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01:48
Slearah: I don't have Steenrod in front of me so can't tell if he's using some offbeat definition (maybe offbeat today but not in his day?) but by the usual definitions, every tensor bundle is a vector bundle, for sure.
 
3 hours later…
04:29
Lol
Last one for acm
04:52
lack of research @YuvrajSingh... Pal
Boomerang @skullpatrol
05:47
Hi. Can anyone tell what is wrong with the following method of computing the effective capacitance between two points (marked with red circles)? :
I got the effective capacitance as 2C when I considered the system to be a combination of balanced Wheatstone network and a capacitor connected in parallel with the terminals. And it's the correct answer as per the book.
06:40
I recall I turned the lightbulb joke into an actual conspiracy theory
that the mere act of joking about screwing a lightbulb will eventually caused it to screw itself in, regardless of what the lightbulb is
It's a conspiracy theory because say you identify lightbulb with the US government
@Secret joke is quite old isn't it?
yup
Do you have some more?
nope I am not good at jokes
Np, do you mind I am talking to you for some time? I haven't talk much with you since I joined this room!
Are you a theoretical physicist?
@Secret
06:47
nah I am a computational chemist
currently doing a PhD
I do have a very strong interest on theoretical physics
but I quite suck at it
Yes as I can see you on mse
However, I think more like an artist and philosopher, and get sentimental
A strong mathematics students would definitely be good in theoretical physics!
I believe *
not necessary, theoretical physics involves some intuitions as well to use the correct assumptions
Also they have their nonrigorous language that is math like but mathematicians have only starting to understood it
Physics is based on how well you can imagine nature working
And you should have mathematics to write that
06:51
Don't need English?
@Secret as a student what you feel can be best difference between mathematical physics and it's reverse physics mathematics, since both have included mathematics and physics?
07:13
mathematical physics is more rigorous, physical mathematics requires a bit of intuition
@Slereah I'm not quite sure what counts as a "tensor bundle" here, but there are algebro-geometric analogues of the (co)tangent bundle in form of the (co)tangent sheafs (see e.g. en.wikipedia.org/wiki/K%C3%A4hler_differential), but these sheafs do not necessarily represent a vector bundle - only when they are locally free
@dumbasarock Please don't post links to your questions here directly after you've posted them; if everyone did that the chat would consist of little else.
okay sir I won't do that again.
You told me you wouldn't call me 'sir' :P
old habit
but can you take a look at that question I just need to know that if I am thinking in the right way ?
although I highly doubt it.
it's like there is a gap fit whatever fits(looks like) in
07:43
@ACuriousMind steenrod uses tensor bundle to mean fiber bundles that have a rep of GL acting on the fiber
@Slereah Then every GL-principal bundle is an example of a non-vector bundle with such an action, right?
@ACuriousMind gonna need to check the definition to see if that fits
@ACuriousMind Are magnetic monopoles instantons, or something similar?
From what I can see they don't seem to be, but they're usually grouped in in the same bag
They're not instantons, but they are non-trivial bundles
07:58
I'm not 100% sure what instantons are since I'm not sure the definition is standard, but it seems to be related to the third homotopy group of the bundle
And that is trivial for $U(1)$
@ACuriousMind Is there a name for the thing that covers all of them?
outside of "non-trivial principal bundle"
I tried looking it up on ncatlab but they started using the word "gerbes" and then I just woke up covered in blood
not sure
but btw I think I figured out/remembered why in classical physics you can't "switch the bundle" - there is no smooth way of doing so, so the equations of motion won't ever evolve an $F$ that comes from one bundle to an $F$ that belongs to another
Speaking of that
But in QM, we just enumerate all the states and do the path integral, there isn't such a "smooth geometry transition" requirement there
One of the standard example for instantons is apparently the $\mathbb{Z}_2$ $\phi^4$ theory, of domain wall fames
Is that a bundle theory?
@ACuriousMind Yes I suspected why that was the reason why it was more important in QM
