2=Michor|first2=Peter|last3=Slovák|first3=Jan |title=Natural operators in differential geometry |url=https://books.google.com/books?id=YQXtCAAAQBAJ&pg=PP1 |year=1993 |publisher=Springer |isbn=978-3-662-02950-3 |pages=161, 400 }}. As [https://web.archive.org/web/20170330154524/http://www.emis.de/monographs/KSM/kmsbookh.pdf PDF]
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