The Whitney sum formula for Stiefel-Whitney classes, $w_n(V \oplus W) = \sum w_i(V) w_{n-i}(W)$, looks a lot like the one for Chern classes $c_n(V \oplus W) = \sum c_i(V)c_{n-i}(W)$. But I don't know a way to prove both formulae "at once".

Question: Is there an abstract computation from which both Whitney sum formulae follow?

For instance, constructing cell structures on $BO$ and $BU$ and then just reading off what the relevant maps do on cohomology doesn't "explain" why the formulas "look the same" in both cases, so doesn't fit the bill for me.


  • The Whitney sum formula for Stiefel-Whitney classes is also related to the Cartan formula for Steenrod squares, $Sq^n(xy) = \sum Sq^i(x)Sq^{n-i}(y)$, since Stiefel-Whitney classes can be defined in terms of Steenrod squares. I don't know a corresponding formula in integral cohomology operations related to Chern classes. An answer which sheds light on this connection would be most welcome.

  • These formulae are equivalent to working out the comultiplication on $H^\ast(BO;\mathbb F_2)$ and $H^\ast(BU;\mathbb Z)$ respectively. It appears to me to be forced algebraically that e.g. the pullback of $c_n \in H^\ast(BU(n);\mathbb Z)$ to $H^\ast(BU(1)^n;\mathbb Z)$ is some scalar multiple of $c_1^{\otimes n}$, but I can't seem to rule out that the scalar multiple is zero except by invoking the splitting principle (which I'd ideally like to avoid -- I'd really like a computation of this comultiplication which implies the splitting principle!), and I'm also not sure I can show that if nonzero, the scalar is a unit.

EDIT: I did eventually arrive at a way to compute this coproduct without constructing complete cell structures: In the fibration $\mathbb{CP}^{n-1} \to BU(n-1) \times BU(1) \to BU(n)$, observe that the Serre spectral sequence for integral cohomology must collapse because we know the rank of all the groups involved, which are free. It follows that $H^\ast(BU(n)) \to H^\ast(BU(n-1) \times BU(1))$ is injective; iterating gives the splitting principle and the coproduct formula. The fibration $\mathbb{RP}^{n-1} \to BO(n-1)\times BO(1) \to BO(n)$ works similarly in the real case. I still find this argument unsatisfactory because one must still treat the two cases "in parallel" rather than proving one theorem and deducing both results from it.

  • There might be some sort of argument which deduces the comultiplication on $H^\ast(BO)$ from the one on $H^\ast(BU)$ or vice versa -- this isn't precisely what I'm looking for, but I'd be interested to see this worked out.

  • It would be very nice if there were an argument which were to abstractly construct an $E_\infty$ map $MU \to H\mathbb Z[t^\pm]$ (where $|t| = 2$) corresponding to the total Chern class $c = \sum_n c_n t^{-n}$, and deduce the comultiplication formula by computing that the map does this on the homology of $\Sigma^{\infty-1} BU \subset MU$ and using that it is multiplicative. I haven't quite been able to see through such an argument though. (As pointed out by Oscar Randal-Williams below, Totaro has shown that this does not work!)

