I'm currently considering principal bundles and classifying spaces in the context of gauge theory and a crucial question came to my mind:

Is there a way to say how many (isomorphism classes of) principal bundles there are over a given base space?

For finite gauge groups the answer is yes: They correspond to elements of $\mathrm{Hom}(\pi_1(M),G)/G$ (where $M$ is the base and $G$ the gauge group). Is there a similar characterization for arbitrary compact Lie groups $G$?

  • $\begingroup$ If you are happy with the kind of characterization that you mention, then the answer is: the number of elements of $[M,BG]$, which the set of homotopy-classes of maps from $M$ into the classifying space $B G$ for G-principal bundles. See ncatlab.org/nlab/show/classifying+space $\endgroup$ Jul 19, 2013 at 12:04
  • $\begingroup$ Unfortunately that's not quite enough for me. I was looking for some kind of algebraic characterization maybe similar to the case of a finite gauge group. $\endgroup$
    – Frank
    Jul 19, 2013 at 12:46
  • $\begingroup$ Notice that this is similar to the case of finite gauge groups: if G is discrete then maps $X \to BG$ are the same as maps $\pi_1(X) \to G$ and the notion of homotopy translates. One thing to realize is that also $Hom(\pi(X),G)/G$ is less trivial than it may seem. It's a moduli space of flat connections, which harbours some non-trivial theory, see ncatlab.org/nlab/show/moduli+space+of+connections $\endgroup$ Jul 19, 2013 at 13:15
  • $\begingroup$ But if you want a hands-on algebraic construction of principal bundles, then you want their description by Cech cocycles ncatlab.org/nlab/show/… . Principal bundles on paracompact spaces can be built and classified like this: choose an open cover of the base manifold which is "good" in that all finite intersections of any of its patches are contractible. Then a Cech cocycle is defined by assigning a G-valued function $g_{i j}$ on the overlap of patch $i$ and$j$, such that on all triple overlaps these functions satisfy the cocycle relation... $\endgroup$ Jul 19, 2013 at 13:22
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    $\begingroup$ Urs Schreiber: all these characterizations are very important theoretically but they hardly help answer how many bundels are there, e.g. how does one decide when there are only finitely many $O(n)$-bundles over a given base? What is an estimate for that finite number? $\endgroup$ Jul 19, 2013 at 13:31

2 Answers 2


If $G$ is a connected compact Lie group and the base $M$ is homotopy equivalent to a finite cell complex, then a rough count of the set $[M, BG]$ is given by the rational homotopy theory. The point is that the classifying space $BG$ is rationally homotopy equivalent to the product of Eilenberg-MacLane spaces, e.g.

  1. for $G=U(n)$ each Eilenberg-MacLane space corresponds to the Chern class.

  2. for $G=SO(n)$ each Eilenberg-Maclane space corresponds to Pontryagin or Euler class.

For example, it follows that up to finite ambiguity a principal $U(n)$-bundles over $M$ is determined by its rational Chern classes, and conversely a multiple of any element in $\oplus_{i=1}^n H^{2i}(M;\mathbb Z)$ is realized as the collection of Chern classes of a principle $U(n)$-bundle over $M$.

One standard example (going back to Serre) is that there are only finitely many principal $G$-bundles over an odd-dimensional sphere (because it has no even-dimensional rational cohomology).

Another example is when $G=U(1)$. Then $[M, BU(1)]=[M, K(2, \mathbb Z)]$ which is bijective to $H^2(M;\mathbb Z)$ via the Euler class (here $M$ is any paracompact space, see Husemoller's book "Fiber bundles", section on characteristic classes).

This is standard material but unfortunately not written in textbooks (except for the $U(1)$ case) so I refer to appendices in my papers here and here.

