Principal SU(2)-bundle

In mathematics, especially differential geometry, principal -bundles (or principal -bundles) are special principal bundles with the second special unitary group (isomorphic to the first symplectic group ) as structure group. Topologically, it has the structure of the three-dimensional sphere, hence principal -bundles without their group action are in particular sphere bundles. These are basically topological spaces with a sphere glued to every point, so that all of them are connected with each other, but globally aren't necessarily a product and can instead be twisted like a Möbius strip.

Principal -bundles are used in many areas of mathematics, for example for the Fields Medal winning proof of Donaldson's theorem[1][2] or instanton Floer homology. Since is the gauge group of the weak interaction, principal -bundles are also of interest in theoretical physics. In particular, principal -bundles over the four-dimensional sphere , which include the quaternionic Hopf fibration, can be used to describe hypothetical magnetic monopoles in five dimensions, known as Wu–Yang monopoles, see also four-dimensional Yang–Mills theory.

Definition

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Principal  -bundles are generalizations of canonical projections   for topological spaces  , so that the source is not globally a product but only locally. More concretely, a continuous map  with a continuous right group action  , which preserves all preimages of points, hence   for all   and  , and also acts free and transitive on all preimages of points, which makes all of them homeomorphic to  , is a principal  -bundle.[3][4]

Since principal bundles are in particular fiber bundles with the group action missing, their nomenclature can be transferred.   is also called the total space and   is also called the base space. Preimages of points are then the fibers. Since   is a Lie group, hence in particular a smooth manifold, the base space   is often chosen to be a smooth manifold as well since this automatically makes the total space   into a smooth manifold as well.

Classification

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Principal  -bundles can be fully classified using the classifying space   of the second special unitary group  , which is exactly the infinite quaternionic projective space  . For a topological space  , let   denote the set of equivalence classes of principal  -bundles over it, then there is a bijection with homotopy classes:[5]

 

  is a CW complex with its  -skeleton being   for the largest natural number   with  .[6] For a  -dimensional CW complex  , the cellular approximation theorem[7] states that every continuous map   is homotopic to a cellular map factoring over the canonical inclusion  . As a result, the induced map   is surjective, but not necessarily injective as higher cells of   allow additional homotopies. In particular if   is a CW complex of seven or less dimensions, then   and with  , there is a connection to cohomotopy sets with a surjective map:

 

If   is a 4-manifold, then injectivity and therefore bijectivity holds since all homotopies can be shifted into the  -skeleton   of  . If   is a 5-manifold, this is no longer holds due to possible torsion in cohomology.[8]

  is the rationalized Eilenberg–MacLane space   under rationalization, but itself not the Eilenberg–MacLane space  ,[9] which represents singular cohomology,[10] compare to Brown's representability theorem. But from the Postnikov tower,[11] there is a canonical map   and therefore by postcomposition a canonical map:

 

(The composition   is the Hurewicz map.) A corresponding map is given by the second Chern class. If   is again a 4-manifold, then the classification is unique.[12] Although characteristic classes are defined for vector bundles, it is possible to also define them for certain principal bundles.

Associated vector bundle

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Given a principal  -bundle  , there is an associated vector bundle  . Intuitively, the spheres at every point are filled over the canonical inclusions  .

Since the determinant is constant on special unitary matrices, the determinant line bundle of this vector bundle is classified by a constant map and hence trivial. Since the determinant preserves the first Chern class, it is always trivial. Therefore the vector bundle is only described by the second Chern class  .

Since there is a canonical inclusion  , every principal  -bundle   can be associated a principal  -bundle  . If   is the associated complex line bundle of  , then   is the associated complex plane bundle of  , exactly as claimed by the canonical inclusion. Hence the Chern classes of   are given by:[13][14]

 
 

If   is a principal  -bundle over a CW complex   with   and   for a singular cohomology class  , then there exists a principal  -bundle   with   since the first Chern class of principal  -bundle over CW complexes is an isomorphism.[15] Hence   and   have identical Chern classes. If   is a 4-manifold, then both principal  -bundles are isomorphic due to the unique classification by the second Chern class.[8][16]

Adjoint vector bundle

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For the associated vector bundle, it is necessary that   is a matrix Lie group. But there is also the adjoint vector bundle, for which this is not necessary, since it uses the always existing adjoint representation   with induced map  . In fact, the adjoint representation is even the double cover  .[17] For a principal  -bundle   with classifying map   with  , the adjoint vector bundle is given by:

 

Since it has a spin structure as just described, its first and second Stiefel–Whitney classes vanish. Its first Pontrjagin class is given by:[17]

 

Unlike the associated vector bundle, a complex plane bundle, the adjoint vector bundle is a orientable real vector bundle of third rank. Also since   acts by simple multiplication on the former and by conjugation on the latter, the vector bundles can't be compared. An application of the adjoint vector bundle is on connections or more generally Lie algebra valued differential forms on the principal  -bundle:

 

Examples

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  • By definition of quaternionic projective space, the canonical projection  is a principal  -bundle. With   the quaternionic Hopf fibration   is a special case. For the general case, the classifying map is the canonical inclusion:
 
  • One has  , which means that there is a principal  -bundle  . Such bundles are classified by:[18]
 
  is the non-trivial one, which can for example be detected by the fourth homotopy group:
 [19][20]
 
  • One has  , which means that (using  ) there is a principal  -bundle  . Such bundles are classified by:[18]
 

See also

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Literature

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  • Donaldson, Simon (1983). "An application of gauge theory to four-dimensional topology". Journal of Differential Geometry. 18 (2). doi:10.4310/jdg/1214437665.
  • Donaldson, Simon (1987). "The orientation of Yang-Mills moduli spaces and 4-manifold topology". Journal of Differential Geometry. 26 (3). doi:10.4310/jdg/1214441485.
  • Freed, Daniel (1991). Instantons and 4-Manifolds. Cambridge University Press. ISBN 978-1-4613-9705-2.
  • Hatcher, Allen (2001). Algebraic Topology. Cambridge University Press. ISBN 0-521-79160-X.
  • Mitchell, Stephen (2011). "Notes on principal bundles and classifying spaces" (PDF).
  • Hatcher, Allen (2017). Vector Bundles and K-Theory (PDF).

References

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  1. ^ Donaldson 1983
  2. ^ Donaldson 1987
  3. ^ Freed & Uhlenbeck 1984, p. 29
  4. ^ Mitchell 2001, p. 2
  5. ^ Mitchell 2011, Theorem 7.4
  6. ^ Hatcher 2001, p. 222
  7. ^ Hatcher 2001, Theorem 4.8.
  8. ^ a b Freed & Uhlenbeck 1984, Theorem E.5.
  9. ^ Hatcher 2001, Example 4.50.
  10. ^ Hatcher 2001, Theorem 4.57.
  11. ^ Hatcher 2001, p. 410
  12. ^ Donaldson 1983, p. 282
  13. ^ Donaldson 1983, p. 287
  14. ^ Freed & Uhlenbeck 1984, p. 34
  15. ^ Hatcher 2017, Proposition 3.10.
  16. ^ Freed & Uhlenbeck 1984, Proposition 2.11.
  17. ^ a b Freed & Uhlenbeck 1984, p. 180
  18. ^ a b Mitchell 2011, Corollary 11.2
  19. ^ Mimura, Mamoru; Toda, Hiroshi (1963). "Homotopy Groups of SU(3), SU(4) and Sp(2)". Journal of Mathematics of Kyoto University. 3 (2): 217–250. doi:10.1215/kjm/1250524818.
  20. ^ Donaldson 1983, p. 295
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