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14:00
The Laplace Runge Lenz vector is a constant of motion in the Kepler problem, right?
"Classical mechanics" is so broad as to convey no useful info - I can imagine many parts of it I'd like to discuss, and equally many I wouldn't like to discuss
@ACuriousMind :P
@TheDarkSide Yes.
@rob mind your 's in 't Hooft
@BalarkaSen Can't say that here. Greenleaf seems like a fairly known band. How come I didn't know about them..
14:02
@ACuriousMind is there any work these days for non-Euclidian space path integrals
@JohnJack My point is that your "specific case" doesn't simplify anything. In mathematics, we generally only prove things for specific cases if the proof there is somehow different from the general case, which is not the case here. Whenever I read the proof of something and some hypothesis does not seem to be used, I wonder whether a) I did not understand the proof or b) the author did not understand the proof, since they thought it necessary to restrict to a specific case.
Path integrals without Wick rotations
@ACuriousMind OK, now in order to define the position vector, we need some origin of co-ordinates ...
@TheDarkSide No. :P
rob
rob
@EmilioPisanty Delayed editing of comments is a nice superpower.
14:03
@Avantgarde so... is that basically edm?
@rob correct spelling on the first try is a nicer one
so that we can define $\vec A = \vec p \times \vec L - mk \hat r$
I can view position as an element of an affine space without any choice of origin. However, in order to do useful things with that, I'll need to choose coordinates and therefore an origin.
@ACuriousMind Yeah agreed.
@rob $\Large{😝}$
14:04
@Cryolune Lol, I was just joking about that. Balarka likes progressive/psychedelic rock, at least.
@ACuriousMind @rob Moderator access to PII is logged, right?
@EmilioPisanty Yes
@ACuriousMind Yes. So, that poor origin is at the center of the gravitating body?
@Avantgarde That's ok. I was more asking if you knew Bengali, because I know of a 70's band from Bengal that I'd recommend pretty much literally anyone. :P Yeah, Greenleaf is really good.
@BalarkaSen Greenleaf seems alright. Mix of hard and stoner rock
14:06
@TheDarkSide Usually, yes.
rob
rob
@EmilioPisanty Of all the languages where I'm a good speller, Dutch isn't one of them.
@BalarkaSen Oh sure, I don't care about the music's language. Share away
@ACuriousMind Alright. How about we shift the origin to some other more convenient spot?
Sure, you're allowed to do that.
@rob oh, for sure
but then that's what google is for
14:07
@Avantgarde Lmao because it wasn't making any sense. I was searching the artists/bands you referred to and also progressive dance pop and it did not really fit. xd
@Avantgarde Moheener Ghoraguli. I think they are the oldest rock bands of India or something?
Note, however, that then the formula for the conserved quantity that's the L-R vector of course changes.
(i.e. for googling the spelling before you post =P)
@Cryolune hahahahahaha
@Cyolune I do like progressive dance pop though. As an example.
14:08
@ACuriousMind Yes it does. OK. Now, suppose I pick a point on the orbit as the origin. The physics doesn't change, it is only a co-ordinate transformation...
@BalarkaSen The vocals are very nice. Well, they're Bengali
@BalarkaSen I don't really have any specific genre of music I listen to because I like basically any song that's interesting to listen to, from any genre.
Sometimes it feels like I'm he's talking physics lol, since there are many Bengalis in physics
but I think most of songs people link me or what I find ends up being some form of EDM for some reason.
@Cryolune Wait, I'll show you something that's not EDM
14:13
@Avantgarde Here is my favorite album of them by the way. They use unreal guitar riffs at places.
The lyrics is good but of course unintelligible to non-natives :P
rob
rob
@EmilioPisanty I would argue that particular apostrophe is especially tricky. I mean, I was just looking at the user page where it is spelled correctly. It's sort of like a a repeated article -- something ordinarily small that sometimes parses as correct even when it isn't.
@ACuriousMind - What I'm trying to figure out is, what is we do this problem backwards? i.e. given a satellite in orbit, suppose I record the co-ordinates relative to some origin and the velocities, I must be able to determine the LRL vector and hence, this constant of motion, right?
@BalarkaSen unintellegible, not unintelligent ;P
rob
rob
I mean, I had just looked at it.
