nLab principal SO(3)-bundle

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Context

Bundles

bundles

Cohomology

cohomology

Special and general types

Special notions

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Extra structure

Operations

Theorems

Contents

Idea

Principal SO(3)-bundles are principal bundles with the third special orthogonal group SO ( 3 ) SO(3) as structure group/gauge group. Applications include the frame bundle of an orientable 3-manifold as well as the (anti) self-dual bundles Λ ± 2TX\Lambda_\pm^2T X for an orientable Riemannian 4-manifold XX, resulting from the splitting 𝔰𝔬(4)𝔰𝔬(3)𝔰𝔬(3)\mathfrak{so}(4)\cong\mathfrak{so}(3)\oplus\mathfrak{so}(3).

Principal SO(3)SO(3)-bundles are in particular induced by principal SU(2)-bundles using the double cover SU(2)Spin(3)SO(3)SU(2)\cong Spin(3)\twoheadrightarrow SO(3) and principal U(2)-bundles using the canonical projection U(2)Spin c(3)Spin h(2)SO(3)U(2)\cong Spin^\mathrm{c}(3)\cong Spin^\mathrm{h}(2)\rightarrow SO(3). In fact the latter example generalizes to every Spin h(n)Spin^\mathrm{h}(n)-bundle using the double cover of the former example:

Spin h(n)(Spin(n)×SU(2))/ 2SU(2)/ 2SO(3). Spin^\mathrm{h}(n) \cong(Spin(n)\times SU(2))/\mathbb{Z}_2 \rightarrow SU(2)/\mathbb{Z}_2 \cong SO(3).

Principal SO(3)-bundles also induce principal SO(2)-bundles and are induced by principal SO(4)-bundles and principal SO(6)-bundles using the canonical inclusions SO(2)SO(3)SO(4)SO(6)SO(2)\hookrightarrow SO(3)\hookrightarrow SO(4)\hookrightarrow SO(6).

Principal SO(3)-bundles also arise from any principal GG-bundle with a three-dimensional real Lie group GG using its adjoint representation Ad:GSL 3()Ad\colon G\rightarrow SL_3(\mathbb{R}), which induces a map Ad:GBSO(3)\mathcal{B}Ad\colon\mathcal{B}G\rightarrow B SO(3).

Characteristic classes

Proposition

A principal SO(3)-bundle PP fulfills:

w 2 2(P)p 1(P)mod2. w_2^2(P) \equiv p_1(P) \mod 2.

(In general, a principal SO(n)SO(n)-bundle PP fulfills w 2k 2(P)p k(P)mod2w_{2k}^2(P)\equiv p_k(P) \mod 2 for 2kn2k\leq n.)

(Milnor & Stasheff 74, Prob. 15-A, Gompf & Stipsicz 99, Ex. 1.4.21 d, Hatcher 17, Prop. 3.15 a)

Proposition

A principal SO(3)-bundle PP fulfills:

w 3(P)e(P)mod2. w_3(P) \equiv e(P) \mod 2.

(In general, a principal SO(n)SO(n)-bundle PP fulfills w n(P)e(P)mod2w_n(P)\equiv e(P) \mod 2.)

(Milnor & Stasheff 74, Prop. 9.5, Hatcher 17, Prop. 3.13 c)

Proposition

A principal SO(3)-bundle PP fulfills:

e(P)=W 3(P)=βw 2(P). e(P) =W_3(P) =\beta w_2(P).

with the third integral Stiefel-Whitney class and the Bockstein homomorphism β:H 2(M, 2)H 3(M,)\beta\colon H^2(M,\mathbb{Z}_2)\rightarrow H^3(M,\mathbb{Z}) of the short exact sequence 0 200\rightarrow\mathbb{Z}\hookrightarrow\mathbb{Z}\twoheadrightarrow\mathbb{Z}_2\rightarrow 0. (In general, a principal SO(2n+1)SO(2n+1)-bundle PP fulfills e(P)=W 2n+1(P)=βw 2n(P)e(P)=W_{2n+1}(P)=\beta w_{2n}(P).)

