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17:00
@0ßelö7 don't you like horror games
what does one do to get both diagonal
He's probably trying to simultaneously diagonalize A and B
what does one do to get one diagonal
@BalarkaSen I played Metro 2033 and it's absolutely horrifying. I really can't into the horror genre as a whole.
I'm so terrified of jump scares
how do you feel about cabin in the woods
best horror movie
17:01
never heard of it
I actively avoid that stuff
@ACuriousMind @dmckee @DavidZ @Qmechanic, maybe get the ball rolling asking the mods at CS and TCS whether this one is migratable to their sites?
0
Q: Solve Travelling salesman problem with light machine

Ilya_GazmanI got a crazy idea how to solve the famous Travelling salesman problem using light machine, and I want your input if such machine can be constructed. It starts by shooting a white(full spectrum) light. Each node(city) will be a device that will absorb part of the light and redirect it to all the...

bleh I wouldn't call Cabin the best horror movie
@0ßelö7 play one without jumpy scaries then
@BalarkaSen Such as?
surival horror like Last of Us
v good game
hows 1408? as an actual scary (horror) movie its my favorite
17:05
Oh I have heard of that one
Never seen it though
I might try it
I'm never gonna get an answer :c
@BalarkaSen isn't that PS4 game?
I asked on the Linear Algebra room 12 hours ago and it's still barren
@Phase I have no idea what the doubt is
what do you mean
17:06
@0ßelö7 oyeahprobably
I'm asking for what the formal method of doing it is
@Phase what's the question?
Diagonalising two hermitians A and B that commute, where one [or both] are degenerate
what about it?
is this not in Shankar
17:07
I'm asking what the formal method of doing it is
diagonalize A, then look at the action of B on each of the eigenspaces of A (which is closed because [A,B]=0) and diagonalize B on each individual eigenspace of A, and you're done
cant you just define C=AB=BA then diagonalize C using normal methods
@shaihorowitz that's a terrible method
im just gonna go with your right, do your method
How much freedom is there to choose the degenerate parts of the eigenbasis?
if both are degenerate
17:09
@Phase in the initial part (diagonalize A) you can choose any eigenbasis you want
after that, when you're diagonalizing B, it is crucial that you don't try to diagonalize B directly, but only its action on the A eigenspaces
at which stage you can choose any eigenbasis you want (within the preexisting A eigenspace)
So
If im not mistaken
which i probably am
If both are finite, like say 2x2 or 3x3
@EmilioPisanty Can do. Do you have a reason to believe it's not on-topic at CS though? (We're not really supposed to bother mods unless whether or not the question is in-scope is unclear. If we possibly wouldn't migrate it for quality reasons, just don't migrate)
@Phase that's too small to be useful
You could take the eigenvectors in the basis that A is diagonal in, and assemble them into the identity matrix and use B?
Oh
Well I just mean finite matrices
yeah, but 2x2 won't fit interestingly different degenerate eigenspaces
17:11
because I'm not sure how decomposition works in infinite dimensional matrices
yeah good point
wait im a bit confused still
Say, take $A=\begin{pmatrix}0&1&0&0\\ 1& 0&0&0 \\0&0&0&1 \\ 0&0&1&0\end{pmatrix}$
What do you mean by look at its action, could you just write down a general form for that?
Oh thanks
and, say
wait
$B=\begin{pmatrix}0&0&1&0\\ 0& 0&0&1 \\1&0&0&0 \\ 0&1&0&0\end{pmatrix}$
god, I hope those commute
^ physics in a nutshell?
excellent, they commute
so
first you diagonalize A
and you find two eigenspaces, one spanned by $e_1=(1,1,0,0)$ and $e_2=(0,0,1,1)$ with eigenvalue $+1$, and one spanned by $e_3=(1,-1,0,0)$ and $e_4=(0,0,1,-1)$ with eigenvalue $-1$.
Then you find the action of $B$ on those eigenspaces
so $Be_1=e_2$ and $Be_2=e_1$, and ditto with $Be_3=e_4$ and $Be_4=e_3$,
17:18
so
note that $Be_1$ does not involve either $e_3$ or $e_4$, which is crucial
A's trace would be 1, 1, -1, -1 and so would B's, because it's just switching 1 and 1
