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00:00 - 16:0016:00 - 00:00

00:00
However, also if this is a resonance and because resonances are B-W peaks, I don't see a reason why this process should continue far above the allowed energy, either.
So if I understand you correctly, I would share your scepticism about this being a lower bound for the process, and not the peak energy which the process happens around.
Maybe a true particle physicist like @dmckee could say something more definite, though
hmm
there's probably some discussion of this in the context of the GZK limit in the literature as well
00:20
*writes $\partial^\mu(\phi_1)\partial_\mu(-i\phi_2)+\partial^\mu i\phi_2\partial_\mu\phi_1$ *
what about it
preeeety sure this is zero 🤔
proof?
no :3
then it's false
false unless proved correct with a Bourbaki proof
00:24
don't worry I will find a way to avoid learning how to manipulate it with the partials again like I did the last 40 times
unless those are operator-valued, what is the issue?
@ACuriousMind This is a torus
the black curve is homotopic to the blue one, right?
@0ßelö7 dunno think it's just magic, unless I can just flip an up/down index anywhere anytime
@GPhys please state that carefully and I will agree/disagree
I think I agree but best be careful here
@0ßelö7 if I write say $g_{\mu\nu}$ and $g^{\mu\nu}$ twice, can the g float out of the partials? In this problem it's really eta though
eta is constant
00:32
since it's lorentz invariant, I guess so :P
but does it work with g?
@GPhys this has nothing to do with Lorentz invariance
@GPhys yes
@0ßelö7 what is lorentz invariance?
is that a rheorical question?
no I think you have some different definition than what I have in my notes somewhere (?)
the metric tensor is a list of numbers.
00:35
Lorentz invariant means it is invariant under Lorentz transformations
what on Earth could it mean beside that?
is eta not ?
that depends wholly on what you mean by "eta"
@0ßelö7 why can I write in the g_\mu\nu and the like here and move them out, but not everything else? What is the property?
maybe @Semiclassical can help, because I'm afraid i don't know what you're talking about
maybe if you write some equations
$\partial^\mu(\phi_1)\partial_\mu(-i\phi_2)+\partial^\mu i\phi_2\partial_\mu\phi_1$
00:40
I mean $a_\mu b^\mu=a^\mu b_\mu$
If you write down any instance of $g_{\mu\nu}$, is there any spatial or time dependence?
everyone knows that
what is the issue with $g$ there?
@0ßelö7 for a certain definition of 'everyone'
$\partial_\nu(g^{\mu\nu}\phi_1)\partial^\nu(-ig_{\mu\nu}\phi_2)+\partial^\mu i\phi_2\partial_\mu\phi_1$
$g^{\mu\nu}g_{\mu\nu}\partial_\nu(\phi_1)\partial^\nu(-i\phi_2)+\partial^\mu i\phi_2\partial_\mu\phi_1$
conservation of indices...
00:42
@Semiclassical if a 10 eV electron hits a 5eV barrier of width 100f, do you expect the transition probability to be 1 to within calculator erorr?
@0ßelö7 the operator $\partial$ doesn't care about the $g$, what is the property a tensor has to have to do this
3 mins ago, by 0ßelö7
I mean $a_\mu b^\mu=a^\mu b_\mu$
@0ßelö7 ugh, i'd have to think about that and I don't have the energy for that.
(I know it's not actually hard---just figure out the momentum and compute the tunneling action---but eh)
@Semiclassical I have the formulas, but I'm wondering if the guy wants me to show that it's not 1 at like the 10th decimal place or what
it's 0.99999999995
1-5E-11
00:46
works for me
