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6:01 AM
choquet bruhat or something
I will read that book one day
one day...
@DavidZ how's the HEP life?
@Slereah how are you deriving the EFE?
 
By fiat
"These are the EFE"
 
@0celo7 Don't be silly, the John Rennie account is really a sockpuppet for Miley Cyrus.
 
@0celo7 busy as always
I'm procrastinating preparing a talk I have to give in two days
 
GR isn't the focus of the book, it's causality!
really for most of the first chapters the stress energy tensor doesn't matter much
except for energy conditions
 
@DavidZ is it a good talk
@JohnRennie Miley....I love you
just want you to know that
 
6:16 AM
@0celo7 Just don't tell my fans I'm really a physics nerd
 
@JohnRennie jiggle physics
 
The wrecking ball video was originally intended as a tutorial on the Lagrangian approach to compound pendulums
 
I listened to wrecking ball on the radio today
it's actually a good song
 
@0celo7 I mainly listen to metal and psychedelia, but then hey I'm a child of the seventies ...
Oops, my cover story might have slipped a bit there :-)
 
6:20 AM
@JohnRennie I mainly listen to hard dance and rap.
 
Hey look
It's a gentle introduction
 
But then hey I'm a child of the internet.
 
@Slereah What book?
 
@JohnRennie the one he linked?
@Slereah pls don't do category theory GR
@JohnRennie I have a strange-ish question
obviously you know a lot about GR, but how much do you know about the abstract formulation of the mathematics?
 
@0celo7 : No that would be silly
it's to do category theory QM
 
6:22 AM
i.e. do you know what is means for the Christoffel symbols to be in the jet bundle
@Slereah y
 
Because apparently AQFT is used a lot in GR
 
Spivak
The name is familiar
 
anyway, I'm off to bed
 
What did he do
 
6:24 AM
@Slereah like a 6 volume series on diff geo
+ an analysis book
 
oh yeah
 
@0celo7 Aha, thanks.
 
@JohnRennie for?
that's not what @Slereah was referring to
 
@0celo7 ah
 
but I might take a look at it one day
check it out from the library and peruse it over a weekend
 
6:28 AM
Oh well, I have to start work now. It's 06:30 here in the UK :-)
 
heheh
The title of an intro to category theory
"Introduction - How do I remove the numbers"
"Mention various people."
I think this is a draft
 
@0celo7 who knows, I haven't given it yet
 
"You will also find in the literature that some people write `A' for the arrow $id_A$. This is a notation so ridiculous that it should be laughed at in the street."
 
6:46 AM
what is "CME"
 
can anyone understand this lousy english sentence of mine ? ---> "now we take the observer who measures into a new system"
 
as a physics graduate school topic to admit for
 
condensed matter experiment?
 
ah, good guess
thanks
 
@Shing yeah, it's understandable, I think: there is an observer who measures something (perhaps as opposed to other observers who don't measure anything) and they are changing systems - presumably it's clear from the context what constitutes a system
 
6:50 AM
La Gage's gravity problems were not asked properly before; physics.stackexchange.com/search?q=Le+sage%27s If there were some answers, they only referred "drag" physics.stackexchange.com/questions/211585/… or the level was very low like physics.stackexchange.com/questions/26692/…
So, I feel this question physics.stackexchange.com/questions/220050/… should be acceptable question, at least after my edit
 
@DavidZ Thanks for the help, I think I should add "without change anything" anyway to avoid confusion.
 
Testing how to write something as a tag:
Nope.
OK. Got it now.
 
There's also [meta-tag:tag]
 
@DavidZ But that didn't work.
Anyways, I was wondering why do we have on Meta.Physics.SE?
 
Huh, maybe it's only in comments. But I thought something like was possible. edit: it is
 
[meta-tag:data-dump] ->
It's supposed to be for the periodic releases of the SE database, a.k.a. the "data dump"
It might be a default tag that exists on every meta site?
 
Aha. But no guidance, no questions?
Absolutely nothing at all on our site.
 
Guess not. I don't think we have much of a need for it.
 
So, we still have it only because it is there by default?
 
Presumably so
Though note that you can link to anything as a tag. e.g. , it doesn't mean the tag actually exists
 
7:04 AM
OK. That prevents a meta post :P Thanks.
 