14:14
@ACuriousMind That's what I said, man
@TheDarkSide Sure, just look at the formula for the LRL vector and see how it transforms under the coordinate change from the gravitating body as origin to the satellite as origin. There's your formula.
Of course, it would be very difficult to figure out there even is a LRL vector if you had never seen the standard derivation. That's why clever choice of coordinates matters.
@BalarkaSen Yeah, I can't understand what they're saying. But it's nice
@Avantgarde What genre is that?
(Maybe @Blue would like them. I think he knows Bengali?)
@ACuriousMind Just a small problem with that. If the origin is in the orbit itself, I'm unable to imagine what all happens to the three vector terms all along the orbit ...
Anonymous
14:20
@BalarkaSen Which one? (I do know Bengali :P)
@Cryolune Industrial black metal
e.g. look at $\hat r$
@Blue Scroll up a few messages, I linked Avantgarde an album of Moheener Ghoraguli.
I don't know if you know of them or how much you have heard of them.
Anonymous
@BalarkaSen Oh sure. Checking.
Anonymous
I haven't heard of them before just now though :P
14:21
They're relatively unknown, which is a shame.
At half an orbit away, it points e.g. from what we call a perigee to the apogee
@Avantgarde I have a friend who loves this kind of music and he plays it too.
Now, velocity is tangential to the trajectory at any instant.
@Cryolune Yeah, I knew quite a few people. I'm not sure if you liked it though? :P
@Avantgarde It's alright. I'm used to being linked similar songs so I've learned to like it. xd
Anonymous
14:25
@BalarkaSen Just listened to this. Yeah, it's really nice! I like calm tunes like this one. Will surely listen to more of this band. :)
So, for $\vec L = \vec r \times \vec p$, won't $\vec p$ point in the same direction as earlier @ACuriousMind?
only a change in $\vec r$, and hence in $\vec L$, and hence in LRL?
@Blue Yeah they are fantastic. They're from the 70's, and the members were part of the Hungry generation.
If you ever want to listen to them rigorously start with this.
Basically, something similar has been dished out earlier : physics.stackexchange.com/questions/208863/…
Or am I mistaken with my $\vec p$ direction preservation guess?
^ I suspect so.
So, the reason why I throw this here is, is an explicit calculation the only way of finding out, or can we deduce?
Anonymous
@BalarkaSen Yep, I'm listening to that now! What's Hungry generation btw? :P
Anonymous
The Hungry Generation (Bengali: হাংরি জেনারেশান) was a literary movement in the Bengali language launched by what is known today as the Hungryalist quartet, i.e. Shakti Chattopadhyay, Malay Roy Choudhury, Samir Roychoudhury and Debi Roy (alias Haradhon Dhara), during the 1960s in Kolkata, India. Due to their involvement in this avant garde cultural movement, the leaders lost their jobs and were jailed by the incumbent government. They challenged contemporary ideas about literature and contributed significantly to the evolution of the language and idiom used by contemporaneous artists to express...
Anonymous
14:33
Ow
70's counterculture in US influenced a massive stoner culture in Bengal
that's what it is
Anonymous
My knowledge of History is poor. Ah, interesting!
surely they're not taught in any history textbook you will see in school, one does not simply turn a kid into a Naxalite :P I got to know about them very recently.
Anonymous
naxalite...lol XD
What are some unsolved problems in the areas of quantum mechanics and particle physics which once solved, will be revolutionary to our way of perceiving the world.
I am going to solve them.
Anonymous
14:40
Some of the major unsolved problems in physics are theoretical, meaning that existing theories seem incapable of explaining a certain observed phenomenon or experimental result. The others are experimental, meaning that there is a difficulty in creating an experiment to test a proposed theory or investigate a phenomenon in greater detail. There are still some deficiencies in the Standard Model of physics, such as the origin of mass, the strong CP problem, neutrino oscillations, matter–antimatter asymmetry, and the nature of dark matter and dark energy. Another problem lies within the mathematical...
Anonymous
Good luck :P
Good luck indeed.
don't forget us when you win the nobel prize
Are you going to solve ALL of them?
Anonymous
Please give me a share of the Nobel Prize too for giving you the list of the unsolved problems. XD
14:42
@rob I'm not sure who you'd be arguing that against
that apostrophe is possibly the trickiest one of all
Down to a more fundamental (or crap) question:
What happens to the unit vector $\hat r$ when this $\vec r = \vec a - \vec b$, and $\vec a$ and $\vec b$ refer to the same points?
