@Bass : it isn't my diagram, it's a Penrose diagram. And no, I can't explain it in simple English. Or things like the prallel antiverse. But see Wikipedia and note that "the precursors to the Penrose diagrams were Kruskal–Szekeres diagrams". I can explain the problem with Kruskal-Szekeres coordinates.
In any case, my interpretation expounded above was heavily influenced by the view taken by one of my professors---who admits that, at heart, he's a geometer. I wouldn't be surprised if his position is heavily biased :P
I think it's a conceptually nice picture, though.
It is not so far off to say that topology is the study of homeomorphism-invariants, is it?
Something not very related, but fun: Erlangen programme studies geometric objects by studying groups which act on it. There is a way to do this in the opposite : studying groups by looking at the geometric objects (in particular, graphs) it act on. Turns out the geometry of the objects a certain group act on is specific to the groups nature, in a sense (so, there are things like hyperbolic groups).
So, for example, if you look at the Cayley graph of the free group on 2 generators, you'll see surprising similarities with the Poincare disk model of the hyperbolic plane.
@Danu that's nice.
Essentially, if $X$ is a simply connected topological space, $G$ is a group which acts on $X$ by homeomorphisms freely and properly discontinuously (for any pt $x \in X$, there is an nbhd $U$ of $x$ such that orbits of $U$ by $G$-action are all disjoint) then $G$ is called the fundamental group of $X/G$ :P
And $X$ is called the universal cover of $X/G$. I am lying slightly, because that's not how it's defined, but you can think of it like this.
@Minhyong Kim: So Klein's notion of geometry is neither more nor less restrictive than the Riemannian one. Klein's includes examples like topology, which have no system of measurement, so in that sense it's more general than Riemannian geometry, not less. — Ben CrowellJan 28 '13 at 15:56
@0celo7 : I know this. It's fairly straightforward, see my answer. Note that the curvature relates to the tidal force, which in general increases towards the centre. This is why people talk about the strong curvature regime in the context of black holes. For the Earth it increases then reduces then increases then reduces.
@ChrisWhite about that flag: ironically we didn't see it because the community was "too efficient" at getting the post automatically deleted :-P we should figure out some way to deal with that
@0celo7 seems to be something like a higher representation of a spin group.. like a normal tensor is a higher representation of the orthogonal group. right?
@ACuriousMind maybe I'm mixing stuff, but the christoffel symbols are kinda matrices but they are no tensors? If every matrix is a tensor, why all these exercises "prove that xyz transforms like a tensor"?
What is the difference between a matrix and a tensor? Or, what makes a tensor, a tensor? I know that a matrix is a table of values, right? But, a tensor?
Perhaps I should clarify that when I say "every matrix is a tensor" I mean "every matrix that is meant to represent a linear map (as matrices are wont to do) is a tensor".
for example, if I wrote down a matrix that count the number of apples in a 2x2 stack of cubicles, this thing obviosuly does not depend on which coordinate system we are choosing
And the three indices on the Christoffels are actually "of different type" - it is actually a one-form taking values in $n\times n$ matrices, see my answer here
@Secret and then you're in represenation theory of some Lie group, right? so, is it correct to say that a Spinsor (tensor with spinor indices) is composed of irreps of the Spin group?
The numbers you saw here are only valid for a certain basis, or may not be related to the basis at all if it is just something like the "apple matrix" I mentioned above
@Bass I am still not terribly good at spinors to comment anything on that, Acuriousmind might be a better person to ask
@ACuriousMind is it correct to say that a Spinsor (tensor with spinor indices) is composed of irreps of the Spin group? like a normal tensor is composed of irreps of the general linear group (or orthogonal?)
@Bass Each gamma matrix is a mapping $S\to S$ for $S$ the spinor representation (since you use it to multiply a spinor and get again a spinor). Hence each $\gamma^\mu$ transforms in $S\otimes S^\ast$. This is intertwined with the transformation of the vector index as $$ \rho_S(\Lambda)^{-1}\gamma^\mu\rho_S(\Lambda) = (\rho_V(\Lambda)\gamma)^\mu$$
@Bass ...I suppose so? I don't really think about it with indices. For any vector space $V$, a linear map $V\to V$ is equivalently a bilinear map $V\times V^\ast \to \mathbb{R}$ since $V\cong \mathrm{Hom}(V^\ast,\mathbb{R})$, and such bilinear maps are precisely the elements of the tensor product $V\otimes V^\ast$
(This message was supposed to be posted 30 mins ago): Finally some nice discussion going on in the chat, I am so bored to death by the recent lack of activity!