@DavidZ: do we know who the Daniel Sank conspiracy nutcase is?
Incidentally he's just added aanother post you might want to delete
 
@JohnRennie we know some relationships between the accounts that have been posting
 
got it
 
You tyrant
 
7:19 AM
I suppose that there are a good number of people that has nothing useful to do in their day... apart talking nonsense of course T__T
anyhow the electromagnetism tag is interesting...this is because DS controls minds and does harm by means of very potent EM emitters? superconducting magnets?
 
lol, who knows
oh, I think maybe we'd better keep these excerpts off the star list
 
@0celo7 That's not a cop out at all.
@ACuriousMind "restricting the domain of discourse from the beginning to consequential morals (as you seem to me to do) is therefore a mistake, in my opinion, because you first have to establish that morality is indeed decided by the actual consequences."
I think there is no issue of "establishing" that morality is decided by the actual consequences; this is, rather, a matter of how we decide to use the word "moral" (and derived words).
 
7:35 AM
@SirCumference-Pies it seems to me the answers to that question pretty much cover it. What extra info are you looking for? Something like:
21
A: Would the inside of a black hole be like a giant mirror?

John RennieLight cannot move outwards inside the event horizon. I would guess you're thinking that an outgoing light ray might leave you in the outgoing direction, then slow to a halt and return - hence you would see yourself. However this doesn't happen. The light leaving you moves inwards not outwards, bu...

 
I cannot think of a notion of "absolute" or "logical" morality which I think is worth wrapping up in a single, commonly used word.
If you can provide one (which doesn't degenerate upon inspection into religious doctrine), then I'll have a change in perspective.
My approach to morality and in particular what that word should even mean is influenced mostly by which notions are actually well formed.
I will not argue that my notion of morality is the better one as compared to Kant's because I think Kant's "isn't even wrong".
 
 
2 hours later…
9:09 AM
I'd better make a shortcut for $\textfrak{A}$ too
Too bloody long
 
9:27 AM
@Slereah I have an SR question
So basicaslly here in minkowski space I have observers B, O A
and I then plot the light cones for B and A at different points of their worldline
I then noticed that for B , the rays that intersect the t axis of O seemed to pile up (which seemed to correlate to how B is travelling very close to c)

and for C it occurs at a less extent
Suppose the observer measure a small time interval in his rest frame say for 5 proper seconds, then we should expect that interval would be 5 light seconds long and would basically be a vertical arrow of 5 units in the diagram
 
That would be the Doppler effect
 
i then noticed the arrows made by the rays of obversers B and A are shorter than the 5 unit long vertical arrow that could have been obtained if O is measuring 5 light seconds of time

Is the ratio of the length of these red arrows with O give the time dilation between O and the corresponding observers? (and simialr the blu arrow give how much things are length contracted)

If the signal is light then is the "bunching" of these rays give the doppler effect?
 
^ Doppler effect
 
Nice zebra costume
The bunching is the doppler effect, yes
 
10:06 AM
Hmm, It seems my interpretaton that the red arrows measure time dilation is wrong, since here it gives the same arrwo length (the time interval between the receiving of the 1st and 4th light signal as measured by O)
In that case, better get back to the maths to see what this diagram mean
I can still see the doppler effect on the far right ,though
@Slereah I am guessing the horizontal spacing of the cones measures the wavelength of the light from E as observed by O (due to doppler effect), but what does the vertical spacing told us?
 
the time between the reception of two wave packets
The talk page of wikipedia on AQFT : "The page is written in the language of category theory. I suggest that many people who would be interested in the Haag-Kastler axioms don't speak that language."
Who knew a theory entirely based on category theory would be written in category theory
 
however I agree that who works on AQFT either do not know anything about physics, or do not know so much about category theory
 
10:25 AM
wot
 
I know two types of people that work on AQFT: mathematicians, and they do not know anything about physics (and essentially use AQFT as an excuse to do category theory); and (not so many) theoretical physicists who usually do not have a research-level knowledge of category theory
but that is just in my experience
 
It ain't easy
 
of course it isn't, but from a physical standpoint it did not yield many interesting results either
 
10:42 AM
So
Which one is Haag
Apparently it's useful for QFT in GR but I still don't know why
 
Have we got any Mathematica users in the room? I want to ask what some Mathematica notation means ...
 
I am, somewhat
 
Does this mean d/dr of the expression?
 
maybe...but I think that we are far away from mathematically understanding QFT, and I have the feeling that AQFT, despite being interesting, is not the solution
 
i.e. d/dr(\sqrt{1-2M/r})
 
10:54 AM
@JohnRennie I think so?
Although it's hard without more context
Could be $\partial_M$ for all I know
Nothing singles out $r$ as a variable out of context in Mathematica
Oh wait
I think the variable might be, without more context, directly $1 - \frac{2M}{r}$
 
I'm using Hartle's Christoffel.nb notebook to try and calculate the Christoffel symbols for the Schwarzschild interior metric. I get ...
 