Of course, the magnitude vanishes.
But unit vector?
$\hat r = \vec r / r$ is a $0/0$ form in that sense?
Or have I completely lost my mind?
Where will the unit vector point?
"and why observed spacetime has 3 spatial dimensions and 1 temporal dimension?"
isnt this wrong
its from the link you gave
just because nothing travels faster than light there is 4 dimensions in total
Once this is settled, the LRL vector shall be settled too ...
and we assume nothing travels faster than light
we dont consider the imaginary dimension
there would be 8 dimension if we accepted that there are things which can travel faster than the speed of light.
@OmarKhayyam if you're planning to revolutionise physics you aren't making a great start.
14:57
noononononononononono
@TheDarkSide What do you mean "unable to imagine"? You should be able to tell how each of the three vectors transforms, you're just doing a shift $r\mapsto r + r_0$.
No imagination involved
i am just asking
for a friend right?
@TheDarkSide There is no unit vector.
and actually where is the best start point to revolutionize physics
14:58
@OmarKhayyam learn it first?
6 mins ago, by The Dark Side
What happens to the unit vector $\hat r$ when this $\vec r = \vec a - \vec b$, and $\vec a$ and $\vec b$ refer to the same points?
The zero vector is the one vector that doesn't have an associated unit vector.
@ACuriousMind exactly!!
So, what happens to the second term in LRL?
do you know cern beamline
i want to run an experiment
$-m k \hat r$
15:00
i need to know what is unknown in physics
Anonymous
@OmarKhayyam Maybe you need to learn what is "known" in Physics, first.
thats not a good argument
@TheDarkSide Ah
@OmarKhayyam I'm afraid it is a good argument.
@ACuriousMind do you mean spoon?
15:01
spoon?
how can you know what is unknown by learning what is known
@OmarKhayyam By observing the gaps in what is known. Learning what is known is the best possible way to understand what precisely we do not know.
@OmarKhayyam because then you only have to 'UN'do all that is known.
so why cant you tell just one gap
Anonymous
15:03
@TheDarkSide lol :P
@OmarKhayyam we don't why Yang-Mills theories with a compact gauge group exhibit confinement, or even if all Yang-Mills theories with a compact gauge group exhibit confinement. Solving that one will win you a million dollars.
@OmarKhayyam how can you possibly determine whether some bit of physics is unknown if you don't already have a solid grasp on the bits we do know?
@JohnRennie we don't why?
So, have we broken Laplace-Runge-Lenz vector with this choice of origin? @ACuriousMind
how can i learn the bits that you know
15:05
@EmilioPisanty that's the mass gap millenium problem.
@JohnRennie yes, but the sentence seems to be missing a verb ;-)
@TheDarkSide You just have that the $\hat{r}$ becomes a $\hat{r'}$ for $r' = r - r_0$, where $r$ is now your coordiante as measured from the new origin and $r_0$ to position of the gravitating body in that system. That won't ever be zero.
Anonymous
@JohnRennie He was pointing out the grammatical error in "we don't why" I guess. :)
@TheDarkSide No, you're just doing the coordinate transformation incorrectly :P
@ACuriousMind Hold on a second :P
15:07
@EmilioPisanty oops yes :-) Dang, it's too late to edit now. Oh well :-)
i have a copy of principles of qm by mr. dirac
is it outdated?
@OmarKhayyam what does 'outdated' mean?
it's a spectrum
you would not read einstens first papers of relativity if you wanted to learn relativity
Anonymous
@OmarKhayyam I don't know if you are trolling. But I guess you should start with learning Physics from standard textbooks and University lectures.
@OmarKhayyam I would not recommend Dirac's Principles of QM as a starting point in QM
15:09
i finished the serway the last summer
But it's still a valuable resource
i am also training for ipo
i just dont know qm
Dirac's QM will probably teach you some nomenclature that we don't use anymore, and not teach you some that we do use, but there should be nothing wrong in it.
@ACuriousMind o.o
so what is the best resource for qm
15:10
Are you really going to say that classical QM is not wrong?