@Slereah that's because people change all the time whether some things should be called "solitons", "instantons", etc...
08:09
Yeah they do seem to be playing a bit loose with the term
Are all (non-trivial) instantons also solitons?
They do seem similar since they have topological charges
Since I've never seen a good definition of a soliton that didn't involve a good measure of "I know it when I see it" I can't answer that :P
Some people use the interchangably
@ACuriousMind Well I can think of one, but I'm not sure it's at the same level of rigor as instantons being the third Chern class of a principal bundle
Some people say "soliton" for spatial configurations and "instantons" for temporal configurations with similar topological characteristics
Something about $$\lim_{t\to\infty} \phi \neq 0$$
@Slereah The rigorous definition for "instantons" I'd use is just "anti-self-dual field strength configuration in a Yang-Mills theory"
@Slereah It's not the "third Chern class". It's that bundles on $S^4$ are classified by homotopy classes of maps $S^3\to G$ (see physics.stackexchange.com/a/127880/50583), and that is the third homotopy group of $G$.
The third chern class would be something like $\int F\wedge F \wedge F$, which doesn't even exist in less than 6 dimensions
08:14
By the way, I get that being anti-self-dual can help cast the action in the proper form to show the chern class, but can the field be not (anti-)self-dual?
and if it can, to what instanton sector does it belong to?
@ACuriousMind Isn't that almost the form of the action though?
@Slereah The field can, but the classical extremum of the action (="vacuum", in the loose parlance of QFT people) is always anti-self-dual
Up to a surface term
@ACuriousMind Ah yes, so it's only the ground state
@Slereah Note the three $F$s. The action only has two
Ah yes, after checking, the instantion action is three $A$'s
not $F$'s
I don't know what the "instanton action" is. Do you mean the Chern-Simons action?
Ah, yes, that term being differentiated there is the "Chern Simons current"
Also apparently nlab says you don't need singularities to pretend to have magnetic monopoles, but then they started talking about gerbes again so I died
@Slereah What I said above is for the Dirac monopole. There are 't Hooft-Polyakov monopoles that don't have singularities, but involve a larger (broken) symmetry group the EM U(1) embeds in
I tried reading up on gerbes but then they started talking about stacks, and the stacks said they were 2-sheafs
And as I'm not quite comfortable with sheafs yet I had to go to bed
It would be nice if there was a bundle simpler than $U(1)$ :p
The $\mathbb{Z}_2$ bundle
But I guess that one has no connection
@Slereah what about 12.7 of Streater's book, does that seem to say the nlab pre-quantization stuff is a bunch of nonsense?
08:29
I mean it's category theory, so of course it is
Also I think Streater was against the usual idea of deformation quantization because it's not an isomorphism
nlab's stuff is geometric quantization, which is I think?
Groenewold and Hove say that we can never have a quantization map with all desired properties, so Streater is out of luck :P
Well no, because Streater argued for that exactly!
@Slereah An isomorphism between what and in what category? :P
It seems like XVI here is roughly that section of the book
and he mentions Groenewold!
Also streater's book isn't saying exactly that those ideas are VERBOTTEN, just that they are well-trodden ground and probably not worth investigating, especially by students
@ACuriousMind The category of prequantum field theories and quantum field theories???
08:32
Ah, sure. I'd agree that the vast majority of physicists can live with the ad-hoc inconsistencies of canonical quantization just fine
Also really it's not like the "real" quantum theory is usually that weird
If you have a classical $xp$ term, I don't think the quantum theory can be $\pi \hat{x} \hat{p} + e \hat{p} \hat{x}$
(Funnily enough the end of this mentions the 'oscillator group' which came up in that verbotten question that was asked the other day about when to use oscillators)
You can probably just try brute force to check all the reasonable theories :p
@Slereah have you read S. Coleman, ”Uses of Instantons” in Aspects of Symmetry, Cambridge University Press (1985)?
Are there any case where the quantum theory isn't $xp$, $px$, $(xp + px) / 2$ or $((xp))$?
@skullpatrol I have not
Although right now I'm reading about classical instantons
It's hard enough as it is without involving QFT :p
08:36
hmm
\o @FakeMod
08:57
XXIII. First causes in physics