Yeah, I checked
Sqrt'[something] does the derivative wrt to the content of the brackets
So it should be $\frac{1}{2\sqrt{1 - \frac{2M}{r}}}$
 
@Slereah Thanks, that's what I guessed.
 
11:18 AM
I've got a thing to compute GR tensor if you want
Probably not the best optimized code but it's fine
 
12:03 PM
I've also got a decent thingy for that stuff
@JohnRennie Yes it does mean that
 
12:24 PM
I am still sad...
T__T
one day to refer and accept the paper...
and it is uninteresting, to say the least
and my two papers on the same journal took $\sim 1$year per paper on average to be accepted
damn peer review process!
 
What do you guys think of Penrose's criticisms of inflation? They are basically ignored in the literature
 
I argue that color is one of the best way to illustrate superposition, because (as far I know) it and sound waves are the only things which the superposition is perceived as something all by itself instead of "simply a stronger or weaker intense thing" or "putting two different things together and still can tell there are two things being put together"
 
12:52 PM
What the hell is motion, really..?
 
@Slereah did you really not sleep
 
user116211
1:46 PM
Sorry for disturbance but couldn't keep myself to share it. The funniest & one of the wittiest profile infos : "Well i am a school student from India whose science teacher can't explain a shit so i depend on physics stack exchange I am simply thankful to one who created this website" .
 
@JohnRennie assuming that's a prime, it means the derivative of sqrt. Just like how you'd write $f'(1 - 2M/r)$, where $f'(x) = df/dx$, except that here the name of the function is sqrt instead of f.
Note that the square root function in Mathematica is Sqrt with a capital S. One would hope that sqrt is defined with the same meaning though....
 
2:08 PM
@DavidZ Thanks. I'm attempting to use Mathematica to calculate Christoffel symbols, and since I have never used Mathematica before and my grasp of differential geometry isn't stellar it's proving an interesting experience :-)
 
@innisfree I think Penrose is not really taken too seriously anymore nowadays.
Mostly because of his weird opinions on non-strictly physics matters.
@JohnRennie Hey JR, I have a really simple thing to calculate GR tensors.
 
@Danu Don't you mean strictly non-physics matters? ;)
 
@ACuriousMind Not according to him ;)
@JohnRennie It's just a few lines of definitions that you actually paste into the .nb, (so no black box!) and it works like a charm to calculate the usual tensors.
 
2:21 PM
@Danu Tsk. You're calculating the components.
 
@0celo7 You're "tsk"-ing me with regards to differential geometry? Tsk.
 
Fight me.
 
@DavidZ I don't think sqrt is defined in Mathematica. Everything goes with caps.
@ACuriousMind Why does the statement that the conserved charge associated to a local gauge symmetry is gauge-dependent and hence unphysical lead to the statement that "gauge symmetry cannot be broken"?
I'm asking you because you're supposed to be our gauge theory dude here.
 
@Danu Breaking a symmetry means that the solution to the equation of motion (or "the vacuum state", or whatever you want to call it) is not invariant under the respective transformation. But the fundamental principle of gauge theory is that all physical states are gauge-invariant.
 
That's a decent statement.
But it does not directly tie in to the charge being unphysical. Is there a more direct argument?
I'm asking because my TA kept on saying this, but I don't really see how
 
2:38 PM
@Danu it's not a builtin function, but it is defined (it shows up in black in the screenshot)
 
@Danu Ah. See this answer, the conserved charge becomes non-conserved and is essentially the Goldstone boson of the symmetry breaking. If the charge is unphysical, you don't get the Goldstone boson, and the d.o.f. of the broken symmetry just vanished into nowhere.
 
@ACuriousMind Thanks a lot.
 
3:25 PM
@ACuriousMind Back to the Lie group thing, how is $X(g)$ defined again?
i.e. given some vector field $v$ on $G$ how does one find the vector whose left translation to $g\in G$ is $v$ at $g$?
 
@0celo7 It's $v(e)$.
 
