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3:00 PM
@acuriousmind I see. That's if you consider attraction to be positive and repulsion to be negative lol
 
@ACuriousMind Is it still arbitrary when we do weird SUSY shit so that proton charge = - electron charge?
Or is there some absolute definition of charge in SUSY
 
@0celo7 What?
SUSY is even more horrible in the sign conventions you have to make
 
Hmm
 
And yes, the sign stays arbitary.
But I don't see what SUSY would have to do with the proton or electron charge
 
Isn't the sign of the electron charge basically the basis you pick for $U(1)$?
 
3:07 PM
@ACuriousMind Oh, not SUSY
I meant SO(10)
I think.
Maybe SU(5)
One of those grand unified theories.
 
Is SU(5) still going on
 
I think it's quite dead
 
Why?
 
Like the particle spectrum is too light or something
 
We should've seen some things by now that we didn't see, I think
 
3:09 PM
None of those light particles have been produced
Did u know
 
@DavidZ so it turns out that this old question
13
Q: What sort of experiment would directly test time reversal invariance?

David ZI guess the title says it all: how could/would you experimentally test whether our universe is truly time reversal invariant, without relying on the CPT theorem? What experiments have been proposed to check this? Have any of them been performed? I know that there are indirect tests of time rever...

 
You could almost do electroweak theory with $U(2)$
 
has had a different answer for like two-thirds of the time since it was posted
 
Because it's like $U(2) \approx SU(2) \times U(1) / Z_2$
 
Kinda makes you wonder what other old semi-canonical questions need revisiting
 
3:14 PM
@Slereah Shit, it really is $\Bbb R^2\times S^2$
 
It is
 
Unless...
 
It's more complicated for Kerr because the singularity is spacelike
 
@ACuriousMind $\Bbb R^3-\{0\}\approx \Bbb R\times S^2$?
seems reasonable honestly
 
If $\approx$ denotes "homotopy equivalent" then yes.
 
3:16 PM
Isomorphism in the smooth category @ACuriousMind
"diffeomorphism"
 
Oh. Yes, I guess that's also true
 
@Slereah HA
 
Well
PROOF???
 
@ACuriousMind I take it back, you're not terrible at geometry
@Slereah Of what?
 
Since removing the point you have that the polar coordinates from $\mathbb{R}_{>0}\times S^2$ cover it and there is a diffeomorphism $\mathbb{R}_{>0} \to\mathbb{R}$.
 
3:17 PM
@ACuriousMind Yes, I know.
I needed someone with pedigree to confirm.
 
On the other hand
Hm
 
Now, is that good for maximally extended too?
 
It's hard to think about Schwarzschild casually
 
I guess look at a Penrose diagram
 
Because it has that weird thing where $t$ becomes spacelike beyond the horizon
 
3:19 PM
@JohnDuffield
 
Nothing but woo
 
It seems to me that the Penrose diagram is $\approx\Bbb R^2$
 
Yes
They suppress angular coordinates
 
And there's a sphere at each point
so it's definitely $\Bbb R^2\times S^2\approx \Bbb R\times(\Bbb R\times S^2)\approx \Bbb R\times(\Bbb R^3-\{0\})$.
 
Well I suppose it makes sense, from Schwarzschild coordinates
 
3:21 PM
@NeuroFuzzy There you go.
 
I wasn't too sure how much you could say from them since they don't cover everything nicely
 
I just picture the spacetime in my mind
but the factor of $\Bbb R$ isn't the Schwarzschild time
it's the
GEROCH TIME FUNCTION
 
:o
 
from the GEROCH THEOREM
So, let's calculate the topology of Reissner-Nordstrom
 
Not too sure about that one
 
3:24 PM
 
I want to say "same", but I dunno
 
Honestly...that looks like $\Bbb R^2$ as well.
@ACuriousMind what do you think
it's certainly an open set of $\Bbb R^2$...
 
I have no idea what you two are talking about
 
Me neither.
 
Is a simply connected open set of $\Bbb R^2$ diff to $\Bbb R^2$?
 
3:26 PM
Yes.
 
Proof?
 
the reader can show
 
Riemann mapping theorem.
This is hard.
 
Could one use Jordan-Brouwer?
 
No idea how you'd do that.
 
3:27 PM
consider the boundary of the thingie
then it encloses a piece homeomorphic to $\Bbb R^2$...
because it's homeomorphic to a disk
 
Oh, you mean Jordan Schoenflies.
 