There aren't any. But what about final causes? I hear you cry. None: these are the same as first causes.
I can't guarantee that all of Streater's point are 100% valid, but on the other hand it is a very fun book
The angriest physics book
You can tell Streater had too many conversations with @vzn or the appropriate equivalent
@ACuriousMind If we can observe "gauge-dependent" things, then whatever that "gauge" transformation is, it's not a gauge transformation because those leave all observables invariant!
@YuvrajSingh... I have no idea what you're talking about or what I have to do with it
@YuvrajSingh... by definition we cannot observe "gauge-dependent" things because the choice of gauge is just a mathematical trick and cannot affect the real world.
09:21
"I think that the problem is much simpler: cosmologists have failed to note the distinction between a gauge group and a mere symmetry group"
That's because "gauge group" rarely has a stabdard definition
Although I guess he means bundle automorphisms leaving the action invariant v. the principal bundle group
I think it's safe to say that gravity gauge business is hard
I'm still not 100% sure of the link between diffeomorphisms and the Poincaré gauge :p
I have a smattering of theorems about it, but it's hard to get a clear picture
09:39
"Reference Book: Gauge Theories of Gravitation: A Reader with Commentaries, M. Blagojević and F. W. Hehl, editors. Foreword by: T. W. B. Kibble, FRS (Imperial College Press, London 2013)
Lecture 1 & 2: Chapter 1 - From Special to General Relativity Theory
Lecture 3 & 4: Chapter 2 - Analyzing General Relativity Theory
Lecture 5 & 6: Chapter 3 - A Fresh Start by Yang-Mills and Utiyama
Lecture 7 & 8: Chapter 4 - Einstein-Cartan(-Sciama-Kibble) Theory as Viable Gravitational Theory
Lecture 9 & 10: Chapter 5 - General Structure of Poincaré Gauge Theory (Including Quadratic Lagrangians)
Going to have to go through this stuff I guess
10:03
Hey it's Hehl
Is he the Hehl-Datta guy
How come the image is so crisp but the sound is so bad
10:19
It's clearer with headphones
This one is super useful already
Pointing out the issues in Utiyama's approach
10:34
Anatoly Alekseyevich Logunov (Russian: Анатолий Алексеевич Логунов, December 30, 1926 – March 1, 2015) was a Soviet and Russian theoretical physicist, academician of the USSR Academy of Sciences and Russian Academy of Sciences. He was awarded the Bogolyubov Prize in 1996. == Biography == Anatoly Logunov was born in Obsharovka village, now in Privolzhsky District, Samara Oblast, Russia. In 1951 he graduated from Moscow University where he studied theoretical physics. From 1954 to 1956 he worked in Moscow University, later worked at Joint Institute for Nuclear Research (Dubna). He became doktor nauk...
What about this approach to GR
"This approach permits constructing, in a unique and unambiguous manner, the theory of gravitational field as a gauge theory"
11:14
let's see how the n cat defines solitons
aw, they don't have a fancy definition
11:29
I'm a bit disappointed that ncatlab doesn't have a mascot called the N cat
12:15
I wonder if the easiest way to show that the circle and square are homeomorphic is to switch from the $\ell_2$ norm to the $\ell_1$ norm
Some homotopy of $\ell_{1 + \lambda}$
hi
Can I request someone to answer my question here? It' pretty simple but isn't catching enough attention.
12:52
@Tachyon209 just post the question interested people will look upon it!
13:10
Thanks.
6 hours ago, by ACuriousMind
@dumbasarock Please don't post links to your questions here directly after you've posted them; if everyone did that the chat would consist of little else.
Your question is an hour old, just have a little patience - many questions aren't answered after that little time.
You know I wish people reprinted old books once in a while
With modern notation
Steenrod's not bad, but the notation is a bit old timey, and the pagesetting is bad
that would be nice
it could use some room to breathe
Unfortunately any book old enough to be out of copyright is probably not interesting enough to warrant such a project
Although I guess I could do it for that proof of the Matthieu equation from the 19th centuyr
13:32
Aah. Sorry @ACuriousMind. I'll keep that in mind. It's just that I was not getting any responses on any of my questions recently. So, was just a little skeptical.
14:30
@ZeroTheHero good evening can you take a look at a question I asked 7 hours ago but I haven't got any response on it yet. It acted like a speed breaker to my study. I could've posted link to it here but pasting question links aren't allowed.
@Slereah I once attended (many years ago) a cosmology seminar on inflation and negative pressures at the start of the inflationary period. Present (but not speaking) was an astronomer to the Vatican Observatory. At the end of the talk this person commented something like: “ Negative pressures, curled up dimensions... really? I think my explanation is simpler.”
I'm not sure Genesis explains the modes of the CMB
@dumbasarock Look, the idea is not to annoy people here with requests to look at a recent questions they already would have seen if they were interested in answering questions and looking at the main site. Whether you post the link or not isn't really the point.
Also, please don't ping specific people unless you have reason to believe your question is of particular interest to them.
This site is good, real good!. There are gems of questions and equally fantastic answers at all levels. I hope the good stuff doesn’t get diluted by the banal homework-style question.
14:43
I am sorry that I ping you and asked a stupid question.
@ACuriousMind If there's a non-trivial principal bundle, does the field have a zero section?