  • 6
    $\begingroup$ Regarding your last point, see B. Totaro "The total Chern class is not a map of multiplicative cohomology theories". $\endgroup$ – Oscar Randal-Williams Mar 20 at 23:29
  • 4
    $\begingroup$ I think the proof in Milnor-Stasheff of the Whitney sum formula for Chern classes works for Stiefel-Whitney (SW) classes. The proof is a computation in $H^*(BU(n))$ and one just has to run it in $H^*(BO(n);\mathbb Z_2)$. The analogy between SW and Chern classes is also explained in Exercise 14.E of Milnor-Stasheff. Both classes satisfy the same axioms and can be constructed in the same way inductively starting with the Euler class (taken mod 2 in the SW case), and without Steenrod squares. $\endgroup$ – Igor Belegradek Mar 21 at 0:07
  • 1
    $\begingroup$ @IgorBelegradek Thanks, but it still looks to me like an "accident" that the coproduct on $H^\ast(BU;\mathbb Z)$ turns out to be given by such a similar formula to the coproduct on $H^\ast(BO;\mathbb F_2)$ (perhaps you're arguing that this is indeed just a "brute fact", a coincidence?). The fact that both classes satisfy the same axioms is question-begging, because one of the axioms is this coproduct / Whitney sum formula! A priori, it should indeed be clear that they can be defined in the same way, but then it's still a "miracle" that their Whitney sum formluas turn out to be the same. $\endgroup$ – Tim Campion Mar 21 at 0:21
  • $\begingroup$ @OscarRandal-Williams Thanks -- already Totaro's title resolves that part of the question in the negative! $\endgroup$ – Tim Campion Mar 21 at 0:22
  • 6
    $\begingroup$ I wonder about Real vector bundles in the sense of Atiyah. I suppose that there are characteristic classes living in equivariant cohomology of the base, and I wonder if the theory of SW classes and the theory of Chern classes are both special cases or reflections of some bigger story. $\endgroup$ – Tom Goodwillie Mar 21 at 1:13

I prefer this approach which I believe is due to Grothendieck. (I haven't checked how this compares with the sources cited by Nick Kuhn.)

Let $(\mathbb{K},R,d)$ be $(\mathbb{R},\mathbb{Z}/2,1)$ or $(\mathbb{C},\mathbb{Z},2)$. Let $V$ be a $\mathbb{K}$-linear vector bundle over $X$. Over the associated projective bundle $PV$ we have a $\mathbb{K}$-linear tautological line bundle $T$ classified by a map $PV\to \mathbb{K}P^\infty$. I'll assume that we know that $H^*(\mathbb{K}P^\infty;R)=R[x]$ with $|x|=d$. Pulling back $x$ gives a class $x\in H^d(PV;R)$. Induction over the cells of $X$ shows that $H^*(PV;R)$ is a free module over $H^*(X;R)$ with basis $\{x^i\mid 0\leq i<\dim(V)\}$. Thus, there is a unique monic polynomial $f_V(t)\in H^*(X;R)[t]$ of degree $\dim(V)$ such that $H^*(PV;R)=H^*(X;R)[x]/f_V(x)$. The characteristic classes of $V$ are just the coefficients of $f_V(t)$ (possibly with an extra $\pm$-sign, according to conventions). The cofibre of the inclusion $PV\to P(V\oplus W)$ is the Thom space of a $\mathbb{K}$-linear vector bundle over $PW$, and it follows that $f_V(x)f_W(x)$ annihilates $H^*(P(V\oplus W);R)$, and thus that $f_{V\oplus W}(t)$ must be equal to $f_V(t)f_W(t)$. By comparing coefficients we get the standard formula for characteristic classes of $V\oplus W$.

  • 2
    $\begingroup$ Yes, we are on the same page here. $\endgroup$ – Nicholas Kuhn Mar 21 at 17:48
  • 1
    $\begingroup$ I find it weird that, when referring to the polynomial $f_V(t)$ in question, seemingly very few articulates that it is the characteristic polynomial (of multiplying $x$, which should be dual to taking the hyperplane section). $\endgroup$ – Z. M Mar 22 at 22:19

There are many ways to prove these formulae uniformly, and, of course, you need to start from an appropriate definition of these classes. But as has already been suggested in the comments, pretty much any definition of the Chern classes can be adapted to give a definition of the Stiefel-Whitney classes, with proofs of their properties also in parallel. Certainly Husemuller's book does this.

When I have taught a course on fiber bundles, I give the proof the Whitney sum formula as presented in [P. Conner and E. Floyd, The relation of cobordism to K-theory, SLNM 28 (1966)]. It also works for any complex oriented theory too (and, if I remember right, it is the proof followed by Husemuller).

Of course, in the end, one learns that these classes for a bundle that is the sum of line bundles are the symmetric functions, and then the fact that the formula is true becomes evident using the splitting principle.