(Milnor & Stasheff 74, Prob. 15-D, Hatcher 17, Ch. 3, Ex. 3)

Classification over 4-manifolds by characteristic classes

Proposition

Let XX be a 4-manifold. Two principal SO(3)-bundles P,QXP,Q\twoheadrightarrow X are isomorphic if and only if their second Stiefel-Whitney class and first Pontrjagin class are equal:

w 2(P)=w 2(Q)H 2(X, 2); w_2(P) =w_2(Q) \in H^2(X,\mathbb{Z}_2);
p 1(P)=p 1(Q)H 4(X,). p_1(P) =p_1(Q) \in H^4(X,\mathbb{Z}).

(But the classes are not independent from each other according to the previous proposition.)

(Dold & Whitney 59, Thrm. 1 a, Gompf & Stipsicz 99, Thrm. 1.4.20)

Certain 4-manifolds yield simplifcations when the singular cohomology groups vanish. For example, for principal SO(3)-bundles over the 4-sphere the second singular cohomology vanishes and therefore the condition of equal second Stiefel-Whitney classes becomes trivial. In this case one has a group isomorphism:

p 1:π 4BSO(3)π 3SO(3). p_1\colon \pi_4 B SO(3) \cong\pi_3 SO(3) \xrightarrow\cong\mathbb{Z}.

An abstract way to obtain this group isomorphism is the exceptional isomorphism Spin(3)SU(2)S 3Spin(3)\cong SU(2)\cong S^3, which double covers SO(3)SO(3) and therefore has the same higher homotopy groups (beyond the fundamental group). Therefore π 3SO(3)π 3(S 3)\pi_3 SO(3)\cong\pi_3(S^3)\cong\mathbb{Z}. (Just the result is also stated in Dold & Whitney 59, Eq. (2).)

Proposition

Let XX be a 44-manifold. For every (w 2,p 1)H 2(X, 2)×H 4(X,)(w_2,p_1)\in H^2(X,\mathbb{Z}_2)\times H^4(X,\mathbb{Z}) with p 1=Pont(w 2)mod4p_1=Pont(w_2) \mod 4, there exists a principal SO(3)-bundle PXP\twoheadrightarrow X with w 2(P)=w 2w_2(P)=w_2 and p 1(P)=p 1p_1(P)=p_1.

(Gompf & Stipsicz 99, Thrm. 1.4.20)

Liftings

Proposition

A principal SO(3)-bundle f:XBSO(3)f\colon X\rightarrow B SO(3) lifts to a principal SU(2)-bundle f^:XBSU(2)P \widehat{f}\colon X\rightarrow B SU(2)\cong\mathbb{H}P^\infty if and only if its second Stiefel-Whitney class vanishes, hence the composition w 2f:XK( 2,2)w_2\circ f\colon X\rightarrow K(\mathbb{Z}_2,2) is nullhomotopic.

Let PP be a principal SU(2)SU(2)-bundle and QQ be the associated principal SO(3)SO(3)-bundle. One then has:

p 1(Q)=p 1Ad(P)=4c 2(P); p_1(Q) =p_1 Ad(P) =-4c_2(P);
w 2(Q)=w 2Ad(P)=0. w_2(Q) =w_2Ad(P) =0.

(Uhlenbeck & Freed 91, Appendix E.6)

Proposition

A principal SO(3)-bundle f:XBSO(3)f\colon X\rightarrow B SO(3) lifts to a principal U(2)-bundle f^:XBU(2)\widehat{f}\colon X\rightarrow B U(2) if and only if its third integral Stiefel-Whitney class vanishes, hence the composition W 3f:XK(,2)W_3\circ f\colon X\rightarrow K(\mathbb{Z},2) is nullhomotopic. If the second Stiefel-Whitney class w 2f:XK( 2,2)w_2\circ f\colon X\rightarrow K(\mathbb{Z}_2,2) lifts to an integral class c:XK(,2)c\colon X\rightarrow K(\mathbb{Z},2), then it is exactly the first Chern class of the lift with c 1f^=cc_1\circ\widehat{f}=c.

(Donaldson & Kronheimer 91, p. 42)

In the situation of this lemma, it is often more useful to consider the exceptional isomorphism SO(3)PU(2)SO(3)\cong PU(2) to the projective unitary group.