@ACuriousMind just to be sure, in your equation above, everything is to be read as operators or matrices, acting on something on their right, is that correct?
@BalarkaSen Far better than some of the random plus lack of activity approx 2 hours ago, as right now, there's some academic discussion going on, thus a chance to learnt more stuff!
@0celo7 From my 3 days of observations, he often come with questions to ask, quite similar when at approx. 3:00 in Syd time, you and Acuriousmind often have nice discussion about topology, group theory and abstract algebra
@BalarkaSen The recent fallout 4 stole a lot of opporunity of otherwise interesting discussions, because too mnya people are playign on it and I was stuck with a malfunctioning program in my honours project
Hi, I wanted to ask you people something. In general, we all learn everything someday. It can be from a source or a thought itself. Would you like to be able to share it somewhere, as in kind of a social network where people share their learning experiences(with source) and you can follow people you like. Does this sound interesting?
@0celo7 : I can explain a lot of things in GR. But I can't explain the parallel universe, the antiverse, the parallel antiverse, the new universe, or the new parallel universe. How on Earth anybody believes in that stuff beats me.
Mostly it can help evaluate the learning outcomes and efficiency of a particular learning source and help you meet and connect to new like minded people.
@0celo7 : you shouldn't, because the precursors to the Penrose diagrams were Kruskal–Szekeres diagrams. See Wikipedia. And Kruskal-Szekeres coordinates are akin to Gullstrand-Painleve coordinates, which Einstein dismissed for good reason.
@0celo7 : mechanics is a whole field, GR is a particular theory. There's a big difference. And when you read up on GR in the Einstein digital papers you appreciate that Penrose diagrams are borne of misunderstanding.
@0celo7 : I will explain why KS coordinates are wrong and why Penrose diagrams are built on a misunderstanding. It's to do with the coordinate speed of light. See this:
"For example, at the event horizon of a black hole the coordinate speed of light is zero, while the proper speed is c.[1] The coordinate speed of light (both instantaneous and average) is slowed in the presence of gravitational fields. The local instantaneous proper speed of light is always c."
The parrot is dead, and nothing you do is ever going to change that.
@0celo7 : the coordinates preferred by the distant observer.
I'm the distant observer, and you're at the event horizon in a bubble of artistic licence. You are at a location where the coordinate speed of light is zero. The parrot is dead.
@0celo7 : you have an optical clock. But because you're at a place where the coordinate speed of light is zero, this clock doesn't tick. Not ever. Never ever ever. Gravitational time dilation is infinite. But Kruskal-Szekeres replace the t coordinate with a T coordinate and claim that the clock somehow starts ticking "in your frame". They effectively claim that a stopped clock ticks from the point of view of a stopped observer.
"The light-like geodesic in $D^2$ lying in the 2-plane $x - t = 0, y = 1$ projects to a light-like geodesic in $M^2$ which is self-intersecting (since the points $t = - 1, x = - 1, y = 1$ and $t = 1, x = 1, y = 1$ of $D^2$ become identified in $M^2$). Time-like geodesics in $D^2$ near the above light-like geodesic also project to self-intersecting geodesics in $M^2$."
@JohnDuffield Anyway, since it's clear that you don't want to talk physics, I think it would be best for us not to converse in the future. It never ends well.
@0celo7 : the stopped clock doesn't tick. Sticking a stopped observer doesn't make it start ticking again. So KS coordinates represent a misunderstanding of GR. And "the precursors to the Penrose diagrams were Kruskal–Szekeres diagrams".
@Bass : yes. If you're at a place where light doesn't move, some people claim that you don't see anything unusual. But the truth of the matter is that you're at a place where light doesn't move. So you don't see anything.
"Some spacetimes, such as G¨odel spacetime, do not admit any global time slices. This is a consequence of three features: it is time orientable; a CTC passes through each point; and it is simply connected. The edge of an achronal surface S is the set of points p such that every open neighborhood O 3 p includes points in I+(p) and I−(p) that can be connected by a timelike curve that does not cross S."
In mathematics, orientability is a property of surfaces in Euclidean space that measures whether it is possible to make a consistent choice of surface normal vector at every point. A choice of surface normal allows one to use the right-hand rule to define a "clockwise" direction of loops in the surface, as needed by Stokes' theorem for instance. More generally, orientability of an abstract surface, or manifold, measures whether one can consistently choose a "clockwise" orientation for all loops in the manifold. Equivalently, a surface is orientable if a two-dimensional figure such as in the space...
just need a double cover to detwist that line element into a proper vector field :p