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user218912
7:00 PM
is it $\frac{1}{2}(d-2)$
 
user218912
in mass units
 
user218912
where d is the dimension of the lagrangian density?
 
@Danu I think there's also a symplectic structure involved.
(I should mention that I don't know crap about Kahler manifolds)
 
user218912
hi @ACuriousMind I'm having an issue with dimensional analysis can you please help?
 
@BalarkaSen Correct.
 
user218912
7:10 PM
@ACuriousMind my prof didn't teach dimensional analysis in qft during the lectures but one of the problems requires it.
 
You're supposed to know that from high school.
Like completing the square.
 
user218912
I know high school dimensional analysis
 
user218912
but idk dimensional analysis in mass units
 
This is exactly the same.
 
user218912
$\hbar = c = 1$
 
user218912
7:11 PM
it's the same?
 
@IceLord Then go to regular units, convert to mass units at the end.
 
@IceLord I don't really know what there is to teach except "The units must match up", but what is your question?
 
I don't like to keep track of units.
It gets complicated often.
 
@BalarkaSen Suppose I have some group acting smoothly on a manifold
 
user218912
i'm learning this from a book right now and it says because the lagrangian is $\mathcal{L} = -\frac{1}{2} \partial^\mu \phi \partial_\mu \phi$ the units of $\phi$ are $\frac{1}{2}(d-2)$
 
7:13 PM
And I consider the subgroup that leaves a point fixed. Is this always a compact subgroup?
 
user218912
and $[\mathcal{L}] = d$
 
@IceLord "the units of $\phi$"? Are you talking about its mass dimension?
 
user218912
yes
 
user218912
sorry bad wording
 
@0celo7 Eh, under what topology of the group?
 
7:16 PM
@IceLord So? What's your problem?
 
user218912
@ACuriousMind how do you derive it?
 
user218912
I've never seen this before
 
@BalarkaSen Compact open. I should mention the group is a subgroup of the diffeomorphism group.
 
@IceLord Well, do you know why the Lagrangian has mass dimension $d$?
 
user218912
yes
 
7:17 PM
Hm. I am inclined to believe this is true, but I am not certain yet. Let me think for a bit.
 
user218912
because the action is dimensionless? @ACuriousMind
 
Okay, do you know what a derivative does to the mass dimension of a field?
 
user218912
nope
 
Well, think about it! The definition of the derivative contains all information you need for this.
 
user218912
the definition with the limit?
 
7:18 PM
@0celo7 So the subgroup of diffeomorphisms of $\Bbb R^n$ fixing the origin is compact in $\text{Diff}(\Bbb R^n)$?
 
Yes, the standard definition as a limit of a difference quotient.
 
user218912
okay. let me think.
 
user218912
alright so the derivative has dimensions of mass
 
I mean, that can't be right because take a translation of $\Bbb R^n$ translating the origin to $(0, 0, \cdots, \epsilon)$ say. You should be able to uniformly approximate that by diffeomorphisms fixing the origin (take diffeomorphisms which fix balls of smaller and smaller radius around the origin, but translates by $\epsilon$ outside a slightly bigger ball).
I am not yet convinced this is uniform though. Let's see.
 
@BalarkaSen Is the diffeomorphism group even a finite-dim Lie group?
 
7:23 PM
No, of course not.
 
the parent group is Lie
 
Well, you never said that.
 
@IceLord Yes, correct
 
My bad.
 
Now you should see how the $\frac{1}{2}(d-2)$ came about, and also that no further knowledge of "dimensional analysis" was needed.
 
7:26 PM
@BalarkaSen You're right lel
 
@Danu Ah, ok.
 
But it comes for free
 
Oops.
 
Because if you have the inner product and compatible almost copmlex structure
then $\omega=\langle I \cdot,\cdot\rangle$ is a 1,1 form which I think gives the symplectic form
Yeah, exactly
It comes for free so the book I have never mentions it
 
Arrrrrrgh, I finally figured out what the weird chirping noise is I've been hearing for the last few hours
 
7:27 PM
@ACuriousMind sooooo?
 
Damn smoke detector is running out of battery
And I have no clue how to make it shut up till I can get someone to replace the battery -.-
 
Get someone?
@ACuriousMind is there PhD level dimensional analysis?
 
@0celo7 Well, I neither have a replacement battery nor do I know what kind of battery I need nor could I get any today since it's Sunday
 
@ACuriousMind Hehehe, I had that happen
I put so much tape on it that I didn't hear the noise anymore :)
 
7:31 PM
@0celo7 Well, then, stabilizer of $p \in M$ under the action of $G$ is cut out of $G$ by the equation $gp = p$. So $G_p$ is preimage of $p$ by the map $G \to M$ given by $g \mapsto gp$. Preimage of compact set is compact.
 
user218912
@ACuriousMind when I solve for $[\phi]$ I get $-\frac{1}{2}$ ._.
 