On one hand, there's instantons all over the damn place, on the other hand, every vector bundle has a zero section
Although I guess the zero section of $TP$ may not be the same as the zero section of $TM$
@Slereah What field?
It's bundles that have zero sections, not fields
And the principal bundle doesn't have a zero section because it has no notion of "zero" :P
The corresponding field of the connection :p
I guess in $HP$
what is true is that no non-trivial principal bundle admits a global section.
@dumbasarock Your question is not stupid but it’s not clear and I don’t have time to deal with this right now.
14:57
The connection form is a $\mathfrak{g}$-valued one-form on $P$, of course it can be identically zero.
the trick for a non-trivial bundle is that the connection form only descends to a connection form on the base spacetime in a trivialization, so you don't get a global connection form on spacetime for non-trivial bundles
This is because the non-trivial principal bundle does not admit a global section by which you could pull back the connection on $P$ to get one on $M$
ah, I guess the instanton business happens on the overlap maps?
if you try to have a zero section
Yes, the transition functions determine the (non-)triviality of the bundle and hence the instanton number
I think Naber talks about that
I need to get back in that
This is how you get things like $\pi_3(G)$ classifying bundles over $S^4$, because on an $S^4$ the overlap of two trivializations is homotopic to $S^3$, so choosing a transition function is the same as picking an element $\pi_3(G)$.
Do spin-2 particles collectively have a name like fermions, scalar/vector bosons etc.?
15:08
They are called tensor fields, usually
Due to reasons, there are typically no tensor fields of rank higher than 2
The name is "graviton", theories with spin-2 bosons that are not gravitational are usually inconsistent
Is that in the context of qft? So is it excluding say the riemann curvature tensor field
I don't know any qft so this is a super soft question I just wondered if they had a fancy name
I mean having a spin-2 particle is usually a QFT idea in general
@Charlie $(1,1)$ irreps of the Lorentz group?
@Charlie What except QFT would be used to talk about "spin x bosons" anyway?
I only mentioned the curvature tensor because you mentioned rank 2 tensors
15:11
Well as mentionned, typically only gravitons are spin 2
So the tensor fields are usually $\approx$ the metric tensor
I'm already out of my depth, thank you though
:)
Spin business is usually nasty
user434058
@ZeroTheHero Hi! I am only acquainted with electric and magnetic flux and that's the reason why I have only used them in my tag wiki edit. Please do edit the tag wiki to make the tag more general. Thank you! :)
Tag Wikis are only really useful if they contain information not obvious from the tag name itself.
"Use for questions about flux" is not very useful
15:21
You never know
Maybe a caveman might get some use out of it
@Slereah A caveman that can read English? :P
@YuvrajSingh... What?
Tried to change the topic , please continue
How is "stop" followed by three asterisks supposed to change the topic? If you offered an alternative topic in a comprehensible manner - or gave reasons to stop discussing the current one - you might be more successful.
15:38
CuriousMind you probably have been asked this a million times but who's in your profile picture?
@Charlie he had replied it several times:-)
Jan 18 at 19:14, by ACuriousMind
3 hours ago, by ACuriousMind
22 hours ago, by ACuriousMind
@Knight It's the protagonist of Disco Elysium
@ACuriousMind there you go I have one question!
how the field theory corresponds to black holes in the gravity dual?
I see haha
His name is hobocop
15:42
@Charlie haha?
I consider string theory as stupid theory with no predictions, and no one can test it's existence and we study it with all the rigorous mathematics!
@Slereah Only if you choose so!
There is no freedom of choice
All is determined
16:08
$$ \array{ && \longleftarrow \\ & \swarrow && \nwarrow \\ V && && V^\ast \\ {}^{{\exp(\tfrac{i}{\hbar} H t)}}\downarrow && && \uparrow^{{id}} \\ V && && V^\ast \\ & \searrow && \nearrow \\ && \longrightarrow } $$
@ACuriousMind Please explain
It would appear you've botched some MathJax :P
Category theory is hard in mathjax
ncat has some weird definition in their mathjax
It's probably better if you just link to the page you're wondering about
I'm afraid I was somehow jesting
I don't expect you to explain all the FQFT article
I'm afraid category theory parody may be even harder to understand than category theory ;)
16:11
Oh that is 100% a real diagram
Despite being a loopdeeloop
it is here, if you are curious
16:42
That's supposed to be Penrose notation for the partition function...
 
1 hour later…
18:04
Spellcheck has been great, but whoever figures out how to get grammar check to work is guaranteed a Nobel.
2
18:45
I have been doing some sums on this kind of problems
But really cant figure this out
18:59
Use the Poisson equation
Yeah but stuck at the laplacian part
What has you down
 
2 hours later…
21:00
0
Q: Where does scoring from question and answers come?

AlfonsoI see that some of my questions and answers have positive and negative integer score. Where does it come this score? I am new in the forum.

 
1 hour later…
vzn
vzn
22:25
@Slereah lol asking for trouble, as usual? and ryan is long nowhere to be found? if you like science comics why dont you try sidney harris, he understands kuhnian paradigm shifts (unlike many "scientists") :P sciencecartoonsplus.com/pages/gallery.php sciencecartoonsplus.com/gallery/physics/index.php

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