We don't even really need smooth stuff here
@BalarkaSen ...maybe?
 
Boundary of a simply connected set in R^2 need not be a circle, though.
 
@BalarkaSen open set
what else could it be
 
Chuck the x-axis out.
 
3:30 PM
ah.
Yes, in my black hole case it's not bounded either
 
Chuck a cantor set out.
 
that set continues on to infinity in both directions
@Slereah Well, it's certainly reasonable that it's $\approx\Bbb R^2$ just by stretching it
 
I would beware
It is full of singularities
 
@SlereahBut doesn't RN have like ring singularity shit or is that Kerr
@Slereah but the singularities are on the boundary
they're not a part of the open set
they would be contained in the closure
 
mb
Kerr has ring singularities
 
3:33 PM
Should I post a thing on it on PSE?
 
Since a point singularity can't carry angular momentum
 
I'd get a nonanswer from Timaeus and a diss by JD
@Slereah what does that even mean
 
Points can't rotate on themselves, yo
 
...electrons
we all know they spin, see Einstein-de Haas
 
Not points.
 
3:35 PM
@0celo7 ::twitches::
 
@ACuriousMind yes?
 
I would have thought @0celo7 was better than that.
 
But I'll duck out since I am not a physicist.
 
I'm genuinely confused
I was trolling but people seem to be confused by my non-trolling too
 
btw
there is a nice little proof that, if you allow for torsion
 
3:36 PM
Proof?
 
A black hole with non-0 spin density has no singularity
 
I'll write a question on PSE
The troll answers will be fun
 
Since a 0, 1 or 2D singularity carries no torsion
 
what does it mean for a singularity to carry torsion
I need HE
@ACuriousMind Dammit, I need to start carrying HE with me again
@Slereah haha, holy shit HE references HE
@Slereah what are the various RN thingies called
maximally extended, ...?
er, no
not maximally extended
there's like $e^2>m^2$, etc.
@Slereah what are those called
@Slereah when do you get a ring singularity for Kerr?
clearly $\Bbb R^3-\text{ring}$ is not $\Bbb R^3-\{0\}$.
@ACuriousMind ...right?
@Slereah Is "ring" just some embedding of $S^1$?
 
3:55 PM
@0celo7 Right. The one with the ring is not simply connected, if I understand what you mean correctly.
 
@ACuriousMind Indeed.
I would ask this question on PSE but I highly doubt I'll get an answer
 
0
Q: Problem with questions

heatherAbout five minutes before I posted this, a question came up in the feed asking users to come up with innovative project ideas for a highschool project with a photoresistor. The question had no research, and it was posted originally without a homework tag. While this question was deleted (maybe a ...

 
@PhysicsMeta personnally I like the idea of an addon that electrocutes the OP just before they post crap.
We could use that in the chat room too, though it might decrease the population a bit too much.
 
@JohnRennie ah, can you answer my question
@JohnRennie savage.
 
:-)
@0celo7 What question? I almost certainly can't answer, but just for a laugh I can attempt it ...
 
4:09 PM
Extremal, @0celo7
 
@JohnR I find something oddly ironic about a supposed middle-school student complaining about high-school students asking poor homework questions :^)
 
@Obliv :-) People take things very seriously when they're young. It's only when you get to my advanced age you decide it's much more fun to just bugger about :-)
 
@JohnRennie I have a conjecture
that all black holes are diffeomorphic to $\Bbb R^2\times S^2$.
 
@0celo7 what's $S^2$
 
@Obliv 2-sphere
@0celo7 silly question, but is Minkowski space diffeomorphic to $\Bbb R^2\times S^2$?
 
4:18 PM
@JohnRennie Don't think so.
because $S^2\not\approx\Bbb R^2$.
 
Well the four standard black holes are all diffeomorphic to Minkowksi space
 
No.
 
Why not?
 
you have to remove the singularities from the manifold
 
Yes, so?
 
4:20 PM
wait wait wait
What is the Penrose diagram of Minkowski spacetime
@JohnRennie fiddling with lasers, give me a minute
Suppose I take $S^2$, and for some reason I remove the north pole
then the resulting space is not longer diffeomorphic to $S^2$
and it's really a myth that Schwarzschild becomes Minkowski in the limit $M\to 0$ @JohnRennie
it becomes Minkowski except for the point where the singularity was
(actually it's a 1D submanifold I think)
 
@0celo7 leaving aside time for the moment, I can describe space with the usual polar coordinates $r$, $\theta$, $\phi$. And constant $r$ is the submanifold $S^2$. So why can't I foliate all of space as $R \times S^2$?
 