@IceLord How did you solve for that?
 
@Danu I believe ya. Unfortunately I only pretend to know what a symplectic form is.
 
@DanielSank You... also have this experience?
 
@ACuriousMind Sunday? Aren't Germans all atheists now?
 
7:31 PM
@BalarkaSen The definition is easy
@0celo7 I wish they weren't so religious here
Religious holidays are the fucking worst
 
@0celo7 That doesn't mean shops would be open
 
NO FOOD :(
 
@BalarkaSen Preimage of compact set is compact?
Are group actions proper?
 
No
But usual ones are
 
Oops, $G$ ain't compact.
For noncompact Lie groups there should be counterexamples, then. Not that I can immediately come up with one.
 
7:33 PM
I'll have to read the original paper then.
 
user218912
@ACuriousMind I did something wrong but
 
user218912
can I show you my reasoning?
 
I don't know, can you? :P
 
user218912
I'm probably approaching this wrong and being excessively retarded so please don't laugh at me.
 
@0celo7 This time I fell in my own trap because subconsciously my manifolds are compact :P
If $G$ is compact however, then that's trivial, so... oh well.
 
user218912
7:36 PM
@ACuriousMind $[S] = 0$ so $[d^dx] = -d$ therefore $[\mathcal{L}] = d$ because $S = \int \mathcal{L}\, d^dx$
 
Yeah, I thought we had already established that
 
user218912
yes and from that
 
user218912
I did
 
user218912
$\mathcal{L} = -\frac{1}{2}\partial^\mu \phi \partial_\mu \phi$
 
user218912
so
 
user218912
7:38 PM
$d = -\frac{1}{2} \, 1 \, [\phi] \, 1 [\phi]$
 
user218912
is that wrong?
 
I do not understand what happened to your r.h.s.
 
user218912
I just replaced the terms by their dimension
 
Hi, everybody.
 
Uh
That's not how it works
 
user218912
7:39 PM
:o
 
user218912
okay so that's my issue
 
user218912
idk how it works
 
user218912
can you explain please? @ACuriousMind
 
@IceLord You're not retarded. However, it's pretty clear that more math experience would help you quite a lot. Isn't it frustrating how we have to learn math while learning physics?
 
user218912
@DanielSank yes I'm learning both at the same time.
 
7:40 PM
It seems so many people learn math "on the job" as they do physics.
 
@IceLord Well, "replacing the terms by their dimensions" is the correct idea. Unfortunately, you didn't replace $\partial_\mu \phi$ by its dimension.
 
One of the joys of learning math is that it's strictly speaking independent from any other branches of science. Although learning some physics isn't bad for getting intuition about things.
 
user218912
@ACuriousMind :o
 
user218912
what did i do then?
 
When you said that "the dimension of the derivative is 1", what I thought you meant (because that's the correct meaning) was "taking a derivative raises the dimension by one". So $[\partial_\mu\phi] = [\phi] + 1$.
 
user218912
7:42 PM
oooh
 
user218912
okay :P
 
user218912
so it works out then
 
user218912
I switched from exponents to regular numbers
 
@Danu Anything interesting?
 
user218912
that's why I messed up @ACuriousMind
 
7:45 PM
@IceLord I don't know what that means but I'm happy you've found your error
 
user218912
thanks
 
user218912
I know how mass dimension works now i think
 
@IceLord Have you noticed that ACM and I frequently can't tell what you're talking about because you're using words to try to describe equations?
Might want to reconsider that.
 
user218912
I'll work on it.
 
That's all a person can do :)
 
7:48 PM
@BalarkaSen I took a break---had dinner n stuff
 
@ACuriousMind download QFT into my head, please.
@Danu Whadya eat?
 
@DanielSank Alrighty, need to make room for it first, though
 
@DanielSank Basic stuff---pasta with oil & garlic
Some fresh tomatos (the small ones) on top
 
You don't need all those octopus facts, do you?
 
I'm experimenting with lemon stuff
Lemon peel and juice
 
7:48 PM
Don't find pasta interesting.
 
Me neither, typically
 
@ACuriousMind Sure do. I can delete real analysis though...
 
That's why I'm trying this lemon stuff.
 
Good idea.
 
@Danu Sounds good.
 
