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7:03 PM
The physicist proof is just Fourier transformation
 
@JohnRennie ::pokes::
 
@BenNiehoff not a genitive, a patronym
I can't point you to anything rigorous, though
 
@EmilioPisanty sad side effect of being a physicist
 
@0celouvsky har har
have a go at this one if you're feeling uppity
3
Q: Does the $p^+p^-e^-$ system have bound states?

Emilio PisantyThis is batted a bit off the wall, so bear with me. The hydrogen molecular ion, $\mathrm{H}_2^+$, is the simplest three-body system in molecular physics, and in the Born-Oppenheimer approximation its electronic Schrödinger equation is separable (though it's unclear whether it's actually exactly s...

=P
 
@EmilioPisanty I don't do PDE with coefficients that are not $L^\infty$ :P
 
7:11 PM
@0celouvsky whazzat? You don't do physically relevant PDEs?
 
@EmilioPisanty heat flow on a Riemannian manifold is physically relevant :o
Apparently it has to do with the melting of ice cubes...
 
@BenNiehoff goodness me, the first page of Google results is absolute bull
the untrustworthy Spanish-language internet has this distinctly 90s web-1.0 feeling
 
Oh lord, the proof uses the Fourier-Laplace transform
Holy shit, any strongly elliptic PDE has a green's function
now THAT is not something your physicist magic could tell you
@EmilioPisanty what?
what the heck is a conjugate space
probably the dual...but why not say dual?
 
7:35 PM
@0celouvsky I was googling the -ez thing
Most search hits are people just making stuff up
But over really 90s web design
 
7:56 PM
@EmilioPisanty I found the answer to the -ez thing
== Breton == === Suffix === -ez f -ess; suffix forming the feminine of a noun ==== Derived terms ==== == French == === Pronunciation === IPA(key): /e/ Homophones: -er, -é === Suffix === -ez suffix forming the formal second-person singular or second-person plural (vous) present indicative of an -er verb. suffix forming the second-person plural imperative. == Hungarian == === Etymology === -e- (“linking vowel”) +‎ -z (“verb suffix”) === Pronunciation === IPA(key): [ɛz] === Suffix === -ez (verb suffix) Added to a noun to form a verb. hely (“place”) → helyez (“to place”) ==...
the patronymic suffix comes from Latin -icus, genitive -icī
but I guess the dream of the 90's is alive on the Spanish internet ;)
 
Anyone here familiar with using memmove to do a circular shift on an array in C?
 
@BernardoMeurer 1. no, 2. why?
do you mean a bitwise shift, or actually shifting one entry of the array to the next?
 
@BenNiehoff I have an array like [3, 1, 0, 0, 0], I want it to be [0, 0, 0, 3, 1]
 
and you think temporary variables are too expensive?
 
I believe you can do that nicely with memmove() but not sure how
@BenNiehoff I just wanted to try doing it with memmove to be honest :P
 
8:04 PM
I don't know, but I have a hunch memmove() can't make it wrap around
but I couldn't tell you for sure
the only low-level memory functions I've used have been malloc and free
 
Can someone walk me through why we ignore surface terms in integration by parts in qft most of the time?
 
That might just be right
Why malloc and not calloc?
 
that's free as in empty, by the way...not freedom, or beer
 
I always do calloc :P
 
@BenNiehoff can you walk me through it?
 
8:07 PM
@BernardoMeurer I forget the difference, what does calloc do?
 
@BenNiehoff your free function is actually FREE SOFTWARE if you're using GNU's libc!
@BenNiehoff Allocate and initialise to 0
 
@BernardoMeurer do you have a github account?
 
Generally safer than just doing a malloc
 
@Cows Nothing to do with QFT - we usually silently assume that physical fields fall off at infinity.
 
8:07 PM
@BernardoMeurer Oh, I just assume every memory location is junk until I've initialized it myself
 
@ACuriousMind omg I had no idea. Is there a physical reason why?
 
@Cows Surface terms are at infinity and we usually work in the infinite-volume limit. You do have to assume sufficiently-fast falloff of all of you fields
 
wow!
@BernardoMeurer what is your github handle?
 
@Cows Almost every field configuration you can write down that does not fall off at infinity will have infinite energy, which is a bit unphysical, don't you agree?
 
