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20:00
@Blue Ikr, but I'm considering a math double major and analysis is a requirement
Anonymous
If the mangoes you ate were awful then those were not "real" mangoes
@Blue No True Mango?
@0celo7 Is it worth buying? I've an interest in stuff like that, but it's not relevant to my work/PhD
@0celo7 Complex analysis on the other hand, apparently is :P
@Mithrandir24601 I use it all the time but I'm a GR guy. Also I got it for Christmas some years ago.
i wish mangos came in banana form, easy to peel
20:01
It is the best GR $\cap$ physics book, IMO.
Though tbh, the math requirements are supposedly as hard as the physics classes, which are by far my most demanding classes
@0celo7 Hmm... I'll have a serious think about it... I've spent far too much money this week already, but £16...
@Mithrandir24601 Oh yeah, get the cheap one
I got the expensive one
Yeah, there's no way I'm spending >£200 on a book that's not even relevant
20:03
@Mithrandir24601 Not relevant?
It's the second most cited GR book after MTW.
It's still a good reference.
@Blue I'll be honest, I'd have no time to study all that course information on my own. Not to mention it wouldn't grant me the same understanding as a uni class would.
Anonymous
@SirCumference I think it'd help to talk with the analysis lecturer and ask him whether he can guide you through analysis separately (beyond class hours). He/she should probably help you out. (That's exactly what I do when I have clashing timings)
@0celo7 For what I'm doing (PT-symmetric Hamiltonians)
@Blue I thought about doing that, but when I checked who the prof was, it just says "Staff"
No other class does that...
@Mithrandir24601 It includes some great disses
He basically calls everyone out on their bullshit that spacetime is actually curved, saying that doesn't even make sense
20:05
Ocelo7 can you elaborate on that?
why doesn't it make sense?
It's getting very tempting...
Anonymous
@SirCumference Perhaps wait for the classes to start. You'll come to know. Register for the one which you find more useful for the time being
@pZombie "Spacetime" is a model. You can't point to it. It's a made-up thing
It represents reality, it is not actually reality.
We do not "live in a curved manifold"
@0celo7 Oh, pedantry
Any time I've looked at astronomy books, the hand-waiving put me off
20:07
@SirCumference In the 70s when people thought they could put GR in a QFT framework it was an important distinction. Quite important.
Ocelo7 - everything is model. That's true. It's how we imagine things to be, based on the local experiences we have, some models seem to predict better than others
Maybe after I read Weinberg's Cosmology I'll be able for the hand-waiving
Because once you decouple the math from the physics you can try to make a better model.
And that is the moral of the story.
Don't star that you fools
Anonymous
Lol
if you don't want people to star s*** you say, maybe say less s*** :P
4
Anonymous
20:09
Lemme flag the "you fools" message now :'D
@Semiclassical It's actually not stupid shit. I was more concerned with the "insanity" part. Is that what you were referring to?
I do believe that John Duffield had some good intentions. Most of what he said was nonsense, but every now and then he made a good point.
s*** is probably over the top
but if you say something here, you assume the risk that someone else will star it
what good point has he made
@Slereah Spacetime isn't in the night sky
Hmm, maybe I should just take the non-honors version
20:11
Well, that's true I guess
That is code for "don't forget that GR is just a model"
I don't think he understands that himself
GR is actually an approximation. There's no reason why there aren't higher order terms in the equation, but we just say they're small for reasons.
The reason is that we don't measure them to be within experimental error
@0celo7 It's somewhat 100% accurate
20:12
@Slereah we don't really have that many tests of GR
uhh
we've got a few
@SirCumference that's very ignorant
@Semiclassical modulo LIGO they're all in the very weak regime
as in, it's close enough to reality that we might as well call it "reality"
Tests of general relativity serve to establish observational evidence for the theory of general relativity. The first three tests, proposed by Einstein in 1915, concerned the "anomalous" precession of the perihelion of Mercury, the bending of light in gravitational fields, and the gravitational redshift. The precession of Mercury was already known; experiments showing light bending in line with the predictions of general relativity was found in 1919, with increasing precision measurements done in subsequent tests, and astrophysical measurement of the gravitational redshift was claimed to be measured...