7:50 PM
@BalarkaSen I usually want to find my food "delicious" rather than "interesting" ;)
 
Putting a bunch of lemon peel in the water has surprisingly little effect
 
@ACuriousMind Can't imagine what I eat being not delicious but interesting.
 
Is there an easy way to drop images into chat?
 
@DanielSank Depends on what you mean by "easy". Clicking the "upload" button doesn't strike me as hard, though
 
@ACuriousMind smartass
Thanks.
Made that.
It's delicious.
1.5 kg chocolate. Twelve eggs.
 
user218912
7:53 PM
so that's the chocolate cake you kept talking about making?
 
Dear god.
 
user218912
how big is it?
 
@IceLord yes
@IceLord Two layers. Diameter is... I dunno... cake size.
 
@BalarkaSen Oh, I've had things I'd describe as "interesting" but certainly not "delicious".
 
Octopus legs?
 
7:55 PM
@ACuriousMind I gotchu: gfycat.com/GroundedGracefulGrouper
@BalarkaSen :(
 
@DanielSank lol
 
That's an... odd recipe.
@DanielSank Oh, forgot you were an octopus-fan. Sorry about that.
 
@BalarkaSen np
 
user218912
@ACuriousMind when I try to show my work I still mess up because idk what to do with the $-\frac{1}{2}$
 
user218912
how do I treat it?
 
8:00 PM
@ACuriousMind Nonsense
If you replace each term by the units, it must be consistent
 
19 mins ago, by ACuriousMind
@IceLord Well, "replacing the terms by their dimensions" is the correct idea. Unfortunately, you didn't replace $\partial_\mu \phi$ by its dimension.
Read the entire conversation before commenting :P
 
Hmm.
 
@ACuriousMind yes
Please.
 
@IceLord Well, is the dimension of $\frac{1}{2}\phi$ any different from that of $\phi$?
 
user218912
ah
 
user218912
8:03 PM
ok it's not so I remove the 1/2?
 
"remove"?
 
user218912
uhm
 
user218912
then what do I do?
 
user218912
it works if I just remove it
 
user218912
ignore it i mean
 
8:05 PM
I don't know what exactly you mean by "remove" or "ignore"
 
user218912
what is the correct way to say it?
 
Are you averse to just writing $[\frac{1}{2} X]=[X]$ instead of trying to find an awkward word for that step?
 
user218912
what I'm saying is that i'll just write
 
user218912
xD
 
user218912
@ACuriousMind alright then
 
user218912
8:06 PM
thanks
 
user218912
wow it says to find it using the equal time commutation relations
 
user218912
same deal though right? @ACuriousMind
 
what says to find what?
 
user218912
the question asks to find the dimensions of the canonical scalar field using the equal time commutation relations for it.
 
user218912
i'll try it out
 
user218912
8:10 PM
using dimensions
 
user218912
okay I have no idea how to do this
 
user218912
I'll do it later. time to work on analysis
 
user218912
@ACuriousMind is the schrodinger equation the most fundamental thing in QM?
 
user218912
or is $[x, p] = i\hbar$ more fundamental?
 
user218912
8:25 PM
where does $\hbar$ come from?
 
I don't know what "most fundamental" means.
 
@ACuriousMind I'd guess "what do we need for an axiomatic construction" or sth
 
Both of the things you mention are basically postulates
 
user218912
okay but why is there an $\hbar$
 
8:26 PM
@Danu lol, you were faster because my bookmarked link for that is deleted :D
 
user218912
@ACuriousMind ignore everything I said
 
user218912
back to the problem I'm working on, can you give me a small hint how to find the dimension of the scalar field using the ETCR for the fields?
 
user218912
because it's not obvious to me
 
@IceLord Uh, there's not really a reason for that.
@IceLord Find the dimension of the delta function first.
 
@ACuriousMind :D
 
user218912
8:28 PM
@ACuriousMind okay
 
user218912
@ACuriousMind thanks I think I know what to do now
 
@ACuriousMind This is so tricky ^^
 
@Danu It is? :O
 
@ACuriousMind It was for me, when I learned about it. Just "obviously dimensionless" is my kneejerk reaction.
 
@Danu Yeah, that's my "intuitive" reaction, too. Just goes to show one can't trust intuition :P
 
8:45 PM
If you think of $\delta$ as a very sharp rectangle, i.e. $\delta(x)=\frac{1}{2\epsilon}$ for $|x|<\epsilon$, it seems pretty intuitive :P
 
physics.stackexchange.com/questions/280948/… does this qualify as "weird personal theory" or not?
 