@BenNiehoff Fair, I just like to be double safe. Calloc is know to be slower than malloc though, which is something to keep in mind
 
8:09 PM
@ACuriousMind I agree totally
 
@ACuriousMind ridiculous
 
IIRC there was once some issue with some linux syscall that made calloc significantly slower than malloc
@Cows bemeurer. My previous answer was a link to my profile
 
@0celouvsky ?
 
spacetime is infinite, what's wrong with infinite energy?
 
@BernardoMeurer Indeed. And the only reason to use plain C is for something where speed is more important than high-level code structure. So, malloc it is!
 
8:10 PM
And besides, you'd have to justify why there's some magical point beyond which the field is <epsilon
I'm assuming there's no source or anything, just a magical field
 
@BernardoMeurer my github handle is kevintah add me. hehe
 
@BenNiehoff Note however that there are occasions where 0-initialization is needed, in fact the code I am working right now, and then calloc is often times better than malloc + zeroing
@Cows I'm not sure one can add people on GitHub
 
@BernardoMeurer I meant follow lol
 
@Cows There is another reason to ignore surface terms, which I call "What if my action had surface terms to begin with, that I've been ignoring this whole time?"
 
@BenNiehoff that's the "Why physics is unconvincing" Lemma
 
8:14 PM
@BenNiehoff Yeah, I saw that, but it's not particularly thick with references
 
wow
 
@0celouvsky That, in most cases, the "infinite" theory is really just for convenience and we're actually only interested in the theory inside a box.
 
@EmilioPisanty True, although it's quite plausible. They love their Visigothic heritage in Spain
 
@BenNiehoff "plausible" is what it says on the top of the door to the rabbit hole of folk etymologies
 
What do you call someone wearing all black in a dark room?
Invisigoth :D
 
8:16 PM
@BenNiehoff an emo
 
You are right that the reasoning doesn't work if I have an infinite matter-filled universe I'm trying to describe but that's simply not the goal of most physical theories.
@BenNiehoff lol
 
@ACuriousMind again...the universe is infinite and matter filled as far as we know
 
@0celouvsky So what? That's not what most physical theories are trying to describe!
We compartmentalize
 
@EmilioPisanty Sure, but folk etymologies are usually folksier than that :P
 
When you're desribing two attacting opposite charges you don't care that there's a third charge in Andromeda
 
8:18 PM
@BenNiehoff this feels pretty folksy tbh
 
When you're describing collisions in the LHC you don't care that aliens on mars are doing a similar collision experiment right now
 
it has that distinct mark of Too Good To Be True that distinguishes all good folk etymologies
 
And so on
 
@ACuriousMind If there's aliens on mars doing precisely the same experiments as the LHC I would most certainly care
 
@EmilioPisanty Well, it survives analogy with Italian patronymics
 
8:19 PM
@EmilioPisanty Sure, but for reasons entirely unrelated to your LHC calculations ;)
 
@ACuriousMind indeed
not that you'd catch me calculating anything relevant to an LHC experiment
unless, of course, they decide to turn it into an FEL in ten years, like they did with SLAC
 
@EmilioPisanty Are you versed in C low-level memory hax?
 
@ACuriousMind you really should
That would be pretty neat
 
@BernardoMeurer nope, but I can help with Mathematica if that's your thing
 
@EmilioPisanty We talk in a couple years when I get that class
I'll bother you a lot :P
 
8:21 PM
@BernardoMeurer good
I suspect you'll quite like the universal-representation aspect of it
 
How is 'spin' defined classicaly and not in quanum mechanics?
 
and you'll probably despise yourself for it, too
 
spin of say an electron
 
@JohnDoe "spin" is a tricky term
but there is such a thing as intrinsic vs extrinsic angular momentum
 
@JohnDoe it isn't
Inb4 Emilio or Bajoran say it is in some strange way
 
8:24 PM
classical spinors are certainly well-defined
just not classical fermions
 
@EmilioPisanty On page 4 of Sakurai he talks about the Stern-Gerlach experiment. He states that the magnetic moment $\mu$ is proportional to spin $\mathbf{S}$ but he doesn't mention what he defines as spin $\mathbf{S}$ and later refers to the $z$ component of spin i.e. $S_z$. This is before he introduces any QM, so I'm assuming he is relying on some classical notion of spin.
@BenNiehoff So there is no classical counterpart to quantum spin?
 