ADDED: regarding the difference between $SO(3)$ and $SU(2)$ bundles, a correct thing to say is that $SU(2)$ equals $Spin(3)$, so an $SO(3)$ bundle has a Spin structure which happens exactly when its second Stiefel-Whitney class vanishes. The class lives in $H^2(M;\mathbb Z_2)$. Thus the question is what "proportion" of $SO(3)$ bundles have a Spin structure. (I put proportion in quotation marks because often both sets of bundles are countably infinite.) The answer of course depends on $M$. If $H^2(M;\mathbb Z_2)=0$, every $SO(3)$ bundle over $M$ is spin. In general, the universal coefficients theorem tells us which classes in $H^2(M;\mathbb Z_2)$ come from $H^2(M;\mathbb Z)$, and any class in the latter group can be realized as the Euler class of an $SO(2)$ bundle, and its mod 2 reduction is the Stiefel-Whitney class. Since any $SO(2)$ bundle is gives rise to an $SO(3)$ bundle we can realize many nonzero classes in $H^2(M;\mathbb Z_2)$ as Stiefel-Whitney classes of some $SO(3)$ bundles; these bundles are not spin.

  • 1
    $\begingroup$ Also if the bundle admits spin structures, then $H^1(M;\mathbb Z_2)$ acts freely and transitively on isomorphism classes of spin structures. $\endgroup$
    – nsrt
    Jul 19, 2013 at 19:15
  • $\begingroup$ Thanks for the answer, this really helped! Do you think it is possible in the way you described to construct for every $x\in H^2(M;\mathbb Z_2)$ a $SO(3)$-bundle $\xi$ such that $w_2(\xi)=x$? $\endgroup$
    – Frank
    Jul 25, 2013 at 12:46
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    $\begingroup$ @Frank: Not every $x \in H^2(M; \mathbb{Z}_2)$ arises as the second Stiefel-Whitney class of an orientable vector bundle (regardless of the rank), see this question. Even if there is an orientable vector bundle with $w_2$ equal to $x$, you can't always choose it to be rank three. $\endgroup$ Feb 5 at 4:22

Let me add a few further remarks to the above very good answer. I think that the problem of classifying principal bundles is one of the most fundamental questions and applications of algebraic topology.

The basic reason why the classification of principal bundles for $G$ a compact Lie group is so much more complicated than for a finite group is that the compact Lie group is not discrete and has higher homotopy. For example, the principal $G$-bundles over $S^n$ are classified by $\pi_n(BG)\cong \pi_{n-1}(G)$. In particular, the complete classification of bundles is not even known over spheres of arbitrary dimension.

The question simplifies a bit if you stabilize, i.e., you look at $O(\infty)$-bundles or $U(\infty)$-bundles. In these cases, the homotopy sets $[M,BO]$ or $[M,BU]$ are topological K-groups and can in principle be computed using long exact sequences and such things.

However, in general, the classification of principal bundles over finite CW-complexes is going to be more and more complicated with growing dimension. To give you some flavour of the sort of results to expect, you might want to have a look at some of the following papers:

A.Dold and H.Whitney. Classification of oriented sphere bundles over a $4$-complex. Ann. of Math. (2) 69 (1959), 667-677.

I.M.James and E.Thomas. An approach to the enumeration problem for non-stable vector bundles. J. Math. Mech. 14 (1965), 485-506.

F.P.Peterson. Some remarks on Chern classes. Ann. of Math. (2) 69 (1959), 414-420.

L. Smith. Complex 2-plane bundles over $\mathbb{CP}(n)$. Manuscripta Math. 24 (1978), 221-228.

R.M.Switzer. Complex 2-plane bundles over complex projective space. Math. Z. 168 (1979), 275-287.

... and for something more recent (look at the progress in dimension)...

M. Cadek and J. Vanzura. On oriented vector bundles over CW-complexes of dimension 6 and 7. Comment. Math. Univ. Carolin. 33 (1992), 727-736.

B. Antieau and B. Williams. On the classification of oriented 3-plane bundles over a 6-complex. arXiv:1209.2219.

This does not even say anything about the classification of principal bundles with exceptional structure groups....

[Edit:] I should have said that in all the above cases, the results are proved using obstruction theory. The answer then classifies bundles in terms of characteristic classes in suitable cohomology theories, together with additional data like compatibilities with Steenrod operations etc. This is a standard procedure in algebraic topology. Look at Hatcher's algebraic topology book for an introduction to Postnikov towers and obstruction theory.


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