@ACuriousMind lol
derp
$dL_gv(e)=v(g)$
thanks
 
 
2 hours later…
5:22 PM
@Danu Cool, can you put the code somewhere I can find it? I've been using Hartle's package from:
and it seems to work for the Schwarzschild metric though I'm struggling to convince myself it's giving the correct answer for the interior metric.
 
user54412
6:00 PM
@ACuriousMind I've heard some bilingual philosophers choose an English translation, since the translator has had a chance to improve Kant's writing for the better. You have to have some faith in the accuracy of the translation, but on the other hand for German you would have to have faith that you aren't putting erroneous 21st century meanings to an 18th century text.
 
user54412
I suppose this is an issue that comes up with any old text.
 
trying to manipulate Lie group things when there are three points and integrals and forms and derivatives involved is turning out to be not fun
 
user54412
Did Hartle really compress a small plaintext file? Some people shouldn't be allowed near computers.
3
 
what's the issue?
 
6:19 PM
@0celo7 Went to bed at noon in the end
 
weakling
 
I'm an old man :(
Hey @ACuriousMind
There is totally a set theoretic definition of categories
Apparently using the Groethiendieck axiom
⊢ ∃y(x ∈ y ∧ ∀z ∈ y (∀w(w ⊆ z → w ∈ y) ∧ ∃w ∈ y ∀v(v ⊆ z → v ∈ w)) ∧ ∀z(z ⊆ y → (z ≈ y ∨ z ∈ y)))
 
@Slereah I didn't say there wasn't, I said you shouldn't think about it that way and that most people just ignore the set-theoretic issues
 
Yes, WEAK PEOPLE
also apparently the original Haag paper didn't use category theory at all
It was all Algebra
 
@ACuriousMind so, now that I actually do this exercise
 
6:25 PM
@Slereah The proper category theorist founds set theory on category theory, cf fully formal ETCS ;P
 
I don't see why the volume form has to be right invariant at all
 
@ACuriousMind : Well I think all foundations of mathematics is expressible in terms of one another
I think that's a theorem of like
computation theory
 
@ACuriousMind Left invariant of the new metric follows from left invariant of the old one...and right invariance follows from left invariance of the volume form math.stackexchange.com/questions/72333/…
 
Set theory is expressible as $\mu$-recursive functions and vice versa
$\mu$-recursive functions are expressible as $\lambda$ functions
etc etc
⊢ Cat = {x ∣ ∃d∃c∃j∃r(x = <.<.d, c>., <.j, r>.>. ∧ ((<.<.d, c>., <.j, r>.>. ∈ Ded ∧ ∀f ∈ dom d∀g ∈ dom d∀h ∈ dom d(((d ‘h) = (c ‘g) ∧ (d ‘g) = (c ‘f)) → (hr(grf)) = ((hrg)rf))) ∧ (∀a ∈ dom j∀f ∈ dom d((c ‘f) = a → ((j ‘a)rf) = f) ∧ ∀a ∈ dom j∀f ∈ dom d((d ‘f) = a → (fr(j ‘a)) = f))))}
A category, apparently
 
@Slereah Tell me again how that notation is useful? :P
 
6:28 PM
Isn't that much nicer than whatever you're using
Yeah that one gets a bit too long :p
 
@0celo7 Why are you telling me this?
 
And that's not even exactly true
Because the guy had to decompose the definition
 
@ACuriousMind because I need help?
 
$Ded$ had to be defined first
Ded being
 
@Slereah why would anyone do that
 
6:29 PM
⊢ Ded = {x ∣ ∃d∃c∃j∃r(x = <.<.d, c>., <.j, r>.>. ∧ ((<.<.d, c>., <.j, r>.>. ∈ Alg ∧ ∀a ∈ dom j((d ‘(j ‘a)) = a ∧ (c ‘(j ‘a)) = a) ∧ ∀f ∈ dom d∀g ∈ dom d(<.g, f>. ∈ dom r ↔ (d ‘g) = (c ‘f))) ∧ (∀f ∈ dom d∀g ∈ dom d((d ‘g) = (c ‘f) → (d ‘(grf)) = (d ‘f)) ∧ ∀f ∈ dom d∀g ∈ dom d((d ‘g) = (c ‘f) → (c ‘(grf)) = (c ‘g)))))}
 
you have got to be kidding
that's not real
 
It totally is
There's a small community of crazy people that tries to prove math theorems entirely from syntactic proofs
 
@0celo7 And...I'm supposed to have your exercise from two days ago or so saved somewhere? You'll have to refresh my memory :P
 
@ACuriousMind Yes.
I have proved left invariance. Right invariance is proved in the MSE post. Nowhere is part (a) used.
That's the proof of left invariance.
 
