Principal SU(2)-bundle

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Template:Short description In mathematics, especially differential geometry, principal SU⁡(2)-bundles (or principal Sp⁡(1)-bundles) are special principal bundles with the second special unitary group SU⁡(2) (isomorphic to the first symplectic group Sp⁡(1)) as structure group. Topologically, it has the structure of the three-dimensional sphere, hence principal SU⁡(2)-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 SU⁡(2)-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 SU⁡(2) is the gauge group of the weak interaction, principal SU⁡(2)-bundles are also of interest in theoretical physics. In particular, principal SU⁡(2)-bundles over the four-dimensional sphere S4, 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

Principal SU⁡(2)-bundles are generalizations of canonical projections B×SU⁡(2)↠B for topological spaces B, so that the source is not globally a product but only locally. More concretely, a continuous map p:E↠B with a continuous right group action E×SU⁡(2)→E, which preserves all preimages of points, hence p(eg)=p(e) for all e∈E and g∈SU⁡(2), and also acts free and transitive on all preimages of points, which makes all of them homeomorphic to SU⁡(2), is a principal SU⁡(2)-bundle.[3][4]

Since principal bundles are in particular fiber bundles with the group action missing, their nomenclature can be transferred. E is also called the total space and B is also called the base space. Preimages of points are then the fibers. Since SU⁡(2) is a Lie group, hence in particular a smooth manifold, the base space B is often chosen to be a smooth manifold as well since this automatically makes the total space E into a smooth manifold as well.

Classification

Principal SU⁡(2)-bundles can be fully classified using the classifying space BSU⁡(2) of the second special unitary group SU⁡(2), which is exactly the infinite quaternionic projective space ℍP∞. For a topological space B, let PrinSU⁡(2)(B) denote the set of equivalence classes of principal SU⁡(2)-bundles over it, then there is a bijection with homotopy classes:[5]

PrinSU⁡(2)(B)≅[B,BSU⁡(2)]≅[B,ℍP∞].

ℍP∞ is a CW complex with its n-skeleton being ℍPk for the largest natural number k∈ℕ with 4k≤n.[6] For a n-dimensional CW complex B, the cellular approximation theorem[7] states that every continuous map B→ℍP∞ is homotopic to a cellular map factoring over the canonical inclusion ℍPk↪ℍP∞. As a result, the induced map [B,ℍPk]↪[B,ℍP∞] is surjective, but not necessarily injective as higher cells of ℍP∞ allow additional homotopies. In particular if B is a CW complex of seven or less dimensions, then k=1 and with ℍP1≅S4, there is a connection to cohomotopy sets with a surjective map:

π4(B)→PrinSU⁡(2)(B).

If B is a 4-manifold, then injectivity and therefore bijectivity holds since all homotopies can be shifted into the 5-skeleton S4 of ℍP∞. If B is a 5-manifold, this is no longer holds due to possible torsion in cohomology.[8]

ℍP∞ is the rationalized Eilenberg–MacLane space K(ℤ,4)ℚ under rationalization, but itself not the Eilenberg–MacLane space K(ℤ,4),[9] which represents singular cohomology,[10] compare to Brown's representability theorem. But from the Postnikov tower,[11] there is a canonical map ℍP∞→K(ℤ,4) and therefore by postcomposition a canonical map:

PrinSU⁡(2)(B)→H4(B,ℤ).

(The composition π4(B)→H4(B,ℤ) is the Hurewicz map.) A corresponding map is given by the second Chern class. If B 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

Given a principal SU⁡(2)-bundle E↠B, there is an associated vector bundle E×SU⁡(2)ℂ2↠B. Intuitively, the spheres at every point are filled over the canonical inclusions SU⁡(2)⊂ℂ2.

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 c2:Vectℂ(B)→H4(B,ℤ).