and switching -1 and -1
in their diagonalised form i mean
@Phase that's true but not specifically useful here
o ok
So, in the A eigenbasis we just found, the matrix representation of B is
17:20
if $Be_n = e_m$, does that mean that it's nth eigenvalue is the value of A's mth?
@Phase no
that's not an eigenvalue relation because $n\neq m$
$[B]_{A\text{ eigenbasis}}=\begin{pmatrix}0&1&0&0\\ 1& 0&0&0 \\0&0&0&1 \\ 0&0&1&0\end{pmatrix}$
hmmm, wait
if only one is degenerate
:40354732 That message was causing strange layout artifacts on my machine, so I have deleted it for the nonce. If this was unique to me I can restore it, but it seemed to be a problem.
17:22
Why couldn't you just use the matrix of eigenvectors of A, sandwiched with B in the middle
and then choose the eigenbasis for the degenerate part
^given A is non-degen, and B is degen
@dmckee can you reply to the message just below? what message was this?
Hi people
@Phase the non-degenerate case is a strict special case of the degenerate case and it does not require additional attention once you're doing the general situation
@Secret Reply to the post below the one I killed. as requested by @EmilioPisanty.
I have a question
17:24
The artifact was a huge vertical blank space that didn't allow any further posts to be displayed.
more specifically, if a given eigenvalue of A is nondegenerate then you'll get a 1x1 block in the B matrix over that eigenbasis, which you then proceed to diagonalize (by doing nothing)
@dmckee ¯\ _(ツ)_/¯ no idea
@Student404Mus don't ask about asking, just ask
(we should choose that as the h bar motto)
4
Hhhhhhm... What are the 1 St concepts I should learn in QFT
@Student404Mus What is "1 St" in that comment?
First
@Student404Mus QFT is a lie.
17:26
@Slereah can confirm
@ACuriousMind might argue but will eventually agree
@dmckee I think it's supposed to mean "first"?
@dmckee O yes, that message of Slereah's somehow infinitely stretch the screen when the latex is rendered, but it display correctly on the main
I mean fist
First
17:28
@Phase that's incomprehensible to me
So like
take the matrix of eigenvectors of A, like you do when you just diagonalise A
and call it V
I never toke any knowledge In relativistic QM
You need to know (0a) enough classical mechanics to know what a Lagrangian is and how to use it; (0b) enough electricity and magnetism to be able to write the energy in an electromagnetic wave; (1) some quantum mechanics; (2) the ladder-operator solution to the harmonic oscillator in quantum mechanics; (3) probably a few other things, but you can pick them up as you need them.
why cant you use $V^{-1}BV$, being aware that it's degenerate with some values and choosing those afterwardS?
@Phase you can
but
it will have a block structure
17:30
@dmckee Lie theory,
wait
like my last matrix above
which is exactly that
I just went back and looked at your B in A eigenbasis again
@0ßelö7 Oohhh, yes. That would be good.
17:30
You need to know that beforehand because no physicist is able to explain it.
And no mathematician cares about the Lorentz group
So it's quite the conundrum
if you neglect that block structure
then you'll be left with an eigenbasis of B that's not an eigenbasis of A
Why isn't B diagonal in it's eigenbasis if it shares eigenvectors with A?
so, for instance
@Phase [A,B]=0 guarantees that they share an eigenbasis, not that they share every eigenbasis
so, say, take $\tilde B =[B]_{A\text{ eigenbasis}}=V^{-1}BV=\begin{pmatrix}0&1&0&0\\ 1& 0&0&0 \\0&0&0&1 \\ 0&0&1&0\end{pmatrix}$
But how come B doesn't even have a single element in it's diagonal? Is that just because every eigenvalue is at least twofold degenerate?
@Phase because you haven't diagonalized it yet
"have elements in its diagonal" is a meaningless criterion
17:32
._. I'm not cut out for this
it's either diagonal (or block diagonal) or not
Here's the thing
there is at least one fact you can infer from the diagonal elements being zero: the trace of the matrix is zero, so the sum of the eigenvalues is zero.