(Anti) self-dual bundles

Using the exceptional isomorphisms Spin(3)SU(2)Spin(3)\cong SU(2) and Spin(4)SU(2)×SU(2)Spin(4)\cong SU(2)\times SU(2), matrices in SO(3) and SO(4) can be represented by matrices in SU(2). In particular there are maps:

ϕ:SO(3)SO(4)[U][(U,U)]; \phi\colon SO(3)\rightarrow SO(4) [U]\mapsto[(U,U)];
ψ :SO(4)SO(3),[(U ,U +)][U ]; \psi_-\colon SO(4)\rightarrow SO(3), [(U_-,U_+)]\mapsto[U_-];
ψ +:SO(4)SO(3),[(U ,U +)][U +] \psi_+\colon SO(4)\rightarrow SO(3), [(U_-,U_+)]\mapsto[U_+]

with ψ ±ϕ=id\psi_\pm\circ\phi=id and so that there is a Lie algebra isomorphism:

(ψ ,ψ +):𝔰𝔬(4)𝔰𝔬(3)𝔰𝔬(3) (\psi_-',\psi_+')\colon \mathfrak{so}(4)\xrightarrow\cong\mathfrak{so}(3)\oplus\mathfrak{so}(3)

Proposition

For an orientable Riemannian 4-manifold XX, one has Λ ± 2TX=(ψ ±) *TX\Lambda_\pm^2T X=(\psi_\pm)_*T X with characteristic classes:

w 2(Λ + 2TX)=w 2(X); w_2(\Lambda_+^2T X) =w_2(X);
p 1(Λ + 2TX)=p 1(X)+2e(X). p_1(\Lambda_+^2T X) =p_1(X) +2e(X).

(Gompf & Stipsicz 99, Thrm. 1.4.20)

According to the first equation, Λ + 2TX\Lambda_+^2T X lifts to a principal SU(2)-bundle if and only if TXT X lifts to a pair of principal SU(2)-bundles (being Spin(3)Spin(3) and Spin(4)Spin(4) structures repsectively). Or just taking the weaker implied equality of the third integral Stiefel-Whitney classes, Λ + 2TX\Lambda_+^2T X lifts to a principal U(2)-bundle if and only if TXT X lifts to a pair of principal U(2)-bundles with same first Chern class (being Spin c(3)Spin^\mathrm{c}(3) and Spin c(4)Spin^\mathrm{c}(4) structures respectively).

According to the second equation, using the fundamental class [X]H 4(X,)[X]\in H_4(X,\mathbb{Z})\cong\mathbb{Z} induced by the orientation as well as Hirzebruch's signature theorem, one has:

p 1(Λ + 2TX),[X]=p 1(X),[X]+2e(X),[X]=3σ(X)+2χ(X) \big\langle p_1(\Lambda_+^2T X),[X]\big\rangle =\big\langle p_1(X),[X]\big\rangle +2\big\langle e(X),[X]\big\rangle =3\sigma(X) +2\chi(X)

This expression appears both in the virtual dimension of the Seiberg-Witten moduli space (Gompf & Stipsicz 99, Thrm. 2.4.24) and Noether’s formula for almost complex structures. (Gompf & Stipsicz 99, Thrm. 1.4.15)

Examples

  • One has S nSO(n+1)/SO(n)S^n\cong SO(n+1)/SO(n), hence there is a principal SO(3)-bundle SO(4)S 3SO(4)\twoheadrightarrow S^3. Such principal bundles are classified by:
    π 3BSO(3)π 2SO(3)1. \pi_3B SO(3) \cong\pi_2 SO(3) \cong 1.

    Hence the bundle is trivial and SO(4)SO(3)×S 7SO(4)\cong SO(3)\times S^7.

Application in Yang-Mills theory

Proposition

Reducible anti self-dual Yang-Mills connections of a principal SO(3)SO(3)-bundle EE over a compact, simply connected, oriented Riemannian 4-manifold XX are in bijective correspondence with non-zero pairs ±cH 2(X,)\pm c\in H^2(X,\mathbb{Z}) with c 2=p 1(E)c^2=p_1(E).

(Donaldson & Kronheimer 97, Prop. (4.2.15))

Proposition

Irreducible anti self-dual Yang-Mills connections of a principal SO(3)SO(3)-bundle EE over a simply connected Riemannian 4-manifold XX are still irreducible under the restriction to any non-empty open subset.

(Donaldson & Kronheimer 97, Lem. (4.3.21))

Particular principal bundles:

References

Last revised on March 12, 2026 at 13:16:43. See the history of this page for a list of all contributions to it.