@JohnRennie The origin.
 
Because $r=0$ is inadmissible
it's not a diffeomorphism there
 
Aaaaaaah. Gosh you mathematicians are sneaky.
 
not even a bijection
I'm not a --- whatever
 
4:27 PM
Penrose for minkowski is a diamond
 
@JohnRennie have you never heard of this before?
the metric in polar coordinates is $dr^2+r^2d\theta^2$
so the volume element is $r$
And at $r=0$ there's a singularity!
But that's just a coordinate singularity
But this also shows that $\Bbb R^2\not\approx \Bbb R\times S^1$.
(for one, they have different fundamental groups)
@ACuriousMind Is their cohomology different too?
de Rham
 
@Slereah a diamond or a triangle i.e. half a diamond?
 
Well, now I'm not convinced that Penrose diagrams are global charts
 
I don't think it matters all that much, since it's just a conformal diagram, but usually diamond
Penrose diagrams are just a spacetime conformal to the one you got, where you bring infinity to a finite distance
 
Wouldn't a diamond imply an extension to Minkowski space analogous to the maximal extension of the Schwarzschild metric?
 
4:31 PM
but my argument would then show Minkowski being $\Bbb R^2\times S^2$ as well
which is wrong
 
Not really?
It's flat space
You can't really extend it
all geodesics already go ALL THE WAY
baby
 
@Slereah That's my point
 
@0celo7 Yes.
 
@ACuriousMind What is the cohomology of $S^1$?
Then you apply that one theorem
...Mayer-Vietoris?
Been a while since I read Lee's cohomology shit
 
@0celo7 Use Poincaré duality and that the homology of spheres is $H_n(S^n) = \mathbb{Z}, H_0(S^n) = \mathbb{Z}$ and zero otherwise. Then use homotopy invariance to contract the $\mathbb{R}$ to a point.
 
4:34 PM
...what
 
I guess you could also use Künneth to compute the cohomology of the product, but that's overkill.
 
Oh, Kunneth
that's what it is
 
Is there a word for "manifold where between two points, there is only one geodesic"
 
@Slereah Hmm
I haven't heard of it
 
Basically axiom 1 of Euclid
I think that means that the normal neighbourhood can cover the whole manifold?
 
4:37 PM
I guess
@ACuriousMind can you please say that slower
 
I think that in those cases, the Hadamard form once renormalized is entirely determined by $\varpi_\gamma(x,y)$
 
I know that all cohomology groups of $\Bbb R^2$ are trivial
 
@0celo7 Nope. The zeroth isn't.
 
@ACuriousMind what is it
 
@0celo7 $\mathbb{Z}$.
Or $\mathbb{R}$, if we're doing real coefficients
 
4:40 PM
Phew, they've gone off on an extended discussion about cohomology so I'm off the hook :-)
 
@JohnRennie this is how GR gets done
 
@ACuriousMind Winding number?
 
@Slereah ?
 
@ACuriousMind Oh, I'm literally retarded
 
Trying to remember how the cohomology works :p
 
4:42 PM
$H^0$ counts the number of connected components
@ACuriousMind Ok, so let's go over this again
We want to calculate $H^k_{dR}(S^1\times\Bbb R)$.
Now you're saying $S^1$ and $S^1\times\Bbb R$ are homotopy equivalent?
@JohnRennie please unstar
that was in very poor taste
 
@0celo7 done
 
@Slereah that's the fundamental group...
@ACuriousMind why isn't cohomotopy a thing
 
All topology looks alike to me
 
5:00 PM
nvm
 
@0celo7 Who says it isn't? (Google "cohomotopy" :P)
 
I guess the simplest way to find out what the terms of the Hadamard form are is to plug them in I s'ppose
Fortunately $\Delta = 1$ in Minkowski space
That's a load off my ass
$$\Box_x \frac{1}{4\pi^2} [\frac{1}{|x-y|} + v(x,y) \ln |x-y| + \varpi(x,y)] = \delta(x-y)$$
Things simplify a fair bit
Hm wait
For the wave equation the Green function is $\delta(t-r)/r$
Is the van Vleck determinant really 1 or is it a delta
 
5:17 PM
shouldn't torque on a dipole in a uniform electric field be $\vec{\tau} = 2\vec{p}\times \vec{E}$?
since the positive and negative side feel the same torque?
 