Since there is a canonical inclusion U⁡(1)↪SU⁡(2),z↦diag⁡(z,z−1), every principal U⁡(1)-bundle E↠B can be associated a principal SU⁡(2)-bundle E^↠B. If L=E×U⁡(1)ℂ is the associated complex line bundle of E, then L⊕L−1=E^×SU⁡(2)ℂ2 is the associated complex plane bundle of E^, exactly as claimed by the canonical inclusion. Hence the Chern classes of E^ are given by:[13][14]

c1(E^)=c1(L⊕L−1)=c1(L)+c1(L−1)=0;
c2(E^)=c2(L⊕L−1)=c2(L)+c2(L−1)+c1(L)c1(L−1)=−c1(L)2=−c1(E)2.

If E↠B is a principal SU⁡(2)-bundle over a CW complex B with c1(F)=0 and c2(F)=−c2 for a singular cohomology class c∈H2(B,ℤ), then there exists a principal U⁡(1)-bundle E↠B with c1(E)=c since the first Chern class of principal U⁡(1)-bundle over CW complexes is an isomorphism.[15] Hence E^ and F have identical Chern classes. If B is a 4-manifold, then both principal SU⁡(2)-bundles are isomorphic due to the unique classification by the second Chern class.[8][16]

Adjoint vector bundle

For the associated vector bundle, it is necessary that SU⁡(2) 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 Ad⁡:SU⁡(2)→Aut⁡(𝔰𝔲(2))≅SL3(ℝ) with induced map ℬAd⁡:BSU⁡(2)→BSL3(ℝ)≅BSO⁡(3). In fact, the adjoint representation is even the double cover SU⁡(2)≅Spin⁡(3)→SO⁡(3).[17] For a principal SU⁡(2)-bundle E↠B with classifying map f:B→BSU⁡(2) with E≅f∗ESU⁡(2), the adjoint vector bundle is given by:

Ad⁡(E):=E×SU⁡(2)𝔰𝔲(2)=(ℬAd⁡∘f)∗γℝ3

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]

p1(Ad⁡(E))=−4c2(E)∈H4(B,ℤ).

Unlike the associated vector bundle, a complex plane bundle, the adjoint vector bundle is a orientable real vector bundle of third rank. Also since SU⁡(2) 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 SU⁡(2)-bundle:

ΩAdk(E,𝔰𝔲(2))≅Ωk(B,Ad⁡(E))

Examples

  • By definition of quaternionic projective space, the canonical projection S4n+3↠ℍPnis a principal SU⁡(2)-bundle. With ℍP1≅S4 the quaternionic Hopf fibration hℍ:S7↠S4 is a special case. For the general case, the classifying map is the canonical inclusion:
ℍPn↪ℍP∞≅BSU⁡(2).
  • One has S2n+1≅SU⁡(n+1)/SU⁡(n), which means that there is a principal SU⁡(2)-bundle SU⁡(3)↠S5. Such bundles are classified by:[18]
π5BSU⁡(2)≅π4SU⁡(2)≅π4S3≅ℤ2.
SU⁡(3)↠S5 is the non-trivial one, which can for example be detected by the fourth homotopy group:
π4SU⁡(3)≅1,[19][20]
π4(S5×SU⁡(2))≅π4(S5)×π4(S3)≅ℤ2.
  • One has S4n+3≅Sp⁡(n+1)/Sp⁡(n), which means that (using SU⁡(2)≅Sp⁡(1)) there is a principal SU⁡(2)-bundle Sp⁡(2)↠S7. Such bundles are classified by:[18]
π7BSU⁡(2)≅π6SU⁡(2)≅π6S3≅ℤ12.

See also

Literature

References

  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. ↑ 8.0 8.1 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. ↑ 17.0 17.1 Freed & Uhlenbeck 1984, p. 180
  18. ↑ 18.0 18.1 Mitchell 2011, Corollary 11.2
  19. ↑ Template:Cite journal
  20. ↑ Donaldson 1983, p. 295