  • $\begingroup$ I was being overly cute when I phrased this question in terms of characteristic classes. What I really want to know is why the coproduct on $H^\ast(BU,\mathbb Z)$ looks the same as the coproduct on $H^\ast(BO,\mathbb F_2)$. I see that in Husemoller's book Fiber bundles he proves this by appeal to the splitting principle in 17.6.2. I couldn't find this in Conner and Floyd. I suppose the argument "in both cases we have a splitting principle, and this is the only comultiplication compatible with that" kind of works... $\endgroup$ – Tim Campion Mar 21 at 3:49
  • $\begingroup$ ... I was hoping for an argument not appealing to the splitting principle (like the argument I gave in the question statement), since I'd like to deduce the splitting principle from the comultiplication and not the other way around. Moreover I was hoping for an argument which isn't applied "in parallel" but rather involves proving one theorem which can be applied to both the real and complex case. I suppose I have in mind something like an algebraic classification of Hopf algebras of such-and-such a form. $\endgroup$ – Tim Campion Mar 21 at 3:49

This is mainly a comment about your point (4), but I do not seem to have enough reputation to comment on Oscar's comment.

In fact, there is an $\mathbb{E}_{\infty}$ ring map $$\Sigma_+^{\infty}\mathrm{BU} \to H\mathbb{Z}[t^{\pm}],$$ or equivalently an infinite loop map $$\mathrm{BU} \to GL_1(H\mathbb{Z}[t^{\pm}]).$$ The claim that the latter map is a loop map recovers the formula for the total chern class of a direct sum of bundles. This $\mathbb{E}_\infty$ ring map is constructed in the many author paper "Algebraic cycles and infinite loop spaces." Allen Yuan once convinced me that the algebraic geometry in their paper can be replaced by a homotopy theoretic argument, but nothing is written about that.

As a warning, to make sense of this one needs to take care about the meaning of $H\mathbb{Z}[t^{\pm}]$. There are several different $\mathbb{E}_\infty$ ring structures on $H\mathbb{Z}[t^{\pm}]$ (which are all equivalent as $\mathbb{E}_2$ rings). The precise $\mathbb{E}_\infty$ ring structure you want here is the one constructed in the many author paper "Algebraic cycles and infinite loop spaces." Of course, it is only the $\mathbb{E}_2$ structure that matters for such an unstructured statement as you want in your question.

I believe that what Totaro proves is that there is no homotopy ring spectrum whose underlying additive spectrum is $sl_1(H\mathbb{Z}[t^{\pm}])$, which Segal hoped would exist but seems like a rather strange thing to ask for from a modern point of view.

  • $\begingroup$ Perhaps it is also worth remarking that to get the double loop map from BU to GL_1 that suffices for your question, one can use classical obstruction theory. Indeed, the double delooping of BU is BSU, which has even cells, and the double delooping of GL_1 has even homotopy groups. $\endgroup$ – Jeremy Hahn Mar 21 at 13:49
  • $\begingroup$ Welcome to MathOverflow, Jeremy! Thank you for sorting this out -- I was very disappointed when I read the title of Totaro's paper (I admit I did not look into it in detail, though), so it is very good to know that the total Chern / SW class is part of an $E_\infty$ map. The idea in the present context was that the existence of such a map, if true, would likely come from some sort of "formal" construction which could be be done without computing anything -- without delving into the details of the many-author paper, I suppose it's unclear whether that's the case here. $\endgroup$ – Tim Campion Mar 21 at 15:42
  • 3
    $\begingroup$ I think perhaps that this can be considered a "calculation-free" construction, of the kind you might have in mind, as long as you only ask for an E_2 ring map (an E_2 map is more than enough to get the formula for the chern class of a sum). The input is that the double delooping of BU (i.e. BSU) has even cells. It looks likely to me that the same argument goes through word for word in the Real setting (using that BSU_{R} has a nice equivariant cell structure), which develops the story for stiefel whitney and chern class in the same construction. $\endgroup$ – Jeremy Hahn Mar 21 at 15:58

Your Answer

By clicking “Post Your Answer”, you agree to our terms of service, privacy policy and cookie policy

Not the answer you're looking for? Browse other questions tagged or ask your own question.