Yeah, I hear that. I didn't know any of this as an undergraduate.
And nobody every really explains it to you.
Actually, yeah, that's kind of dumb. You should ask me and other people here lots of questions.
It's like this: you apply to universities for grad school. You get into some and not others. You have a *much* bigger chance of getting in if: 1) You have good grades and do well on the tests. 2) One of the professors at that university wants you to work in their lab/group.
When you get to the university, frequently for the first year you work as a TA to get money for rent and food and whatever else.
The first ~3 years of PhD here are sort of like a masters, and you can get a masters degree at that time if you want, but for the most part it's really all just one PhD.
@0celo7 That US power plugs work in Chinese outlets.
user54412
I've actually been here before, and yet I didn't remember that.
user54412
The conference actually starts tomorrow. Today was just meeting important people in my field I had never spoken to face-to-face. Which is arguably the most important thing to do anyway.
@ACuriousMind Suppose we have an infinite sequence of sets of the form $A_0\supset A_1\supset \cdots\supset A_b\supset\cdots$. What can we say about the intersection $\cap_{b=0}^\infty A_b$? Apparently it's only guaranteed to be nonempty if the whole thing is a subset of a compact set $S$.
@0celo7 I don't think you can generically say something about the intersection (unless the space is compact, as you say, or, even stronger, Noetherian, for example).
@0celo7 Compactness is equivalent to "Every collection of subsets with the finite intersection property has non-empty intersection".
A chain of subsets trivially fulfills the finite intersection property, so the intersection over the whole chain is non-empty if the chain is inside a compact set.
user54412
1:04 PM
0celo7: "How does A imply B?" ACM: "A is equivalent to B."
@0celo7 Good. Suppose the intersection is empty. Then, take the open cover $\{X - A_0, X - A_1, X - A_2,...\}$. By compactness, there is a finite subcover $\{X - A_{i_1},\dots,X-A_{i_n}\}$, which means $\bigcap_{j = 1}^n A_{i_j} = \emptyset$, which is a contradicition to the finite intersection property. Hence, the intersection of the collection is non-empty.
@ChrisWhite Not to split hairs, but adapters rarely have any electronics in them (sometimes they are fused), so it's more about the kind of equipment you use: Laptops and mobile phones have transformers in the chargers, and those are usually built to handle the electric supply of any country. If you buy electronics from China which plug directly into whatever the voltage is you get from the wall (say power tools, kitchen appliances the like), those might blow up back home.
Did you take the maglev train? If you do, make sure you take it during the fast hours (from what I remember, most of the day it runs a bit slower than the max speed).
@ACuriousMind GDI, why does a finite number of them have empty intersection? Are we allowed to choose the finite subcover so that their intersection is empty?
Or do we write $S=\cap_{i=1}^n (S-A_i)$ and deduce it from there?
@ACuriousMind In the second part of the proof, they say "If no finite subcollection sovers $S$". Doesn't there have to be a finite subcollection that covers $S$ due to compactness?
@ACuriousMind So...we assume that there is no finite subcover, and this leads to a contradiction. I don't see what part of the contradiction implies the theorem.
I'm also not sure why $\cap_\alpha(S-O_\alpha)\ne\emptyset$.
@0celo7 You use it to show that the original cover wasn't a cover to begin with (since you derive the non-empty infinite intersection from the non-empty finite intersections).
Their proof could be written clearer
Let $U_i$ be an open cover of $S$. Assume $U_i$ has no finite subcover. Then, the collection $\{S - U_i\}$ has non-empty finite intersections. By assumption, $\bigcap_i (S - U_i)$ is then also non-empty, implying $\bigcup_i U_i \neq S$, which contradicts $U_i$ being a cover. Thus, $U_i$ must have a finite subcover, and $S$ is compact.
@0celo7 Yes, my group theory homework has been to prove the above and $\chi_{\Lambda^2 V}(g) = 0.5(\chi_V(g)^2 - \chi_V(g^2))$.
So now we need only use that the adjoint of $\mathrm{SU}(2)$ is the...symmetric part of the product of the fundamental with itself, I think, and we have what we wanted to prove, I think.
Could also be the antisymmetric part, but anyway, the trace formula itself does, surprisingly, not really rely on the properties of $\mathrm{SO}(N)$ or $\mathrm{SU}(N)$.
@0celo7 Because I'm tracing the matrix I got by applying $\rho_\otimes$ to the basis of $S^2\Lambda$ - that is the definition of the trace on $S^2\Lambda$.
@0celo7 Well, the task was just "Prove that this formula holds", so, for lack of any other approach, I just wrote down the naive basis for the symmetric part and tried to trace over that. And, to my own surprise, it worked.
@0celo7 I think I will. This is so much simpler than what Lubos does.
I was discussing the weak energy condition of GR with my supervisor a while ago (energy densities must be measured non-negative by any observer). I remember him telling me that pointwise violations of the WEC aren't a concern as it is not "physical" to measure an energy density at a point. What is meant by "not physical"? Is it that a density is an average over a volume of spacetime, thus a pointwise value bares no real meaning or is it that a pointwise measurement is not practically achievable?
I have to explain the concept of a continuum that is used for the description of the dynamic behaviour of the fluids, and to explain how this concept is related on the one side with the laboratory measurements of diverse sizes (velocity, density, etc.), and on the other side with the mathematical...
@Rammus I think it is the latter - you can't measure things at a "point", every experiment will measure things within an interval. We measure energies, not densities, and the energy is the integral of the density, but a point is a zero measure set, so the integral of the density over a point, or a set of discrete points, is always zero - it carries no physical meaning at all.
@DanielSank thx for sharing! wondering, did the google acquisition affect salaries at all over there? also there are rumors martinis wants to get into adiabatic QM computing somehow but it seems like the lab doesnt have any papers on that...(so far)?
@Rammus I think something along those lines, yeah. But then you'd have to show something like $\forall \epsilon >0 $ the density averaged over the $\epsilon$-cube is larger than zero, to make it be okay
@Danu Yeah, I was looking at violations of the strong energy condition for the real scalar field so I was specifically looking for negative values when averaged over world tubes/lower bounds for this. Similar to what Hawking and Ellis did in The large scale structure of spacetime pp. 95-96
@ACuriousMind Ok, then check out Prop 6.5.1 on p. 202. They say "neighborhood" in the second sentence, but it clearly seems wrong. For instance, take $q$ to be in $\bar{\mathscr{S}}$. Then an open nbd of $q$ will intersect the set.
@Danu HE never does this or use a separate equality for definitions. The latter leaves me wondering if there's something obvious I missed or they're defining things with desirable properties.
@vzn I graduated with my degree and got a job as a Google employee. That made my income go up. Most of the post-docs quit their university jobs and got hired by Google, so their incomes also went up. The grad students are still UCSB grad students, so they get the same stipend as before.
Background
We get a lot of posts asking several related by independent questions [1].
Often the posts are even formatted as enumerated lists, making it clear that the author knows that he/she is asking more than one question.
I believe that the quality of the question/answer system increases if ...