@Sanya Sigh...kpv's been at this for a while.
It's not really a personal theory though, it's just that they analyzed some data and believe that there are patterns in them. Too bad that they don't do any statistical analysis to back up the claim those patterns are in any way significant.
 
@ACuriousMind I mean, I've got nothing to say against the stuff he writes in his post here; basically "I want to have a detailed statistical analysis of Bell Inequality tests" - but if you look at the paper he linked - well, it's very badly presented and doesn't involve you to really go through it AND he actually makes some more dramatic claims in the paper
 
I know, I've looked at the paper before.
 
@ACuriousMind ah ok - well, I mean, in the first place, it would be very weird if no one had done decent statistical analysis in Bell tests anyway :|
 
8:58 PM
@Sanya Well, the question is - what kind of analysis would one run? If one doesn't go in with a particular idea of what pattern to find, what is one looking for?
 
@ACuriousMind tbh I've never gotten into statistics as deep as I should have, maybe because I in the end never did too much experimental stuff - but to me, the only obvious tests would be to test how likely it is that the data would have been produced even though our hypothesis is wrong and well ... other things not, I'd guess, I see your point
 
9:28 PM
@BalarkaSen How do you get to the point where you assume all manifolds are compact?
@ACuriousMind I have a really important question for you.
@ACuriousMind What does $L_X\nabla$ mean?
Seems like some physicist thing
 
@0celo7 Context! I have no idea what you're talking about
2
 
@ACuriousMind $L$ - Lie derivative, $\nabla$ - LC.
$X$ - smooth vf.
 
Then it's the operator that first takes the covariant and then Lie derivative, no?
 
No, because I have the claim: $L_X(\nabla)=0$ iff $X$ is Killing.
But it's certainly not true in general that $L_X(\nabla T)=0$ if $X$ is Killing.
 
@0celo7 Well, I can't magically divine what whatever you're reading is talking about, either
 
9:41 PM
If this were representation theory I bet you could!
Wtf $(L_X\nabla)_UV=(L_X\nabla)(U,V)$??
What does that even mean
$=L_X(\nabla_UV)-\nabla_{L_XU}V-\nabla_U(L_XV)$
have you seen such sorcery before @ACuriousMind
 
I don't think moderators should be allowed to delete/edit posts past the 2 min limit unless there's a rule violation.
 
@0celo7 I have seen \nabla used as the symbol for a connection :o
 
Why ":o"
I'm using it as a connection here.
 
but then you know what your symbols mean
 
9:47 PM
I'm not sure what $L_X(\nabla)$ means even if I know what all the symbols involved are.
I think ACM knows
I just have to extract it
 
what is wrong?
 
I have clearly stated I don't know. Why do you believe otherwise?
 
Oh I believe you.
Doesn't mean it's not in there somewhere.
You could have been walking past some geometers who talked about it.
@ACuriousMind Correct me if I'm wrong please, but $(Z,Y)\mapsto \nabla_ZY$ is not tensorial.
does that even make sense?
Yeah that's not a $(1,2)$ tensor.
So what is $L_X\nabla$ even?
$L_X$ is defined on tensors.
Ok, it's a formal product rule.
We take the object $\nabla_UV$, then differentiate it: $$L_X(\nabla_UV)=(L_X\nabla)(U,V)+\nabla_{L_XU}V+\nabla_UL_XV$$
then rearrange.
seems useless
 
10:06 PM
@0celo7 Not sure what you mean.
 
@ACuriousMind I'm sorry I gave you shit for not knowing why the isometry group is Lie. The proof is horrible :/
 
I suspected that :P
 
@ACuriousMind Petersen has a "full" proof if you do a 9 part functional analysis exercise first
 
@ACuriousMind How much time have you spent with the compact-open topology, Arzela-Ascoli, etc.?
 
10:10 PM
None with the compact-open topology, some with A-A
 
@ACuriousMind Do you know a bit of complex algebraic geometry?
Perhaps familiar with the "Kodaira dimension" of a connected complex manifold [see math chat if interested]?
 
@Danu Not really, and the only thing I know of the Kodaira dimension is its name
 
@ACuriousMind I'm not asking for much more :P
Just a little bit of motivation behind its definition
 
@ACuriousMind Did you prove A-A in your FA course?
 
@0celo7 yes
@Danu I mean, I literally only know its name. I don't know what its definition or its use is :D
 
10:17 PM
@ACuriousMind It's related to the algebraic dimension... Somethingsomething.
 
@ACuriousMind Ok, my analysis book proves it for functions on $\Bbb R$, then claims (I think) that the idea is the same for $\Bbb R^n$, or at least that the generalization is easy.
 