@JohnDoe I'm not sure my answer is particularly helpful
I wouldn't read too much into it
 
@JohnDoe if you model electrons as little balls of charge, then yes, they have a magnetic dipole moment that's proportional to their intrinsic angular momentum
that's the portion of their angular momentum that's independent of the origin
 
@EmilioPisanty what?
 
8:28 PM
@EmilioPisanty So spin is classically just taken as orbital angular momentum in a sense?
 
Has anyone actually done the calculation for the classical rotation speed of an electron?
 
if you literally imagine an object spinning, that is classical spin, sure...but you can only get spin 1 that way, not spin 1/2
 
As opposed to the orbital/extrinsic angular momentum, which transforms as $\mathbf L \mapsto \mathbf L'=\mathbf L - \mathbf r_0 \times \mathbf p$ under a translation by $\mathbf r_0$, with $\mathbf p$ the total momentum.
 
@0celouvsky Uh...assuming what electron radius?
 
@JohnDoe no
 
8:29 PM
@0celouvsky yes, it's a famous result! The electron magnetic moment is 2x what it "should" be
 
Damnit
 
note the if
 
@BenNiehoff spin 1 is still intrinsic, so not classical...
 
It's not hard. I think if you set a reasonably small radius you get faster-than-light rotation
 
@ACuriousMind we'll there's the classic tale of Pauli or whoever doing it and concluding all is lost
So I wonder what radius to use
 
8:30 PM
@EmilioPisanty Yes that's how he is modelling it I think.
 
@JohnDoe Ultimately, the spinning-ball-of-charge argument only serves to suggest that a hamiltonian of the form $H=g \mu_B \mathbf S\cdot\mathbf B$ might be an interesting thing to try
 
@BenNiehoff that's QFT, I'm not talking about that.
 
@0celouvsky no, QFT is for getting you the "anomolous" part; i.e., it's actually slightly more than 2x what it should be
 
but the intrinsic magnetic moment of the electron is just that, a fundamental property of the electron
 
@EmilioPisanty What do you mean by "universal-representation aspect of it"?
 
8:31 PM
the 2x just comes from quantum mechanics
 
@BenNiehoff @0celouvsky do you guys mean something like this physics.stackexchange.com/questions/205580/…
 
TBH I'm just worried that it will be yet another class that forces me to use proprietary malware
0
Q: Circular shifting an array with `memmove`

Bernardo MeurerSay I have an integer array like such #define MAX 5 int bar [MAX] = {0}; int foo [MAX] = {3,1,0,0,0}; Now I'd like to shift this array so that all null entries are to the left, i.e. foo = {0,0,0,3,1}. I thought I could do this by Finding the number of shifts I must perform Using memmove() t...

 
@BenNiehoff the Dirac equation gives you the 2. It's the higher order corrections that give the little extra
 
@BernardoMeurer the fact that code and data and variables all come in on the same footing
 
O.o
That sounds like BASH
 
8:33 PM
@BernardoMeurer no, way better than that
 
@EmilioPisanty I'm just trying to get an idea of what classical notion of spin Sakurai is referring to when discussing spin before ever mentioning any QM notions. And where the classical prediction of the SG experiment comes from. I think the spin in taken as orbital angular momentum of charge moving around a sphere.
 
@0celouvsky I could have sworn there was a non-relativistic equation that gave you the 2...like just writing the Schrödinger equation in spin 1/2
but ok
 
There is, but it's just a trick.
The Dirac equation gives it directly.
 
so you can take some big complex function/construct/graphics object/whatever, and operate on it with the same functions, say Part or Map or whatever, that you would use for some structured list of data
 
Obviously the Dirac equation is more fundamental
 
8:34 PM
@BernardoMeurer Mathematica borrows heavily from LISP for its basic structure
 
@JohnDoe So long as you understand that this is for motivation only, then yes, he's taking about a model that's just a spinning ball of charge with orbital angular momentum.
 
@BenNiehoff ::shakes::
 
@EmilioPisanty Okay thanks.
 
Ok opening calculus book now lol.
 
@ACuriousMind I agree with @OBE. You have a habit of responding to questions by immediately telling the asker that their question is bad/unclear.
And "what" doesn't even tell the asker what to clarify.
 
