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3:00 PM
Those are based on the charges which generate the electric field
 
@Semiclassical aha I see
 
If an electric field is monopolar or dipolar, that means the vector field has one or two (resp.) singularities, that's all.
 
@ACuriousMind That's not a good habit especially when others are around you, calculating.
 
Those singularities correspond to position of the test charge that generates the field
 
@lılostafa Obviously I tone it down when others are nearby
 
3:01 PM
Suppose I put a collection of positive charges near the origin. If I zoom out, I’ll just see field lines emanating from the origin
 
@Semiclassical very good. So as a sanity check for myself: when we say magnetic fields are dipolar, the field itself is still a vector-valued function of position, but the source of the field is dipolar
 
Although my former roommate once knocked on my door, asking who I was talking to. I was just tackling a particularly stubborn exercise.
 
So I can characterize the behavior far away in terms of how far away I am from the origin. All other sense of directionality gets washed out
 
@user929304 Yes
 
You can have energy without a Noether charge
 
3:03 PM
By contrast, suppose I put a positive and a negative charge near the origin and zoom out.
 
@Slereah So then it's the generator of time translation still.
 
true
well, depends on the definition I think
 
No matter how far out I go, I’ll still have a preferred direction: the line connecting the two charges
 
@JohnRennie oh so the different orders of poles can be thought of as a elementary decomposition of the field in a basis (I mean similar to vector decomposition)
 
@ACuriousMind autocorrect went insane
I said you're a mathematician
 
3:05 PM
@Semiclassical sigh... now I m losing you again.... sry
 
@0celo7 I guessed, but mttaaician is an odd thing to autocorrect to ;)
 
@user929304 Exactly. It's called a multipole expansion and is widely used in physics.
 
@ACuriousMind I thought so too.
 
it helps to draw pictures here
Namely the field lines for a positive-negative charge pair
 
@JohnRennie Great, thanks. God... self learning is not going well, so much ground to cover ( I never had formal training in physics). But I love it so will never lose my ambition of wanting to learn more about it :)
@Semiclassical it s true. For a closure, to avoid extended discussions here, let us take an example: we know magnetic fields have dipolar sources, and GW's are quadrupolar, from a physics point of view, what is the main contrasting feature between the sources of the two latter fields?
 
3:09 PM
@user929304 This is chat, extended discussions are not really a problem here (unless the participants in it tire of it)
 
well, let's simplify this a bit
let's compare the pictures for a monopole charge config, a dipole charge config, and a quadrupole charge config
that's the field of a monopole: field lines emanating from a single positive charge.
that's the field lines in the plane, anyways, but you should imagine them coming out of the page and into the page as well
 
@ACuriousMind alrighty great :) by the way I ve been meaning to ask you something about QM and information: specially in the new Q-information field, one hears a lot people saying "information is conserved". I understand they refer to the unitarity of the evolution of the whole system,
but do I understand correctly that there's no "law of conservation of information" in physics right? I mean for one thing, we have the second law of thermodynamics telling us all systems evolve in producing more information/entropy.
 
a key point here is that if i were to rotate this picture a bit, it wouldn't change. so all I need to know is how far I am from the charge, and what the strength of the charge is.
by contrast, here's the field of a pair of positive and negative charges:
 
@Semiclassical aha, makes perfect sense.
 
that's a bit different!
the positive/negative charges are at (0,1) and (0,-1) respectively
 
3:16 PM
@Semiclassical indeed, now we see a circular pattern
 
@user929304 Whenever I hear "information is conserved", I just substitute "time evolution is unitary".
 
sure. moreover, though, there's a preferred axis
no matter how far out I go, i'll always have field lines running up the y-axis
 
As for how the second law of thermodynamics is compatible with a reversible (unitary) time evolution, that's Loschmidt's paradox
 
and keep in mind that this is just a cross-section of the 3d picture
 
@ACuriousMind yes :) I do the same. How do interpret the unitary here without resorting to notions of "information"?
 
3:18 PM
if i imagine rotating my system along the y-axis, i'd find that the system wouldn't change
the positive and negative charges stay in the same place, so nothing actually changes
by contrast, if i rotate around any other axis, i definitely change where the particles are and therefore change the picture
 
@user929304 It's meant literally, in the mathematical sense of "unitary": The time evolution operator is a unitary operator on the space of states
 
@Semiclassical yes I see. so in a sense you re pinpointing the different symmetries of the generated filds
 
something like that
what that means is that, if I want to describe the field far away from the origin, I now need to know not only how far away I am and the strength of the charges involved
i also need to know what that axis of symmetry is
and that axis is characterized by a vector pointing in that direction
 
@ACuriousMind aha, so for example in the sense that: if I know the state of my system at anytime t, I know its full history and future?
 