take $\tilde B =[B]_{A\text{ eigenbasis}}=V^{-1}BV=\begin{pmatrix}0&1&0&0\\ 1& 0&0&0 \\0&0&0&1 \\ 0&0&1&0\end{pmatrix}$ as above and say that you want to diagonalize it. You might say "hey, $(1,1,0,0)$ looks like a handy eigenvector. Or you might say "hey $(1,1,1,1)$ looks like a handy eigenvector".
do you see the difference between the two?
and similarly the determinant is 1, so the product of the eigenvalues is 1. that sets some pretty strong constraints on it. that'd allow eigenvalues like 1,1,-1,-1; but, it'd also allow 2,-2, 1/2, -1/2. (that doesn't happen here, but the facts i've quoted aren't enough to prevent that)
keeping in mind that in that basis $\tilde A =[A]_{A\text{ eigenbasis}}=V^{-1}AV=\begin{pmatrix}1&0&0&0\\ 0& 1&0&0 \\0&0&-1&0 \\ 0&0&0&-1\end{pmatrix}$
$(1,1,0,0)$ stays inside the upper 2x2 block and it is therefore guaranteed to be an eigenvector of $A$. $(1,1,1,1)$ breaks out of that block and it is therefore not an eigenvector of $A$.
this is why it is crucial that you diagonalize $B$, on the $A$ eigenbasis, on a block-by-block (i.e. eigenspace by eigenspace) basis
17:37
@EmilioPisanty that's in the Math chat room description
so it's not a bad idea (though it gets ignored all the time)
i see
so because in a twofold degenerate eigenspace, any two orthogonal vectors in it are eigenvectors right? So you can break it into two 2x2 matrices each representing the eigenspace?
*an eigenspace
@Phase break what?
Break the 4x4 matrix into the two 2x2 matrices
but yes, any vector in an eigenspace is an eigenvector
and ignore the 2 2x2 matrices with zeros in all the elements
yeah but I mean when it comes to choosing what the eigenvectors are
17:40
@Phase No, that's not trivial, and you strictly require [A,B]=0 for that to be possible
ignore, misread you
?
Oh ok
im confused
Emilio what is your comment in response to?
@Student404Mus you want to take this abstrusegoose.com/272 from step 3 onwards
@Phase the fact that the representation of B in the A eigenbasis is block-diagonal
Sorry im not familiar with the term block-diagonal
i.e. that it can be broken down into the direct sum of two 2x2 blocks
17:42
oh right
Well
@EmilioPisanty oh man, that's great
huh
ok thanks emilio
@Phase $\begin{pmatrix}P& 0 &0 & \cdots\\ 0& Q & 0 & \cdots \\ 0& 0&R&\cdots \\ \vdots & \vdots & \vdots & \end{pmatrix}$ where $P,Q,R$ are submatrices and the zeros are rectangular matrices of zeroes
for a physics grad student it's more like "well, i've got half the books on my table. but do i really want to do the other half?"
@EmilioPisanty I still love the "Witten to English Dictonary"
3
17:43
@ACuriousMind yup
wait how would you expand that
for some reason it always takes me ten minutes to find that one every time I want to cite it
reminds me, there's a paper of his I still need to read
Is A the whole matrix, and then B is the whole matrix minus A's column and row and so on
@Phase exactly like the B representation on A in the original example
17:46
I'm interested in Lefschetz thimble stuff
and Witten has some good stuff on that in one of his papers
Kip Thorne's brilliant interview after winning the Physics Nobel of 2017 !
@AlexKChen ah. well played.
Yeah, isn't it very interesting ?
@EmilioPisanty Hey. I forgot to list Fourier analysis in the prerequisites. I guess that should be (-1a).
@dmckee not to be too pratronizing but what do you even need? Definition and formal manipulations?
vzn
vzn
18:00
@Semiclassical ... solitons ... =D
Hi @vzn
vzn
vzn
@AlexKChen hey
Is the book by Klepneer and it's exercises good for learning basic Newtonian mechanics ?
Anonymous
@dmckee I have a C question: When I use scanf("%3d %3d %3d",&a,&b,&c); here why does b get the value 4 and not 456? Using %3d %3d %3d should extract non-whitespace consecutive (3) characters and place them in the variables a, b and c respectively, isn't it ? Any ideas?
Anonymous
18:38
Ok, I got it now. "three consecutive non-whitespace characters"
Anonymous
"3" is the maximum field width here
18:55
Thoughts on whether this question is clear enough to be reopened?
0
Q: Detecting light path

