2 MU(n) and MU
Definition
2.1
We define MU(n) to be the Thom space of the tautological vector bundle of BU(n).
We define MU to be the Thom spectrum of the tautological virtual vector bundle of BU. Equivalently,
MU=ncolimΣ−2nΣ∞MU(n).
The direct sum map BU×BU→BU induces a map MU∧MU→MU, which turns MU into a ring spectrum (and in fact an E∞-ring spectrum).
The crucial insight of Thom was that this spectrum is closely related to cobordism theory.
Theorem
2.2
(Pontryagin–Thom)
Let X be a space. Then MU∗(X+) admits the following description:
A class in MUd(X+) is represented by a d-dimensional stably almost complex manifold M and a map f:M→X. Addition is given by disjoint union.
Two classes f1,f2 are equivalent if there is a cobordism g:N→X between them.
[Proof idea] Given a class in
MUd(X+), I explain how to get such a map
f:M→X. By the Whitney embedding theorem.
A map Sd→MU∧X+ factors through a map Sd→Σ−2nMU(n)∧X+ for some n, and is thus given a map of spaces ϕ:Sd+2n→MU(n)∧X+, increasing n if necessary (since Σ2kMU(n)↪MU(n+k)). Recall that
MU(n)∧X+=MU(n)×X/{∗}×X,
where the point on the right is point at infinity. MU(n) also contains the “zero section” isomorphic to BU(n), and the normal bundle of the zero section is the tautological bundle of BU(n). Generically, we can choose ϕ to intersect transversely in a way that ϕ−1(BU(n)×X) is a codimension 2n submanifold of Sd+2n, and the normal bundle, being pulled back from BU(n), has an almost complex structure. This gives a stably almost complex manifold of dimension d with a map to X. A homotopy of ϕ gives a cobordism between such maps.
So in particular, MU∗=π∗MU is the complex cobordism group. Remarkably, these groups are entirely computable.
Proposition
2.3
H∗(MU)π∗(MU)=Z[b1,b2,b3,…]=Z[m1,m2,m3,…]
where ∣mi∣=∣bi∣=2i. The Hurewicz map π∗(MU)→H∗(MU) is injective but not surjective.
[Proof sketch] Since the tautological vector bundle of
BU is oriented, the first part follows from the Thom isomorphism theorem and the standard calculation of the homology of
BU. The homotopy groups follow from a more involved Adams spectral sequence calculation.