And you need help with what?
 
6:36 PM
He needs help for everything
For he is just a baby
 
@ACuriousMind Do you agree with my proof for left invariance?
@Slereah No
@Slereah Maybe?
I agreed with it until I completed the whole thing and I never used part (a).
Maybe I'm missing some subtlety?
 
Hey @ACuriousMind
Why are the plane and hyperbolic space not conformal according to the uniformization theorem
They're both $\Bbb R^2$ and both of them have a metric $g = f(x) \delta$
 
@0celo7 The proof is correct, but you define $f$ but never use it, and you don't really show where you use that $\langle\dot{},\dot{}\rangle$ is left-invariant.
 
@ACuriousMind I define $f$ for the proof of right invariance.
And the other objection: proof is in the book
 
@0celo7 The math.SE proof used a change of variable approach, which is basically equivalent to showing that left-invariant things are right-invariant things.
 
6:44 PM
wait
 
The exercise just intends you to use right-invariance there and not apply the change of variable thing
 
I use left invariance after "we see that"
@ACuriousMind o
 
@0celo7 Exactly, but you don't say it, that's why the "we see that" is a bit unclear to someone who doesn't know how the proof is supposed to work
 
@ACuriousMind ah
 
@Slereah Because the hyperbolic space is conformally equivalent to the open unit disk?
 
6:46 PM
I'll add in another step and explain
thanks
 
Isn't the open unit disc the same topology as $\Bbb R^2$?
 
@Slereah So?
 
what's the difference between the two metric?
Aren't they conformally related?
 
The uniformization theorem says there are three conformal equivalence classes: The open unit disk, the plane, the sphere.
 
Or am I using a too physics definition of "conformal"
 
6:47 PM
Hyperbolic space is in the open unit disk, and the plane is, well, the plane
 
What's the difference between the open disk and the plane outside of the geometry?
 
@Slereah I don't understand where your confusion lies at all - hyperbolic space is not the plane. There are several models of it, but none on the full plane
 
I dunno
I guess it's because in GR, you usually consider manifolds to be the same if they are homeomorphic
 
@Slereah *diffeo
 
w/e
 
6:49 PM
Let's turn it around - what do you think is the actual map under which they are conformally equivalent?
 
@ACuriousMind that's unfair
why did people star by dead bird comment
 
$ds^2 = dz d\bar z \rightarrow ds^2 = \frac{dz d\bar z }{Im(z)}$
 
wonder if they cleaned that up
 
Or something
 
@0celo7 No, if someone asks me "Why isn't $A\cong B$?", it's a completely fair question to ask "Why do you think it should be?"
@Slereah That's not a definition of a map
 
6:50 PM
Hm
 
@ACuriousMind what?
 
You need to give an actual conformal map $f : H\to\mathbb{R}^2, z\mapsto f(z)$.
 
that's the definition of a physics map
 
@0celo7 No, definitely not. Just writing down two metrics does not define a map at all
 
@ACuriousMind wonder if I can find some book that disagrees
 
6:51 PM
A map is defined by mapping every point of one space to one point of the other.
@0celo7 People sometimes omit writing down the actual map if it is "obvious" and they are mostly interested in the metric
But that doesn't make writing down two metrics a definition of a map
 
I'm not disagreeing with you for the record
 
Isn't there always a map between a simply connected open set of $\Bbb R^n$ and $\Bbb R^n$
 
@Slereah doesn't have to be a conformal isometry
 
@Slereah: Also, you should fix the model of hyperbolic space you're working with - upper half-plane, Poincare disk, projective space?
@Slereah No (at least not a homeomorphism, much less a conformal equivalence)
 
Well it is usually given as the open disk
 
6:54 PM
@ACuriousMind ._.
 
$(D^2 , \frac{dzd\bar z}{Im(z)^2})$
I guess I have too much GR definitions in me brain
 
@ACuriousMind I thought any simply connected open set of $R^n$ is homeomorphic to a ball...is that wrong?
 
@0celo7 Yes, we've been over this before.
 
the fuck
where?
I would have bet my life on that
 
"However, I must admit that his discussion of the "many worlds" in quantum mechanics, which Brian considers "inevitable", along with all of his thoroughly irrational attacks against the proper Copenhagen quantum mechanics, was driving me up the wall."
Motl really takes things too seriously
 
6:58 PM
ah
the annulus
@Slereah No
 
Well yes, you say that now you fake :V
 

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