8:37 PM
Is it his fault that they frequently are? :P
 
@0celouvsky No.
I noticed just this morning a question on main where ACM responded with a comment basically telling OP "You have no idea what you're talking about". That's not particularly helpful.
 
Without contex I have to say there's a chance OP has no clue what he was talking about.
Especially if it was one of those posts claiming to have discovered something...
 
@DanielSank I see the point about the "what?", but my comments on the main site usually specify what irks me about a post, at least I intend to leave comments like that. Which one are you talking about?
 
@ACuriousMind Does this make sense to you?
He's using $||\cdot||$ for the $L^2$ norm in that section, so that equation doesn't make sense.
And I don't know what the "conjugate space" is supposed to be.
 
Why does the magnetic field have to inhomogenous in the Stern-Gerlach experiment?
 
8:51 PM
@0celouvsky I suspect the author forgot to divide the exponent by half on the r.h.s. then, and I agree with your earlier guess that the conjugate space is probably the dual
 
@ACuriousMind But if it's a Hilbert space, the dual should be itself unless I'm missing something.
 
what is the cheapest new car one can buy in 2017
 
@0celouvsky Oh, the dual is isomorphic to the original, sure, but I think the claim is that if you ask "What are the continuous linear functionals on $L^2_\epsilon(\mathbb{R}^n)$?" the answer is "integrating against a function from $L_{-\epsilon}^2(\mathbb{R}^n)$".
 
@ACuriousMind So the dual pairing is the usual $L^2$ pairing?
 
Yeah
 
8:56 PM
I'm not sure that makes sense, what is the inner product supposed to be?
 
Oh it's because there would be no force unless it was.
 
that's actually quite handy
 
But since I know neither your context or what this is supposed to be for, I don't know any more than you do
 
Time to hunt down Hörmander's original paper unless @yuggib is around
 
8:57 PM
rubs eyes
last midterm tomorrow: statistical physics
 
rob
@JohnDoe Yes, a magnetic dipole feels a torque in a uniform field, but a force in a nonuniform field.
 
@rob Understood thanks.
 
@rob I asked Handler this last semester but he didn't know. Suppose I charge a capacitor and just yank it out of the circuit. What happens?
 
@0celouvsky never do that
 
rob
@0celouvsky You have a charged capacitor in your hand. You can use it to zap people. When you compute $RC$, use a half-megaohm for the skin resistance of your target.
 
9:01 PM
an explosion at the very least
 
rob
@EmilioPisanty You and I are thinking about different-sized capacitors.
 
@ACuriousMind
Let's see about this dual business now
It's just $L^2$ with a different measure, and such spaces are well-studied
 
@rob he did say a 1F capacitor under 100kV, right?
 
I don't know why this is confusing me.
@EmilioPisanty jayzus
 
wait
@0celouvsky is that Zeus in bird form?
 
9:03 PM
It's Kanye West in Ancient Greece
Er
Jay Z in Ancient Greece
Ok apparently it's just the dual
Time to prove that
 
rob
@EmilioPisanty $U = \frac12 C (\Delta V)^2 = \rm5\,GJ$, holy cow, why would such a thing exist?
 
Why did he say "under" 100kV
 
@ACuriousMind I'll try to remember to notify you next time I see an example. This morning is had something to do with translations on manifolds.
 
Why not make it more?
 
@rob so roughly 10ktons?
 
9:06 PM
Why do you think a general curved spacetime has a "generator of translations"? What does "translation" mean to you on a general manifold? — ACuriousMind ♦ 4 hours ago
 
yeah, as I said, explosion, definitely
 
@ACuriousMind That seems fairly condescending
 
@0celouvsky I was going to say this was on the "usefully Socratic" end of the spectrum.
 
He probably just means a transitive isometry group or something...
 
There are others that are less so.
 
rob
9:08 PM
@EmilioPisanty Yeah, I was thinking millifarad, 10V, like you might extract from a wall-wart power supply. Not explosion.
 
@rob boring, though
 
@rob Oooooh we're blowing things up?
 
for extra fun, though, you could plug it back in the wrong way and then turn the circuit back on
 
rob
@0celouvsky, or whatever your name is today: don't zap people with a gigajoule capacitor. Strictly a low-voltage phenomenon.
 