Ilya_GazmanIs it possible to build a machine that will be able to detect a path chosen by a ray of light? My idea is to created stations along the path of the light, each station is a device that absorb part of the light and redirect it to all the other stations. My goal is to detect when the light have ...

@Blue yeah, when you provide a field width, that's only the maximum number of characters it will read. It still stops on spaces etc.
I didn't think using field widths with scanf was very common but I'm not sure
@AlexKChen flagged
Anonymous
@DavidZ Yup, got it!
Anonymous
@DavidZ I found it in a book. I too have never seen real code using field widths for scanf before.
@Icemybread don't say you're flagging things. If you're going to flag a message, just flag it, there's no need to announce it.
@Blue yeah it sounds like the kind of thing that would appear in a book and nowhere else
@BalarkaSen Is Hirzebruch's book on algebraic geometry good? I was just handed it
19:09
i heard of it a few times
too heavy 4 me
You mean topological methods in algebr geom right?
19:21
@BalarkaSen Yeah
My advisor says that Hirzebruch explains what the mysterious A-roof genus is
@Semiclassical but things change based on us observing them...
@0ßelö7 Well, what you really need is the understanding that you can form arbitrary(*) functions by summing over the basis functions, and that there is a methodical approach to finding the coefficients of the sum for any desired result.
(*) For 'physicist' values of arbitrary, of course.
@dmckee you know me too well
@BalarkaSen I'm about to give Talk 1 a run and see how long it takes me. Do you want to Skype
19:40
@0ßelö7 i don't skype. use a rubberduck
"Here, B is any so-called Bott manifold i.e. a simply connected
8-dimensional spin manifold"
Wonderful
wott manifold
@BalarkaSen What's the bordism group of $n$-dimensional spin manifolds
I'm in algebraic topology hell, pls halp
Don't think there's a simple description
what the hell does any of this mean
19:50
Oh, right there's a Pontryagin Thom theorem for cobordism groups with additional structure
How would I even go about finding out what this stuff is
Are you being unhelpful on purpose?
nopeee
So you don't know what it is either?
19:52
I don't know what the general form of Pontryagin-Thom is, no, but I have definitely seen it flying around
Maybe check out tom Dieck
@BalarkaSen dam son
I'm in the library right now
this book looks lit
tom Dieck?
yeah
I liked that book
There's a chapter on Thom spectra iirc so that might be useful
19:54
@EmilioPisanty 7: me irl
I have 3 weeks to learn that stuff
and write it into the talk
and somehow not seem like an idiot
...
Teach me after you learn it
@BalarkaSen kk. Really I just need enough to understand the statement of the theorem lol
I'm trying to find the state of the art on obstruction theory for positive scalar curvature metrics
it's a homotopy theoretic mess
unsurprisingly
dem homotopy theorists everywhere
19:57
@BalarkaSen My advisor pulled that stunt again
Gave me a paper that he definitely does not understand
gave me a false sense of hope
Who you calling a homotopy theorist
20:29
@ACuriousMind or @DavidZ or @dmckee or @Qmechanic would you mind paying a bit of attention to this question? Under the answer by user171097, there are quite a lot of comments that are more like quarrels and will not be useful to future users. Please delete them as necessary. Requesting here as it's not possible to flag every comment.
@WrichikBasu Just flag one of the comments in such cases, we'll deal with it
-2
Q: Why centripetal force does not pull the object towards the center?

reghuI know that the force is used to change the direction of the velocity but my question is while it has 3 options either to pull the object towards the center or change the direction of velocity or both. It would have been more appropriate if it did both.

@WrichikBasu The usual thing is to flag one comment with a custom reason and explain that there is a mess.
@dmckee should I do it now, or you'll look to it?
I'll keep that in mind from next time.
We're looking at it now.
20:31
@dmckee ok. :-)
how can i find the function of a string that is between two points
Anonymous
@nasil What?
Anonymous
What string?
you take a rope
Anonymous
20:42
@nasil Ok, then?
Anonymous
What function are you looking for ?
take arbitary two points on that line
then pin those points on some arbitrary points in 2d space
Anonymous
So, you're looking for standing waves on a string.
Anonymous
Plenty of information about that stuff on the net
Anonymous
Just look around a bit
20:45
i am looking for the right word
and that is not what i am looking for
Anonymous
Start from here
lets make up two cordinates
y and x
x horizontal
and is f(x)
every x y pair represents a point on the rope
@dmckee cc @WrichikBasu FWIW I usually look at the full comment thread even if there's a standard flag on just one comment.
@Blue did you understand the question?
Anonymous
20:47
In physics, a standing wave – also known as a stationary wave – is a wave which at each point in its medium has a constant amplitude. The amplitude of the wave's oscillations may vary at different points in space, but are constant in time. The locations at which the amplitude is minimum are called nodes, and the locations where the amplitude is maximum are called antinodes. Standing waves were first noticed by Michael Faraday in 1831. Faraday observed standing waves on the surface of a liquid in a vibrating container. Franz Melde coined the term "standing wave" (German: stehende Welle or Stehwelle...
length of the rope is given
its not a standing wave
it is just a stationary rope
That sounds like the catenary problem
thanks a bunch
Anonymous
Oh. That should be hyperbolic.
Anonymous
So you were not looking for waves
20:49
nope
Anonymous
In physics and geometry, a catenary (US: , UK: ) is the curve that an idealized hanging chain or cable assumes under its own weight when supported only at its ends. The catenary curve has a U-like shape, superficially similar in appearance to a parabola, but it is not a parabola. The curve appears in the design of certain types of arches and as a cross section of the catenoid—the shape assumed by a soap film bounded by two parallel circular rings. The catenary is also called the alysoid, chainette, or, particularly in the materials sciences, funicular. Mathematically, the catenary curve is the...
Anonymous
"Mathematically, the catenary curve is the graph of the hyperbolic cosine function. "

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