@OmarKhayyam assuming that everybody in the world knows the meaning of every acronym of your local examinations board won't really help you communicate much
It's pretty much 100% wrong
Technically speaking
international physics olympiad
= ipo
60
Q: What is a good introductory book on quantum mechanics?

PhaDaPhunkI'm really interested in quantum theory and would like to learn all that I can about it. I've followed a few tutorials and read a few books but none satisfied me completely. I'm looking for introductions for beginners which do not depend heavily on linear algebra or calculus, or which provide a s...

Anonymous
@OmarKhayyam That's IPhO and not IPO.
15:11
IPhO*
@OmarKhayyam "Quantum Theory for Mathematicians" by B. Hall
@0celouvskyopoulo7 Yes, I am going to say in a physics chat in a physics context that there is nothing wrong with QM.
yes i call it ipo
big deal
@ACuriousMind Oh. I thought this was a cooking, music, and math chat.
@0celouvskyopoulo7 you want him to die?
15:12
That no one here shares your standard of rigor is your problem, not mine :P
thanks @EmilioPisanty
@ACuriousMind I can play loose with rigor
look
That's...not playing loose with rigor :P
@0celouvskyopoulo7 can you, really?
@TheDarkSide depends
a little functional analysis has never killed anybody
@EmilioPisanty There's one proof where say that someting is a diffeomorphism, but tbh I didn't actually check that
Does that count?
15:15
@0celouvskyopoulo7 not much, no
what is time orientability
is this equivalent to having a 1 dimensional trivial line bundle in TM
I reckon it's relatively easy to come up with some delta-function manipulations that'll make you choke on your own tongue
@BalarkaSen No.
but I can't be bothered to think them up
15:16
$$\sum_{k=1}^na_i\delta^k(x)$$
Mathematicians will cry at horror to this
what is timelike
@BalarkaSen $v\in T_pM$ is timelike if $g(v,v)<0$
ahhh ok
time orientable means it is possible to continuously define a "future"
@EmilioPisanty We did have that paper that Taylor expanded delta functions once...
15:18
@EmilioPisanty wait, what?
@ACuriousMind ah, yeah, that's what it was
I'm confused as to what I'm being accused of
And why I would choke
Mar 16 at 18:29, by 0celo7
He's Taylor expanding a Dirac delta holy shit
that paper was satan. So?
I reckon a power series delta function is even worse
15:19
@0celouvskyopoulo7 $$\delta(x-x_0) = \sum_{n=0}^\infty \frac{(x_1-x_0)^n}{n!} \delta^{(n)}(x-x_1)$$
@Secret You can't multiply delta functions, so yeah.
Pretty awful.
let's see you use that in practice
@EmilioPisanty You know, that's not even that bad.
then you can say that you can play loose with rigour
The derivatives could be distributional and the series might converge in the $\mathscr D'$ topology
15:20
@ACuriousMind - Remember that bad gravity analogy. Ball on a membrane.
@0celouvskyopoulo7 the fact that you're quibbling about that stuff instead of just rolling with it takes you out of the play-loose game
distortion of spacetime ...
Nowadays I just think of a grid of cloth where the grid itself get distorted without the cloth become buckled
So, the ball on the membrane is (a bad) example of a satellite ...
that eliminates the "need to embed in a higher dimension" problem
15:23
In other news, I just found out that Pasteur discovered molecular chirality when he was 24
I wonder how my knuckles smell like Canadian bacon
it's people like that that make you realize how little you've accomplished
They certainly never touched any
@EmilioPisanty and I still can't fix coordinate transformations... (cf. above) :D
@EmilioPisanty Lebesgue discovered measure theory while trying to solve some PDE
15:23
for instance, it's well known that when Évariste Galois was my age, he'd been dead for nine years
he couldn't get the Riemann integrals to converge so he just YOLO'd it
he did that as a small part of his thesis
So, back to the point, how do you choose the LRL for this problem, the origin: "center" of gravity is sitting where?
("warped" space)
@EmilioPisanty I'll bet your life has fewer duels than his, though
(with due apologies to Tom Lehrer)
@TheDarkSide I do not understand the question
15:27
@ACuriousMind If we were in 1800 would you accept my challenge to a duel?
@ACuriousMind Of course, the paradigm itself is wrong. But just saying ...