I wonder what the precision on trig tables in the calculator is
well, you're going to plug uthe tunneling action into $e^{-\Gamma/\hbar}$ (or whatever it is)
or is g just the only thing I will ever write down that can do this?
@GPhys can you prove what I wrote or not?
00:48
if you write down any element of $g_{\mu\nu}$, what can it be?
ah, that thing
@0ßelö7 sure, the index switching with g works fine
it just seemed like it was exactly 1, had to trick the calculator into giving more decimals
What does $k_2a$ work out to in this case?
00:49
@GPhys so those derivatives are just vectors
the same identity applies
@Semiclassical wolframalpha.com/input/?i=(2*mass+of+electron%2Fhbar%5E2+*5eV)%5E(1%2‌​F2)*100+fermi
damn you link
ah, the joy of WA links being stoopid
a handy factoid for doing this by hand is that $\hbar c$=1240 nm-eV =1.24 fm-keV
...how does $c$ enter?
mass of an electron = 511 keV/c^2
ah, ok
I should check if I have that product right, mind
I know 1240 nm-eV is right
00:52
@0ßelö7 is there a tensor other than the metric that works to float outside the partial like that though?
but I'm juggling the powers of 10 in my head to get fm and keV
@GPhys I honestly don't know why you're fixated on the partial derivatives.
The metric is not being differentiated
@GPhys to be clear: Is the metric tensor here just the usual SR case?
@Semiclassical It doesn't matter!
There are no derivatives on any metric :/
I'm fixated because it was the only thing I was trying to ask about, I have known this thing is zero the entire time
00:55
...is it an issue that the thing is zero?
no, I genuinely just want to figure the conditions for the things that don't have derivatives, so I am free to rearrange them
@GPhys idk if I'm being dense but that sentence does not parse. Please write a specific equation and a specific question
@0ßelö7 oh derp
hc=1240 nm-eV
h or hbar?
$\hbar c$ = 197 nm-eV
01:00
@0ßelö7 I did earlier, but you responded with a different equation :3
@GPhys link?
I tend to remember the hc version for reasons I don't remember.
around 20:40 gave an example of a property g had that in general tensors do not have
@GPhys this?
and have been asking when a tensor has that property
01:01
Because I genuinely do not know what that is supposed to mean
I honestly can't tell if you're serious
What you're asking about seems to be this. Under what conditions does $\partial_\rho(g^{\mu \nu}A)=g^{\mu \nu}\partial_\rho(A)$ for a tensor $g$?
that's a bad question
the answer is "in coordinates when $g$ is constant in those coordinates"
which is why I was asking what his metric tensor was....
I guess in SR there's an implicit assumption that everything is happening in cartesian coordinates
because already in polar coordinates that isn't true
01:24
oh god do I have to vary phi and phi dagger independently
:o
have fun with that
::laughs at peasant physicist doing calculation::
::continues deriving inequalities::
@Semiclassical in other news, I found a formal statement for Lagrange multipliers for a variational problem on an infinite dimensional space
turns out everyone has been cheating, there's a PITA hypothesis
there's an issue with the constraint map being singular at the minimum point
@0ßelö7 a what
@GPhys pain in the ass hypothesis
you need to check that the derivative of the constraint map $E\to \Bbb R^k$ is surjective at the minimum point
that's usually a complete pain
...especially when the constraints are nonlinear integral operators
 