@0celo7 It is a thing. In appropriate context, cohomotopy is also known as cohomology.
@0celo7 Yes, $\Bbb R^3$ minus ring deformation retracts to a torus, whereas $\Bbb R^3 - 0$ deformation retracts to a sphere.
Torus and sphere are different.
 
vzn
5:37 PM
156
Q: What are some examples of when Mathematics 'accidentally' discovered something about the world?

TrogdorI do not remember precisely what the equations or who the relevant mathematicians and physicists were, but I recall being told the following story. I apologise in advance if I have misunderstood anything, or just have it plain wrong. The story is as follows. A quantum physicist created some e...

↑ via reddit/ hot network question, lots of refs to famous physics cases
...
@0celo7 you might enjoy this, its big on the radio/ top40 right now, found the deconstruction amusing/ deep/ penetrating genius.com/9271412
 
Cellular automatons are great stuff.
 
vzn
@BalarkaSen =D
 
http://physics.stackexchange.com/questions/266426/what-does-the-moons-orbit-around-the-sun-look-like

So does every other satellite have roughly same orbit ? Also does the moons of other planets have rouhly same orbit ?
 
user54412
5:56 PM
@ritwiksinha Roughly, but some of them are more exotic. Note the spiraling pattern everyone mentions is not what the Moon looks like. Well, Jupiter's orbital speed is 13 km/s, while its moon Io goes around at 17 km/s. Thus for part of its orbit Io is in fact going backward around the Sun.
 
6:11 PM
@ChrisWhite Do you know what the topology of a generic black hole is?
156
Q: What are some examples of when Mathematics 'accidentally' discovered something about the world?

TrogdorI do not remember precisely what the equations or who the relevant mathematicians and physicists were, but I recall being told the following story. I apologise in advance if I have misunderstood anything, or just have it plain wrong. The story is as follows. A quantum physicist created some e...

Physics is not mathematics.
@ACuriousMind So do you now know something about M theory?
 
user54412
@0celo7 spherical?
 
user54412
3
A: Gravitational lensing image from merging black holes

Chris WhiteNot even light can pass through a toroidal black hole before the hole closes up, so the question is moot. To set the stage for why toroidal black holes are interesting, I'll start with Hawking's 1972 result that "a stationary black hole must have topologically spherical boundary." That is, once ...

 
user54412
Unless you're including the whole thing inside the horizon too. In which case, are they supposed to be the same?
 
@0celo7 yes
 
vzn
@0celo7 did you read any of the answers?
 
user54412
6:19 PM
@0celo7 Halfway down the page and I haven't found any accidental examples. Apparently mathematicians think anything a physicist does is accidental :/
 
@Qmechanic Welcome back! I miss you! :-)
 
@vzn yes
most of them are random physics things
@ACuriousMind so what is it
 
vzn
@ChrisWhite your use of the word "accidental" seems not to match that used/ interpreted
 
@0celo7 Nobody knows!
 
vzn
am a bit surprised you guys dont like the question/ answers, its like a big ad for physics on the math site, and youre all kneedeep in math etc, it highlights/ unifies key discoveries etc
 
6:23 PM
@ACuriousMind That's a thoroughly dissatisfying answer and you know it.
 
@0celo7 But it is true
M-theory is the conjectured theory of which all known string theories and 11d SUGRA are particular limits.
But no one knows what that theory is
 
hmm
when I am retired I will revisit this @ACuriousMind
 
Some of its objects - like the M2- and M5-branes - are known by finding their corresponding objects in the limiting cases and noting they are stable against smooth deformations ("BPS states")
 
@lucas : Thanks. I'll be officially back on Sunday.
 
BPS state?
 
6:27 PM
@0celo7 That's what one calls these states that are safe against perturbative corrections and hence should still be present in the full non-perturbative theory
They usually fulfill some extremality condition
Kind of like the masslessness of a vector boson in QFT- also an extremal mass condition - inherently protects it against acquiring mass
 
@MAFIA36790 Pokemon GO is the top free app in the app store
But not a single advertisment for it anywhere
quite impressive, really
@ACuriousMind what does that mean
@ACuriousMind I don't know anything about massless vector bosons...
 
