Bundle structures and lifting problems (Ex)

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[edit] 1 Lifting maps

Given a (pointed) map g: Y\to Z of pointed topological spaces, we define the homotopy fibre of g as

\displaystyle  \mathrm{hofib}(g):=\{(y,\gamma)\in Y\times PZ|\,\gamma(1)=g(y),\,\gamma(0)=z_0\},

where PZ is the space of paths starting at the base-point of Z. We denote by p: \mathrm{hofib}(g)\to Y the projection.

Exercise 2.1. Prove the following:

A map f:X \to Y of pointed space has a lift \bar f:X\to \text{hofib}(g) along p if and only if g\circ f is homotopic to the constant map.

Hint 2.2. This is a special case of [Hatcher2002, Proposition 4.72].

[edit] 2 Classification of orientations and spin structures on vector bundles

Recall the Definition of Eilenberg-MacLane-spaces. We denote the space of pointed loops in a space X by \Omega X.

Exercise 4.1.

  • Show: There is a homotopy equivalence \Omega K(n+1,\Zz/2\Zz)\simeq K(n,\Zz/2\Zz).

Hint: Use the uniqueness of Eilenberg-MacLane-spaces and the long exact sequence in homotopy associated to the path-space-fibration

\displaystyle \Omega K(n+1,\Zz/2 \Zz)\to P(K(n+1,\Zz/2 \Zz))\to K(n+1,\Zz/2 \Zz) \;.

Recall that the path-space is contractible.

  • Show that the set of homotopy classes of pointed maps [Y,\Omega X] has a group structure induced by composition of paths.

Hint: This is similar to the group structure of the fundamental group.

Maybe you've heard that the group H^1(X,\Zz/2\Zz) acts free and transitively on the set of spin structures of an oriented vector bundle \xi\to X (X a compact pointed space). Now recall that \ref{The group structure on H^1(X,\Zz/2\Zz) is due to the Exercise 3.2.} H^1(X,\Zz/2\Zz)\cong [X,K(1,\Zz/2\Zz)], where K(1,\Zz/2\Zz) denotes an Eilenberg-MacLane-space.

So we first prove the statement about classification of spin structures. The warm-up is the classification of orientations:

  1. The first Stiefel-Whitney class is a map w_1:BO\to K(1,\Zz/2\Zz).
  2. The homotopy fiber hofib(w_1) is BSO.
  3. The projection p:BSO\to BO is the map induced by SO\hookrightarrow O.

Exercise 4.2. Assume that the homotopy groups of O are known.

  1. Calculate the homotopy groups of BO using the fibration O\to EO\to BO.
  2. Calculate the homotopy groups of BSO using the fibration
    \displaystyle BSO\to BO\stackrel{w_1}{\to} K(1,\Zz/2\Zz)\;.
  3. Calculate the homotopy fibre of p:BSO\to BO.

Now we can classify the orientations on a vector bundle \xi: E\to X. For this we need to know that the sequence

\displaystyle \text{hofib}(p)\to BSO \to BO

fits into the following diagram\footnote{It's non-trivial to see that the functor B can be applied to each of those spaces.}:

\displaystyle  \xymatrix{ \mathrm{hofib}(p) \ar[r]^q \ar[d]^{\simeq}   & BSO \ar[r]^p \ar[d]^{\simeq}   & BO \ar[d]^{\simeq} \\ \Omega B\mathrm{hofib}(p) \ar[r]^{\Omega Bq} & \Omega BBSO \ar[r]^{\Omega Bp} & \Omega BBO }

Hence there are group structures on [X,\text{hofib}(p)] and [X,BSO] (the latter one is the Whitney-sum of vector bundles). Furthermore there is an action of [X,\text{hofib}(p)] on [X,BSO] induced by q.

Definition 4.3. A vector bundle is called orientable if its classifying map f: X \to BO lifts along p:BSO \to BO. An orientation is the choice of such a lift. The first Stiefel-Whitney class of \xi is defined as the composition w_1\circ f, where w_1 is defined as above.

Exercise 4.4. Let X denote a compact pointed space and \xi: E\to X a vector bundle on X.

  1. Use Exercise 3.1 to show that \xi is orientable if and only if its first Stiefel-Whitney class vanishes.
  2. Show that the group [X,\text{hofib}(p)] acts free and transitively on the set of homotopy classes of lifts.

Hint: Use the homotopy-lifting property and Exercise 3.1

  1. Give an interpretation of the group [X,\text{hofib}(p)].

Now there are similar results for spin structures (on oriented vector bundles).

Exercise 4.5. Repeat Exercises 3.3 and 3.4 using the second Stiefel-Whitney class w_2:BSO\to K(2,\Zz/2\Zz). The homotopy fibre of w_2 is BSpin, where Spin is the colimit over Spin(n), the universal cover of SO(n).

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