@Daminark for each open $U \subseteq \Bbb R$, declare $\mathscr F(U)$ to be the functions $s : U \to F$ such that $\pi \circ s = \operatorname{id}|_U$, i.e. a sort of "partial" sections
@Daminark and then this will give us our original sheaf. If we started with a presheaf, we'll still end up with a sheaf, called the sheafification (you might have heard of this)
Problem: Let $M$ be a module over the integral domain $R$. If $x \in Tor(M)$ is nonzero, show that $x$ and $0$ are "linearly independent"...Question: what does linearly independent mean in this context?
we were working through Zagier's proof of the Eichler-Selberg trace formula in the appendix of Lang in our modular forms lecture, the prof is sick, so a post doc (and friend of mine) has to the proofs, there are some really nasty errors and stuff like "that's easy with the substitution bla", but substitution bla just leads to a really nasty integral
Projection from the espace étalé to the base is a local homeomorphism, just like with a covering space. But what else is needed for a covering space, and can you see where that goes wrong?
@MikeMiller it does - for me it's kind of just something that's good to know behind the scenes rather than thinking too much about it though - but as balarka mentioned earlier maybe they're important in topology
@TedShifrin if we have open $U \ni x$, we can't partition $\pi^{-1}(U)$ into disjoint sets, each homeomorphic to $U$, since what I said makes the obvious partition not disjoint
adele rings are also local to global things (with local to global in a different sense), so maybe I should think of etale spaces as the topological analog of adele rings
@Eric so the options which came up were group cohomology, modular forms, and just raw ANT (class groups, all that) First two are more likely at the moment
I always like telling people to understand the espace etale of the trivial sheaf with fiber R, and that of the sheaf of sections of the trivial vector bundle R
In German we say "welke Garben" for flabby/flasque sheaves, so one theorem is "welke Garben sind schlaff", "flabby sheaves are acyclic" which sounds really funny in German
when studying a rigid body in some paper that gives model equations for its motion, why do the authors only care about the center-of-mass velocity? what about the instantaneous velocity at the other parts of the body? the papers make a "quasi-steady" assumption - does this mean that the velocity is assumed to not change throughout the body for a time, t_0?
@TedShifrin if we have an abelian group-valued sheaf $\mathscr F$ on topological space $X$, then the support of a global section $s \in \mathscr F(X)$ is the points $p \in X$ for which the germ $s_p$ is nonzero
@TedShifrin then what does the model being "quasi-steady" mean? I don't see what's quasi-steady about it; I had guessed that it meant that the velocity does not change throughout the body for some time, t_0
While looking through some of the formulae I came across this formula.$$\left(\dfrac pq\right)\left(\dfrac qp\right)=(-1)^{\frac{p-1}{2}\frac{q-1}{2}}$$
What I know is $\left(\dfrac pq\right)\left(\dfrac qp\right)=1$. But I have no idea how the above formula was derived. I just want to know how i...
those brackets in a lot of variations are well-established in number theory (and partially algebra), you use them for Legendre symbols, Jacobi symbols, Kronecker symbols, Artin symbols, Hilbert symbols and for generalized quaternion algebras as elements in the Brauer group
@TedShifrin Quasi-steady-state-approximation: A method to reduce the number of variables of a system that includes processes on different time scales which can be separated into slow and fast. One assumes that the fast processes are always in a steady state, which changes on the slow time scale.
@TedShifrin yeah, the system is described by a force model - so, not a great deal of variables - position, velocity, acceleration, torque, so, I'm not really sure where the quasi-steady assumption was applied to