2 hours later…
03:46
So. Heat wave incoming in Australia. Is it possible to harvest its energy thus lowering its temperature?
@BalarkaSen I have a doozey for you
@BalarkaSen Do there exist complete $n$-manifolds $(M,g)$ with $\mathrm{sec}\ge 0$ such that the sum of Betti numbers is arbitrarily large?
What about CP^n?
Or are you fixing dimension
I mean $n$ fixed
03:49
Got it
cute question
@BalarkaSen if you come up with the right answer we will call you gromov
@Secret Antarctica is next door. Just put the cold end of your heat engine in Antarctica.
holy shit @JohnRennie is a genius
why can't we build a heat engine from the Sahara to Antarctica
0
Q: How to interpret 1 second equals to approximately 300,000km in general relativity?

user6760I am reading how massive object can cause other object to shrink in 4D (haven't touch the math yet), just want to know why time must becomes spatial dimension in order for relativity to work?

wot
So I am guessing large betti numbers somehow imply that the manifold can't admit nonnegative sectional curvature
That'd be pretty interesting though
I have no idea why something like that should hold
04:01
@BalarkaSen I have no idea how his proof works
Can you link me ze paper
He showed that for those hypotheses, $\sum b_i$ is bounded by $C(n)$ and also that the number of generators of $\pi_1(M)$ is bounded
Woah. (What's $C(n)$?)
a constant depending on n
04:02
@BalarkaSen looking
@BalarkaSen jstor.org/stable/2161381?seq=1#page_scan_tab_contents and references therein
Gromov's 1981 paper should reference a 1978 one with the fundamental group result
ok thanks
@BalarkaSen it would be interesting to see if anyone has calculated some of the $C(n)$s!
@BalarkaSen Mike might know about that. I don't know anyone that deep into Gromov-type geometry.
user308168
Why is there only one ad in the right sidebar of the main site?
04:13
I dunno, are you a narc?
what kind of question is that
@JohnRennie Who is this mystical Captain Beefheart
@BalarkaSen I have a topological doubt
cringe go ahead
ok I'm not that bad at topology
no need to cringe
just need to make sure before I tell a prof he's wrong
04:16
this is a torus. The blue and black curves are homotopic
@JohnRennie I don't but them for that purpose, but it is a big part of why apple can sell them so dearly.
@BalarkaSen I claim that there is no other curve in their homotopy class disjoint from both
user308168
I want to know whether there exists a limitation on the number of ads on the main site.
@BalarkaSen It's a long and psychosis ridden story involving Frank Zappa and some other very strange people.
04:16
They are generally well built and durable, but a comparably well build windows laptop is generally 20ish% less expensive.
I do think that Apple puts some thought into the engineering tradeoffs, but again, you can find windows laptops that exhibit very similar choices and they cost less.
@dmckee I think you're making a mistake by comparing OSX and Windows machines
@dmckee my (somewhat bitchy :-) comment applies to pretty much every consumer product. Cars for example. Humans are like that :-)
I buy them because (a) unix (b) on day one with (c) all the peripherals working.
@0ßelö7 That doesn't look true (by homotopy class you don't mean to fix endpoints, do you?).
Oh, I see, no, you should be correct.
yeah no one cares about endpoints
I want it to be disjoint anyway
04:20
If you project the cylinder as $S^1 \times I \to S^1$, the black curve maps to the full $S^1$ being the point
You constructed it that way
yeah and it intersects the middle line which you can't cross
so if you start on either side of the blue line you eventually run into the black one
Yeah, that works.
@BalarkaSen Now to put this in tikz...
help
@0ßelö7 Wait. What if you perturb the blue curve slightly to the left so that it becomes disjoint from the black curve?
What about it?
04:25
Ah, I keep forgetting it's a closed cylinder. You'd still need to make it disjoint from the original blue curve at the endpoints; that's impossibruh
ok ok ok you're good
I'm pretty happy with this
two profs said it shouldn't be possible
it makes the fluid mechanics homework 10x harder though :P
now it's a geometric measure theory problem
Good counterexample, proud of you for drawing that picture :P
I draw lots of pictures
@BalarkaSen I think this is also a good counterexample for the problem. What's a $\Sigma$ such that $\partial\Sigma$ is a union of those curves?
it really doesn't work because the black one is on both sides of the blue one
04:30
well they intersect each other
@BalarkaSen yeah? Never said the union has to be disjoint
Disjoint mod sets of measure zero or some shit
No I mean that implies there's no such $\Sigma$ right?
That's very not a surface; what is $\Sigma$?
a Lipschitz manifold
04:33
lol
alright then that should do the trick
@BalarkaSen But not in the case I drew because of the torus shenanigans
the curve wraps around and intersects on the wrong side!
Right, there's no way to consistently fill the regions bounded by the black curves.
that's actually a doubly wonderful counterexample then
can't apply Stokes theorem in any obvious way
I mean you can't apply Stokes on any surface that's sandwiched between the curves, but they are homotopic so there's a map $H : [0, 1]^2 \to S^1 \times I$ sending two sides of the squares to the curves you drew and pullback whatever form $\omega$ you have along $H$, then apply Stokes to $H^* \omega$ on $[0, 1]^2$.
but remember, $\omega$ is not closed
I have a vector field $u$ (velocity) such that $\nabla\times u$ (vorticity) is tangent to the surface
04:41
Frick ok yeah
@JohnRennie any bets on what a benchmark will show?
@0ßelö7 that you have too much free time?
@JohnRennie random speeds keep going down
@0ßelö7 meanwhile my neuron count keeps going down and my cholesterol level keeps going up. Shrug.
stop drinking so much then
04:54
If I stop drinking it won't mean I'll live longer, it will just feel that way
@JohnRennie you need brain cells to do math
@0ßelö7 now you know why all the great maths is done by people under the age of forty :-)
They either drink themselves to death or go insane?
Gnight
 
1 hour later…
vzn
vzn
06:12
get the led out was awesome, 3rd times a charm =D
That's pretty standard colloid science :-)
It's also the reason why ground liquifaction occurs in earthquakes
Although that's due to water fluidising the earth rather than air
Incidentally that technique is known as a fluidised bed
@JohnRennie is physics.SE down?
06:31
It's fine here ...
07:25
Hey hey
 