Depends on how good I'd actually be with the weapon ;P
@ACuriousMind Take a fabric, launch a marble on it.
As bad as the analogy is, it can simulate a satellite.
In this sense that it orbits.
no, there's no 1/r^2 force
Just "orbiting" is not enough for a LRL vector
0
Q: Other spaces like Fourier space

Hosein HashemiAre there any other spaces like Fourier space in which one can more physical information than configuration space? In a summer school about scattering amplitudes, someone told me that this relation between twister space and scattering amplitudes is like the correspondence between Fourier space an...

too broad?
15:29
@ACuriousMind OK. Just give me a minute.
@ACuriousMind isn't it amazing how math experience works?
A year ago I was unable to understand this proof, and asked a few professors for help and still didn't get it
@ACuriousMind - can you access this?
Yesterday I did it without looking at the book
Quite strange how something goes from impossible to routine
Although maybe all of life is like that
life is nonexistent simplicity
@BalarkaSen here's a question...does the existence of a Lorenztian metric imply the existence of a Riemannian one?
that is, does a Lorentzian metric imply the manifold is paracompact
@Slereah ^
15:37
I was about to ask what that even means, but then I realized you have nonstandard definition of manifolds
@0celouvskyopoulo7 That's clear from the proof of the theorem.
:P
Slereah would probably be able to answer that better than me, certainly
@BalarkaSen Yeah, assuming "manifold" does not mean paracompact, for the moment.
It should be noted that Kobayashi and Nomizu do not assume manifolds are paracompact.
how vulgar
So in half the book they have to write "if M is paracompact"
For a Riemannian metric, you can show that it induces a distance function, hence $M$ is metrizable. Stone's theorem implies it is paracompact.
But if $g$ is Lorentzian...there's no distance function.
15:42
@0celouvskyopoulo7 If you have a Lorentz metric just do the reverse construction of the usual thing
$$h = g + 2\frac{\xi \otimes \xi}{g(\xi, \xi)}$$
Or something
What's that supposed to do
Define a Riemannian metric tensor
15:43
also from the Steenrod theorem you can see that a section of Lorentz metrics means you always have a Riemannian metric
It relies on some matrix theorem showing that a matrix of that signature is the product of a Riemannian one and some other matrix
Wait how do integral curves work
Why does $X(\gamma)$ make sense
$\gamma$ isn't $C^\infty(M)$
Apparently there's a Ruse
You define $\gamma$ as the equivalency class of functions $f \circ \gamma$ for all $f \in C^\infty (M)$
or something
I don't understand the question. Integral curve of $X$ is a smooth curve $\gamma(t)$ such that $\gamma'(t) = X(\gamma(t))$
I'm guessing it's covered in the isomorphisms between vectors as tangents and vectors as derivations
Well yes, but $X$ doesn't act on curves, it acts on smooth functions
(of M)
$M \to \Bbb R$ not $I \to M$
$X(\gamma(t))$ is the vector on the vector field $X$ at $T_{\gamma(t)} M$
It's not acting on anything
$X(p)$ means the vector at $T_p M$
Ah alright
I also dislike this notation, btw :)
15:55
I thought it was the action of the vector on a function
@0celouvskyopoulo7 You know J Peter May right
This isn't my stupidest confusion, really
One time I was stuck for days on some expression that involved $\sigma^2$
Turns out it was the second Pauli matrix, not a square
Notations, notations
Let us make some math which does not use any notation whatsoever
Or it could be some kind of telepathic thing.
Also that sounds weird.
@0celouvskyopoulo7 there are paracompact spaces that are not metrizable
16:08
Paracompact and hausdorff he means, I assume
Although you can certainly define metrics on a non-hausdorff manifold
still there are paracompact and Hausdorff that are not metrizable
Much better than a non-paracompact one, anyway
@yuggib and second countable :p
(and connected)
although I'm guessing that if it's all that, it admits a Riemann metric anyway
if it is second countable and paracompact and Hausdorff, then it is metrizable
yeah
but anyway, I think my point remains
@yuggib I never claimed that was the case?
16:11
Even if it's not metrizable, if it admits a Lorentz metric tensor, it admits a Riemann metric tensor
It's just that the Riemann metric tensor may not define a distance function
I claimed a metric space is paracompact.
@BalarkaSen the algebraic topologist?