@0celo7 I'm not sure how to answer that briefly. There is usually a significant function of mass and charge of an object associated to that object, and there's something special about when this function becomes extremal - for example, the number of the allowed fields living on it change, and this cannot be a smooth transition, so if the object is sitting there at weak coupling it must also be there at strong coupling.
@0celo7 You do not know that all massless vector bosons are gauge bosons and protected from acquiring mass by gauge symmetry? Shame on you! ;P
 
@ACuriousMind No, I'm not a physicist.
All I remember from the QFT days are pain.
QFT was enough to make me hate all of physics, do you really think I know anything about it?
I'll revisit it after my grad course on QM. If it's still beyond me I will conclude I'm not smart enough for it.
 
@ACuriousMind I'm saying it's a path integral
Just to bother all the people who told me UGH STRING THEORY ISN'T AN ACTION THEORY
 
@ACuriousMind Although I will say I understood Timo's notes on it just fine
But as soon as people start talking about irreps my brain aneurysms
 
6:38 PM
@0celo7 is it the math that bothers you?
 
I think his notes were relatively group theory free
@Obliv I do not understand representation theory.
And I've come to despise it so I never want to learn it.
QFT books make me feel like an inferior human being.
Hard math books make me feel like I have a lot to learn.
 
@0celo7 That's because the second-half of QFT2 is missing from them where we discussed anomalies and instantons and symmetry breaking :D
 
Hard physics books just make me feel like shit.
 
Isn't representation theory just a morphism between whatever group and a subset of $M(n)$
 
@Slereah What the heck does that even mean?
 
6:40 PM
I'm saying it's an action theory
 
No, according to Weinberg it's $D_{\sigma\sigma'}\Psi$ shit.
 
Bam
 
Or something.
 
Can't prove me wrong!
Until u prove M theory
 
And Zee says it's something with transformations, I don't even know.
 
6:43 PM
@Slereah What?
 
Am I the only one who feels this way?
 
A single representation is a group morphism from the group to the group of automorphisms of some vector space
If you mean matrices with $M(n)$, then you have excluded all infinite-dimensional representations, in particular the entire quantum theory of the Lorentz group :P
 
@ACuriousMind Why not just say a homomorphism to $\mathfrak{gl}(V)$
 
@0celo7 It would be $\mathrm{GL}(V)$ (we're talking groups not algebras), and how is that different from what I said?
 
@ACuriousMind Operators are nothing but continuous matrices
 
6:46 PM
@0celo7 What way?
 
That's right I said it
 
If you mean feeling like physicists are shit at explaining group theory, then certainly no
 
@ACuriousMind Hard math is motivating but hard physics destroys the soul.
 
@0celo7 I'd guess other mathematicians might also feel that way!
 
I'm not a mathematician.
 
6:48 PM
Hm
Thinking about it
I guess the first two terms of the Hadamard form might describe like
The local behaviour of fields?
 
What are you talking about now?
 
Since the first one is $\approx 1/r$ and the second one is $\approx \ln r$
 
Do I want to know?
 
5 hours ago, by Slereah
So the Green's function in curved spacetime is $$G(x,y) = \sum_\gamma \frac{\Delta_\gamma (x,y)^{\frac{1}{2}}}{4\pi^2} [\frac{1}{\sigma_\gamma(x,y)} + v_\gamma(x,y) \ln |\sigma_\gamma(x,y)| + \varpi_\gamma (x,y)]$$
This
 
Proof?
 
6:50 PM
Well I'm trying to find the proof
It's somewhere in there
 
is there no reference in the book you're reading
 
Not in the same notation, no
it's a bit tricky to find
 
@ACuriousMind I wouldn't make a good mathematician either
I get bored too quickly by things
So this is a thing.
 
But considering that $1/r$ is the solution in $d>2$ and $ln r$ is the solution for $d=2$
I'm guessing that's where those terms come from
 
@Slereah By "the Green's function" you mean the Green's function of the d'Alembertian?
 
6:53 PM
what is $\varpi$?
@ACuriousMind ON CURVED SPACETIME
 
@0celo7 I don't see why I wouldn't call it the d'Alembertian in curved space, if that's your problem
 
Well because it's not called the D'Alambertian in curved spacetime
It's called the Laplace Beltrami operator
Also I'm not quite sure if it's the Green's function, reading up on it?
It's an old timey book so it's hard to read the notation
Hm, lemme thing
 
@ACuriousMind On a general Lor. mfld. the wave operator is just the Laplacian.
 

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