for reference
oh and there was the binary pular experiment
20:13
you wouldn't be a good physicists if you ever called some theory to be real
I have the modern ones more in mind
or ever believed in direct observation. Never happened
The Shapiro delay effect is pretty cool
@Semiclassical I think I'm familiar with all of them. The pulsar one is strong gravity, but we still don't have direct observations of black holes.
define direct observation
20:15
if you mean that one is only testing a leading effect of GR, though, I see your point
@Semiclassical That is exactly what I am saying
We don't have enough strong regime experiments to rule out any kind of f(R) gravity, AFAIK.
I imagine there's at least some constraints on the size of the possible corrections, but some constraints != strong constraints
And GR isn't quantum, so it's certainly not "reality".
and quantum is not GR so it is not reality either
Correct. Although QM is more of a foundation for reality than GR is.
20:17
I'd put my money on quantum being more basically correct than GR, yeah
An LQG-ist might disagree
i wouldn't put much money, mind
@0celo7 We have plenty
Have u not read that great book
By Samuel Lereah
both are good theories in the sense that they allow for useful predictions, but they are both incomplete
Anonymous
20:19
@pZombie That's probably true for every theory in physics :P
well, screw physics
heh, look at the title/author of this paper: adsabs.harvard.edu/full/1970CoASP...2...35T
and then look at the publication date
How do I become a good cosmologist like @Slereah
Am I a good cosmologist
I basically don't remember anything about cosmological models
I think?
20:23
@0celo7 I guess the real question is how small of corrections we'd reasonably expect to exist
I mean I could look it up I guess
but on the spot
I don't think I remember much
aren't you a cosmology student?
@Semiclassical well, the classic argument is that if you want a term like $Riem\cdot Ric$ in the field equations, you need a coupling constant with some strange dimensions
and then you make out out of the planck units and it's tiny compared to $G$
so you just declare it zero
hmm
so the scale you'd need to look in order to see corrections is huuuuge
20:25
yeah or small scale with huge energy
which I'm guessing is what you had in mind with that R in f(R)
f(R) gravity just means the Einstein-Hilbert action is $\int f(R)$
regular GR is f(R)=R
I find it hard to get excited by beyond standard model physics, whether that be the standard model of particle physics or GR as the standard model of gravity
20:27
same
because it ends up being so hard to test
the one exception to that is neutrino physics. that's genuinely cool
hard to test and anything harder than the Einstein equations makes me want to cry
@Semiclassical protip: If you want to star something like that, wait until it's not removable/editable and then do it ;)
3
@0celo7 Wait, do you like cosmology?
20:28
Guys can someone help me out with a sanity check on index notation : $(\partial_a T_b) M^aM^b + (\partial_a T_c) M^aM^c$. Can I swap the $a$ index in the first expression to a $c$ and the $a$ in the next expression to a $b$?? I am having a massive brain fart as I just woke up and am wondering does it have to be the same change for the entire expression!!
yes
yeah, you're good
@SirCumference idk, why
@0celo7 Curious
is inertial mass an emerging property?
or is it something inherent elemental particles are supposed to posses?
20:30
Aw good!! I answered a question like this last night and then when I woke up I doubted whether I was right and didn't want lead someone down the wrong path! Cheers!
Anonymous
the tricky thing is that, absent a theory which puts QFT and GR on the same footing, it's hard to say that we've fully explained the origin of mass
i think a lot would reveal itself if anyone actually tried to write an accurate relativistic particle simulation even if it would be able to simulate just a fraction of a nanosecond. By accurate, i mean one that could be set to arbitrary accuracy, sacrificing simulation speed.