@0celouvskyopoulo7 I know. But you complained they had to write it explicitly, even if it is necessary to do it if you deal with non-metrizable spaces
@yuggib Most people take paracompact to be a part of the definition of manifold
they didn't, so for stuff where they need a metric, they had to specify paracompactness
question merges are weird
10
Q: Why is the speed of light defined as 299792458 m/s?

XplaneWhy is the speed of light defined as $299792458$ $m/s$? Why did they choose that number and no other number? Or phrased differently: Why is a metre $1/299792458$ of the distance light travels in a sec in a vacuum?

I'm not sure what you're talking about
16:15
click on the "Active 1 year and 4 months" link on the right
CC @rob
Spivak's DG appendix proves paracompact = metrizable = etc if that is what you are trying to prove
16:32
I am not trying to fucking prove that
God dammit people
Anonymous
@JohnRennie lol, I suppose you had several quarrels with the Oxford guys during your grad days XD
@Blue no, there was never any real rivalry, or at least none that I was aware of. There was the boat race of course, and various other sporting fixtures like rugby, but the science students seemed generally not very interested in these.
@0celouvskyopoulo7 Correct. Now watch this
16:48
@JohnRennie In my experience (mostly confined to the world of academic research), only the graduate programs of these "high-ranked" universities stand out (and not always) compared to the others. And of course, they are able to hire very good people. But I cannot see such a difference in effectiveness/quality when it comes to undergraduate programs.
BOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOO
Hey guys
How are y'all doing?
DID YOU HAVE A NICE
DAY?
@0celouvskyopoulo7
What symbol for vector flow
$\Phi_X$?
Meh day overall. Trying to finish up some last work.
Meh day overall. Trying to finish up some last work.
Haha.
16:53
I'm having fun by acting in a stupid manner.
0
Q: Energy density of dust in f(R) gravity

Naveen BalajiUsually during the calculation of the Einstein-Hilbert action, we consider the integral of the variation of the Ricci tensor to be zero as the variation of it, at the boundary was assumed to be zero, as: $$-\frac{1}{16\kappa{\pi}}\int{d^{4}x[\delta\sqrt{|g|}(R+\Lambda)+\sqrt{|g|}(\delta{g^{\m...

Anyone? please
17:28
@Slereah that or $\mathrm{Fl}^X$
fairly ugly
let's go with Phi
@EmilioPisanty Have you seen this?: physics.stackexchange.com/questions/340190
I'd like to know the answer for the orbital angular momentum
17:44
Can someone please help me understand atomic structure? I am tired of reading contradicting stuff every where :'(
@Slereah if you say so
@Slereah What's a good TeX editor for PC?
I use texstudio
I have also used texwork in the past
Both are fine
Anonymous
@Abcd What type of help?
I use sharelatex :3
@Blue I can't understand the difference between Principal Quantum Number, Energy Levels, Orbits and Shells. They all seem to mean the same.
17:55
@BalarkaSen Hippie
@BalarkaSen I will watch your video after work
principle quantum number is a number, and orbit(als) are regions (where the electron lies with high probability density) in the 3-space, so there's that :P
Anonymous
@Abcd They are essentially the same thing. The Principal Quantum Number is defined in a slightly different way. n=1 holds for electrons in first shell, n=2 holds for electrons in second shell and so on...
a number can't be the same as a region. it's just associated to the regions in some way
#pedant
@Blue :( . Circular orbits and energy levels are same!?
@0celo Sure, sure
Anonymous
17:57
@Abcd "Energy level" is a very vague term. But at your level, yes.
@BalarkaSen orbit(als)? WHy complicate things more :(
@Abcd The orbitals (not orbits!) are just the energy levels. Every orbital/energy level has a specific value of the principal quantum number, and a "shell" is the set of all levels with the same principal quantum number.
@Blue I am in Grade 11.
@Blue is it vague?
@Abcd Nobody is complicating anything. I am just saying a number cannot be the same as a region.
17:58
it's just the eigenvalue of the Hamiltonian
energy level is exactly what one calls it
Anonymous
@0celouvskyopoulo7 Yeah. Depends heavily on the context.
@Slereah Can you please read my Section 1.2?
I am actually quite proud of it
I managed to avoid the argument in Wald with the auxiliary metric

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