1 hour later…
Sid
Sid
08:33
@JohnRennie yeah, stop drinking and do yoga and stuff. You will be healthier
And try eating healthy stuff too..
08:54
user image
3
beautiful
40 keks to you
Hurray
So differential geometry question
If I have a (punctured) Clifford torus with coordinates $(x,y)$, is it a good idea to switch to polar coordinates
Depends on what you want to do
08:57
$r^2 = x^2 + y^2$ and such
Well I need to have a coordinate system centered around the puncture so I can send it off to infinity
But I'm not 100% sure that this coordinate system makes sense on a torus
It seems like this kind of thing is natural if you're describing your torus as a Riemann surface
so, a complex plane with two branch cuts
but I'm not sure how one does differential geometry this way
ah, I'm beginning to see it
a torus is just two copies of the Riemann sphere, glued together along the cuts
09:19
The issue is the range of those coordinates mostly I suppose
09:30
I guess I could just do one coordinate patch of this that's a disk
and then try to match them
@LeakyNun interesting. didn't know this
The first two comments were funny though :)
10:14
@Kaumudi.H: ping me when you're out of the exams
10:38
@0ßelö7 : Ceci est une pipe!
@Slereah Noooo!!!! I thought I'd finished with diff geom over a year ago, only to come here and find alas! It will always be there, ready to pounce when I least expect it
@Mithrandir24601 As long as this chat has ocelot at Slereah visiting it, you'll always ahve a chance to stumble over random geometry here ;P
@ACuriousMind maybe that'll sink in some day. Perhaps I'm just in denial?
10:59
@Mithrandir24601 Bad channel to come to if you don't like diff geo!
@ACuriousMind I have a problem
keeping track of my signs in my QFT homework 😩
@GPhys May Feynman have mercy on your soul. Signs are the worst.
@Mithrandir24601 Unlikely if you're in Bristol. More likely you're in de Avon.
why do you hate geometry
thats so rude of you
user228700
11:30
@JohnRennie Ping! :-)
Aha. Exams over! Have a look on Hangouts ...
user228700
Wokay.
12:15
@JohnRennie Well... I'm actually in Crete at the moment :) Aside from a couple of annoying things, I don't actually mind diff geometry - I was just being slightly dramatic :P
12:45
@BalarkaSen The class of R folds with $vol\ge v,$ $diam\le D$, and $sec\ge -k$ has finitely many homotopy types
13:09
@JohnRennie would be a pity if something sunk, lol
@0ßelö7 what is an R-fold
you mean complete riemannian manifolds?
Just Riemannian manifold
okizay
that's a pretty neat result
I'm not sure if one needs completeness
Needless to say the proof is impossible
is this also by the G-dawg?
13:16
Nope
Grove and Petersen
Who is
the G-dawg
It requires one to look at the "space" of all Riemannian manifolds with the Gromov-Hausdorff distance
@Slereah the baboon man
gromov
@0ßelö7 Ah yes that's a thing
The gyroscope continuously amaze me.
13:19
@BalarkaSen you basically "cover" this "space" with "balls" in which things are homotopy equivalent, and then use a "compactness" result
The actual proof doesn't look that bad.
@BalarkaSen Gromov's theorem requires two-index exact sequences and filtrations, which give me Bott and Tu PTSD flashbacks
uh oh lol
Actually the fundamental group bound looks elementary
Anyway I think you should compute the gromov constants for your PhD @BalarkaSen
I imagine that's a seriously difficult task
0
Q: Why was I blocked from asking a question despite recently having only positive answer and question reactions?

Aditya RadhakrishnanIn my early days of using Physics Stack Exchange, I had no idea how the website worked and admittedly didn't do my research. And I'm talking about one question. I've asked only 6 questions - two with a total of 3 downvotes asked a while ago, one without any positive or negative votes, and three ...

 
1 hour later…
14:59
@EmilioPisanty TeXGod, I need to use a .cls file and tex.stackexchange.com/questions/1137/… is very inconsistent with how that's actually supposed to work
@EmilioPisanty I can't find this /texmf file
there's a hidden file /texmf-var
15:15
@0ßelö7 what sacrifice did you use?
anything less than a lamb and two chickens is unlikely to work with that one
@EmilioPisanty I have two young nephews
@0ßelö7 about one and a half, then
seriously, though, how desperately do you need this to be installed centrally?
@EmilioPisanty I want to turn my notes into something a little more organized and want to use the springer monograph template
including the usual Springer math fonts, etc. which I really like
that wasn't the question ;-)
I don't know the answer to your question
I am telling you what I want to do
15:19
you know you can just put the .cls file on the same folder as your .tex, right?
maybe you can figure out what my answer should be then
@EmilioPisanty and it will run?
the question you linked is for when you want to avoid doing that
@0ßelö7 yes
@EmilioPisanty why would one want to avoid that?
this is me doing just that right this minute
@0ßelö7 'cause you use the same cls file over and over and you don't want the hassle
or similar situations
I have over 100 tex in the same folder
so if I just keep doing that and put the .cls in there I'm good?
15:25
@0ßelö7 sure
whatever compiles that you're happy with
I'm not one to criticize others for their coding practices
I'll criticize others' coding practices every day.
@EmilioPisanty I've tried to clean it up but it's too much of a hassle
Woo hoo
the week end
Anonymous
15:41
@LeakyNun You might be interested in this, this and this.
thanks lol
@Slereah still got an exam
what are you examining
Anonymous
@LeakyNun The papers are good though. The tension explanation we used yesterday was hand-wavy. Also, I tried out the experiment today (mentioned it in my question). BTW, I see nothing to be lol-ing about.
00:00 - 16:0016:00 - 00:00

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