O'0celouvskyopolous
3
I like it
 
OBE
9:09 PM
@0celouvsky lol if you actually do that.
 
@rob But, science!
 
@0celouvsky It does? I have genuinely no idea what a translation might be on a general manifold! Is it the quotes? How could I have asked less condescendingly for what OP means by "translation" in their question?
 
@ACuriousMind It's the italics imo
 
OBE
@0celouvsky I see you figured out the infinite name change glitch.
 
speaking of kilotons, though
 
9:10 PM
@OBE I did?
 
boy does googling anything remotely nuclear end up with some gruesome science
 
I just changed my name, what's a glitch about it?
 
These guys are pretty good
 
OBE
@0celouvsky you changed from 0celou7 to 0celouvsky in less than 30 days.
there's a glitch that allows you to do that which I revealed last year.
hasn't been fixed yet.
 
Hey guys, I always hear and read that the signature of spacetime is a matter of taste of the author, but I never read what kind of taste. I mean what a guy using $(+---)$ prefers compared to $(-+++)$ and viceversa?
 
9:12 PM
@Runlikehell according to @ACuriousMind the signature matters for string theory
 
@Runlikehell $(+---)$ people tend to be your standard whisky on the rocks folks
$(-+++)$ are more G&Ts or rum and coke
 
^ What?
 
@0celouvsky Only possibly, and the existence of Majorana spinors is not something of purely string-theoretic interest
 
@EmilioPisanty My favorite drink is bourbon on the rocks and I use -+++
 
Whisky on the rocks is more "standard" than gin and tonic?
 
OBE
9:13 PM
from my experience advanced books used mostly minus and beginner books use mostly plus.
dunno why
 
@OBE no one asked you and you're wrong
 
@OBE Minus on what part!?
That is such a confusing comment.
 
@DanielSank I'm making this up as I go along, and in a hurry before all y'all post something serious, take it easy
 
OBE
@0celouvsky wow
 
rob
I find that whiskey by itself is neater.
 
9:15 PM
@rob har
har
 
did you have to link wiki?
what is it with mods and their link fetish
 
I'm not clicking.
 
@EmilioPisanty mmh what kind of guy (or alcohol) you think I should trust more?
 
9:16 PM
@EmilioPisanty I thought Zelda was the boy
Legend of Zelda, no?
 
link, I think
@0celouvsky wut?
 
what?
 
@Runlikehell seriously though, I think it just comes down to what notation your college textbook used
@0celouvsky why would you think that?
 
most people do
 
@EmilioPisanty ::take it not easy::
 
9:18 PM
and it's a meme, never mind
I know who Zelda is
 
@0celouvsky he says, five minutes later
 
She's the little fairy, right?
 
Hey, listen!
 
OBE
omg
i remember that
 
9:19 PM
@0celouvsky I had that as my sms notification for a while
folks from my parents' generations got weirdly upset by it
 
@EmilioPisanty got it, so one basically takes the signature used in the course he struggle more and has to use that signature for months eheh
 
mm
bad choice since she isn't in that one :P
 
@0celouvsky We've got a pilot grip guy here. The best
 
well, she's in a flashback
 
9:22 PM
@0celouvsky you're gonna pretend that flashbacks count now?
 
@EmilioPisanty I have oot right there on the screen
And a link between worlds
You have to believe me
And a link to the past!
 
OBE
@0celouvsky what note book do you use?
 
@ACuriousMind Here's the deal. By Riesz-Fisher, the dual of $L_\epsilon^2$ is indeed $L_\epsilon^2$, by the identification $T(f)=(g_T,f)=\int g_Tfe^{2\epsilon|x|}\,dx$. But if we absorb that exponential we find $\tilde g=g_Te^{2\epsilon |x|}\in L^2_{-\epsilon}$, so the dual can be viewed as $L_{-\epsilon}^2$ with the pairing given by regular integration $T(f)=\int \tilde gf\, dx$ without that factor.
@OBE a nice one
 
OBE
what's it called?
 
Hans
 
OBE
9:35 PM
oh okay.
 
the back flap says markings by CR Gibson
@Danu Lol, Drake OD'd on weed in Amsterdam
 
9:58 PM
@0celouvsky OD'ing on weed is not really a thing
 

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