@Semiclassical time for fortran ;_;
god help you
20:40
no simplifications should be contained within the simulation
the most general case
@Semiclassical it's just asking me to implement RK4
seems like it shouldn't be the end of the world
no
but i imagine it's not without its headaches
I'm sure I'll learn some new things about fortran in the process however
like the god damn formatting
@Semiclassical without looking, what is the golden ratio
1.618...?
it's something like $\frac12(1+\sqrt{5})$
@Semiclassical Yeah I got a 95 on one of my fortran homeworks because I said that. The prof swears it's 1/ that
20:48
well, to be fair, 1/1.618 = 0.618
yes, it's a bit strange that way
but phi >0 is pretty solid
pretty solid?
i mean that phi being greater than 1 and not less than one is something I'm pretty confident in
me too
wonder how he will respond
my code is right if you use his wrong definitions
@Semiclassical are you a linux guy?
20:52
lolnope
@Semiclassical erm, how would I solve $y'= 2e^{4x/5}+3y$ analytically
well, $y'-3y=\frac{dy}{dx}-3y=e^{3x}\frac{d}{dx}(ye^{-3x})$ I think?
ah yes, integrating factor
thx
so therefore that's equivalent to $\frac{d}{dx}(ye^{-3x})=2 e^{4x/5}e^{-3x}=2e^{-11x/5}$
in which case yeah
I had the integrating factor idea in mind, i just was able to do it by inspection here
for some reason I thought you had to have homogenous for that to work but apparently not
@Semiclassical yay, got my grade bumped up
21:09
woo
@Semiclassical This should make you happy: if $V\in L^2_\text{loc}$ is positive, then $-\Delta +V$ has a nondegenerate strictly positive ground state.
@Semiclassical er, if $V\to \infty$ at infinity
kk
yeah, that makes sense
@Semiclassical If you change signs I think you see degeneracy in general.
@Semiclassical Reed and Simon are so wonderful because I can go to them for something completely unrelated to QM and come away with some QM magic
in this case, positivity conditions for semigroups and I learn about ground states
21:42
@0celo7 near the end of Gromov's paper
he has the following
"Since $\pi_1(SO(n\geq 3))=\Bbb Z_2$, there are just two orientable vector bundles of rank $n\geq 3$ over orientable surfaces."
I don't understand this statement. I know how to do this over $S^2$, using the clutching construction. But to reduce say a torus to contractible pieces I need 2 cuts, not just one.
@Danu Agreed, so you'd have to worry about the gluing conditions at the two cuts.
I don't know, there is probably some consistency condition then. @BalarkaSen would know.
@Danu I'm trying to think of how the bundle looks on the polygonal representation of the surface.
21:59
Trivial on the interior
you're just gluing along the 1-skeleton
@Danu Yeah it's trivial but it should be "pre-twisted" so that when you glue you don't have to do any more twisting
like if you cut a Mobius strip
It's not going to be so easy to visualize
Indeed.
It's an $n\ge 3$ thing.
even e.g. the non-trivial $S^2$-bundle over $S^2$ is already $\Bbb C\mathrm P^2\#\overline{\Bbb C\mathrm P^2}$
I once found a way to sorta visualize it but it didn't last long :P
lol yeah I was trying to imagine the clutching construction on $S^2$ as a warm-up and was reminded why I'm not an algebraic topologist
22:05
I have it written out
but even with the notes it's very hard I remember
I managed to derive some intuition from the real projective case, which is much easier to visualize
@Danu This seems like something that would be in Milnor-Stasheff but I haven't read it.
The kind of topology that all these 4-manifold guys are fucking good at
@0celo7 Don't think it's in there.
Unrelated but do you use HBO Go?
no
Why do you ask?
Also, does that even exist in EU?
@Danu I keep having this problem where it thinks I'm using it on multiple devices but I'm not
was wondering if there's a trick to resolve the issue
google is unhelpful
 
2 hours later…
23:51
@JohnRennie Are you around?
@BernardoMeurer If he were at this time that would be highly unusual :P
@ACuriousMind Yeah, I just always try anyway so when he wakes up he pings me back
@ACuriousMind Do you happen to be familiar with audio equipment?
@BernardoMeurer Would it not be more efficient if you just pinged him with whatever you actually want from him?
@BernardoMeurer Not at all, I'm afraid
@ACuriousMind No, I want to be wanted
dont we all
23:59
@ACuriousMind True that

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