Conversation started Jan 14, 2019 at 23:05.
Jan 14, 2019 23:05
Clean approach: given a vector bundle $E \to M$ of rank $n$, consider the action of $GL_n$ on $E \setminus 0$ (which is a $\Bbb R^n \setminus 0$ bundle), and on $\mu_2$ by the action of the determinant. Then the "orientation double cover of $E$" is the double cover $\Lambda(E) \to M$, where $$\Lambda(E) = (E \setminus 0) \times_{GL_n} \mu_2.$$
That is, all you're saying is "Forget the bases, just remember the orientation", and there is a way to make this happen just by taking products and quotients - insert a factor for arbitrary orientations, and then quotient by the rule saying a basis is equivalent to the corresponding orientation
This is usually called the cocycle description of vector bundles; this data is precisely what is called a Cech cocycle in $Z^1(M; \mathcal{GL}_n)$, where the latter is the sheaf of groups given by $\mathcal{GL}_n(U) = \text{Map}(U, GL_n)$; one can perfectly make sense of first cohomology with coefficients in sheaves of nonabelian groups, and what the above description says is $$H^1(M; \mathcal{GL}_n) \cong \text{Vect}_n(M).$$
There's no real reason here to restrict to $GL_n$. Here is the general definition: a fiber bundle $E \to M$ with fiber $F$ and structure group $G \subset \text{Aut}(F)$ (automorphisms continuous or smooth or whatever is appropriate here) is equipped with local trivializations $E \big|_U \cong U \times F$ as above, so that the transition maps $U_i \cap U_j \to \text{Aut}(F)$ always factor through $G$
Jan 14, 2019 23:13
I should have taken that to be $\text{Fr}(E) \times_{GL_n} \mu_2$, where the first is the fiber bundle with $$\text{Fr}_x(E) = \text{Space of bases for } E_x.$$
@LeakyNun Exactly, these are called "Principal G-bundles", and we took a vector bundle and spat out a principal GL(n)-bundle
It's easier to pass between different principal bundles by the formal operations above, so it is nice to pass to that first
Conversation ended Jan 14, 2019 at 23:31.
Wisdom from Mike
Jan '1914
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random cohomology for quantum nerds
covariance is unacceptable
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