This is why complex varieties are better. Dimension is easy enough.
 
because when the author references it in his geometric analysis book he writes the pages of his analysis book where he proves it on $\Bbb R$
@ACuriousMind Can I see the proof you learned?
 
@BalarkaSen Dimension is no problem either way.
Algebraic dimension is something different
As is Kodaira dimension
The normal definition of dimension is not so bad (just take a regular point of your variety and look at the dimension of the manifold).
 
Sure.
 
10:20 PM
@0celo7 Here
 
Anyways, I've got a huge headache "rising"... So I guess I better go to bed.
Bye, guys.
 
@ACuriousMind wtf you did PDEs in that course?
Don't tell me you don't know anything about PDEs
 
The tangent space definition isn't really the right version of the defn anyway.
Transcendence degree of the field of rational (or as you would say, meromorphic) functions over it is.
 
@ACuriousMind What is $\mathscr L$?
 
Bye, @Danu.
I should head to bed too.
 
10:22 PM
Spitting bars, again!
 
@0celo7 continuous linear operators
 
Proof: Omitted?
You skipped the inverse function theorem?
 
That's standard.
 
@0celo7 Ain't nobody got time for that!
 
@BalarkaSen What's standard?
 
10:25 PM
Inverse function theorem.
 
So? Most things in math are "standard"
 
No.
 
@BalarkaSen So one shouldn't prove the transversality homotopy theorem in a diff top class because it's standard?
 
I didn't say that.
Just that people would probably do calculus before functional analysis.
 
Inverse function theorem is not...oh forget it.
@ACuriousMind Um, has anyone told you your Ys are backwards?
 
10:28 PM
@BalarkaSen This inverse function theorem is a variant for general Banach spaces. We didn't do that in my analysis class.
 
'Tis the exact same proof tho
 
@0celo7 Yes, multiple times :D
 
@BalarkaSen Do you actually remember the proof of it?
 
sure
 
Don't ever give that "bad memory" BS.
 
10:29 PM
All you need is a normed vector space where contraction mapping holds.
aka a complete normed space
aka Banach space
same proof.
@0celo7 I don't know if there's anything to memorize about it. It's a straightforward application of contraction mapping theorem.
 
Do you mean the Banach fixed point theorem?
 
Those are not distinct theorems.
 
I recall having to prove the implicit function theorem first, and that taking a couple pages.
 
I have never heard of proving implicit function theorem before inverse function theorem.
 
cf. Bredon.
 
10:34 PM
I'll look at it. Weird.
 
cf. Jost
 
For me it's always the implicit function theorem the proof idea of which I forget. One has to come up with an appropriate function to use inverse function theorem but that requires a few manipulations.
 
@BalarkaSen I remembered a geometry book you might be interested in
I heard about it from T. Tao
 
Hmm ok.
 
It's super short.
180 pages.
 
10:42 PM
Nice.
Pretty quick-and-dirty.
 
@BalarkaSen I'm going to the library to print something and get a book. I'll pick up this too and take a look.
 
alright. thanks.
I want to read something on differential forms where you actually do something nontrivial with them except introduce them as "fun, elementary, and beginning de Rham theory". Bott-Tu is too technical, I'd prefer something more geometric and non-homotopical.
Don't want to do algebraic topology with forms.
 
Bott & Tu is very technical
I will attack that book again next summer.
 
so, any ideas what to read?
 
@BalarkaSen Honestly...GR.
Diff forms are incredibly powerful in GR
 
10:47 PM
Eh. Maybe not now.
I'll ask Ted or Mike.
 
Kobayashi & Nomizu use forms a lot but they put B-T to shame in terms of technicality.
 
Ted's a fan of diff geom done with forms, so hopefully he'll tell something interesting. Mike was also saying a thing or two about sympletic and contact topology after smooth manifolds.
 
Has Ted recommended Chern's book?
 
I haven't talked to Ted about this, so no.
do you know anything about foliation geometry?
 
Just the basics, i.e. what's in Lee and other Lee.
 
10:51 PM
what does it do
oh nevermind found an MO post on that
 
You fill your manifold with a bunch of submanifolds.
 
yeah, just saying what I can do with it
 
Oh, you can prove the Frobenius theorem in PDE.
The main applications I know of are technical theorems for Lie groups.
I don't have much desire to learn about foliations for the sake of foliations.
 
I have heard it in the context of 3-manifold topology a lot.
something I want to learn someday
alright gotta sleep
 
11:35 PM
@BalarkaSen Candel and Conlon Vol 2 spends a lot of time on foliations of 3-manifolds.
 

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