@user929304 Yes, precisely, and from any point in the past or future, you can also know all of that
 
3:21 PM
@ACuriousMind so long as no measurements are made :)
 
@Semiclassical Sure, the measurement problem rears its ugly head :P
 
@Semiclassical that's a decoherent argument!
 
now for the quadrupole case, and this one is a doozy
to get a dipole field instead of a monopole field, I picked my charges so that they had opposite signs
hence the net charge was zero.
to create a quadrupole, I'll take two dipole configurations of equal strength but opposite direction
(there are other ways to do it, but this is a simple one)
 
@ACuriousMind and naively, why do we say that time evolution should preserve the normalisation that we have chosen for our states?
@Semiclassical nice picture, very helpful!
 
3:26 PM
@Semiclassical wait a minute, are you generating these in mathematica as we speak? :) wow
 
in this pictures, there's positive charges at (1,1) & (-1,-1) and negative charges at (1,-1) & (-1,1)
yup
the joys of StreamPlot :)
 
@Semiclassical how do you generate them so quickly?
 
experience
i know what the functions are for the vector fields as functions of position in the plane
and to get the effect of all four charges together you just add those functions together
so it's actually easier than you might expect
 
@ACuriousMind I mean, it seems that unitary "evolution" of a system, is not really an evolution, as nothing seems to be changing, as in everything's stationary
 
anyways
key point here is that we've now got this weird four-lobed creature
 
3:29 PM
@user929304 Frankly, I don't like that argument for why time evolution is unitary. The better argument, imo, is that the Schrödinger equation tells us that $U(t) = \exp(\mathrm{i}Ht)$, and if $H$ is self-adjoint (as it has to be, since the Hamiltonian is often the energy, which is an observable) then $U$ is unitary.
 
@Semiclassical ye I see, I ll try to play with these on my own in mathematica. Yes
 
@user929304 What do you mean "everything is stationary"? A superposition of stationary states with different eigenvalues is not stationary.
 
StreamPlot[q{x - h, y -k}/((x - h)^2 + (y - k)^2)^(3/2),{x,-3,3},{y,-3,3}] plots the electric field lines of a charge q at (h,k)
you'll need to pick values for q,h,k for that to run, of course
then you just take different such functions and add them together before doing streamplot
 
@ACuriousMind that s true, I meant in the sense that we say: the probability to find the state $\psi$ in $\phi$ at $t_0$ should be the same as finding the evolved state $\psi$ in the evolved state $\phi$ at $t_1$. Which then prompts one to ask: then what has changed in the system from $t_0$ to $t_1?$
 
3:31 PM
I should emphasize again that this is just a 2D cut, though
there's not a stream-plot 3D that I know of
 
@user929304 What has changed is the probability to find it in state $\phi$ (not evolved).
 
@Semiclassical sure, thanks a lot, very nice explanations.
 
(though there is VectorPlot3D)
 
If $\phi$ is the eigenstate of some observable you want to measure, that's a very significant change.
 
anyways. key point here is that there's no longer a single preferred axis
you do have the lines y=x, y=-x
 
3:32 PM
@ACuriousMind ohhhhh I see now where I was going wrong!!
 
This is the difference between the Schrödinger and Heisenberg pictures: In the Schrödinger picture, the state of the system evolves but the states we want to measure do not. In the Heisenberg picture, the state of the system doesn't change but the states we want to measure do.
 
so now if you want to characterize this system, we're not going to be successful just by knowing the charges, the distance, and a single vector
we're going to need a bit more info than that.
the information one needs is characterized by the rank-2 quadrupole tensor
 
@ACuriousMind so as to preserve overlaps (inner products), true true. Physically, what gave us the hint to expect unitary time evolution?
 
@user929304 I don't think anything gave us the hint. It just follows from the Schrödinger equation.
 
there's still a definite notion of geometry here---the orientations of the four lobes---but that geometric info isn't as simple to characterize as just "what direction does it point"
 
3:35 PM
@ACuriousMind I mean people often give arguments that, the probability of finding the electron cannot be 0, as it MUST be somewhere, right? and then we impose that \sum p_i = 1 as a normalisation (or more correctly the squared modulus being summed)
 
Are we asking why the Hamiltonian is self-adjoint again
 
why time evolution of the wavefunction should be unitary
Now I'm wondering what VectorPlot3D would say
 
@Semiclassical That follows form self-adjointness of the Hamiltonian though
I don't know the physical meaning of that
 
@user929304 Yes. But that's a silly argument because there's no obvious reason for why a non-unitary operator would necessarily mean some probability becomes 0, and the normalization argument is also silly because there's a version of the Born rule that computes the probabilities also for non-normalized states (you just divide by the norms of the states involved).
 
3:38 PM
@BalarkaSen that eigenvalues should be real? (as in measurable experimentally)
 
@user929304 Yes, exactly.
 
@user929304 There are lots of non-symmetric matrices with real eigenvalues
 
@BalarkaSen it's not always
 
@BalarkaSen The crucial condition is "measureable experimentally" - physical observables are by definition self-adjoint.
 
There are those God Awful classical things that quantize to God Awful operators
@JohnRennie Galloway wrote back...
 
3:40 PM
QM gives you no recipe for "measuring" non-Hermitian operators.
@BalarkaSen A different take on the physical meaning is "the system is closed". Open systems can have non-Hermitian Hamiltonians and therefore also non-unitary time evolution (parts of the system escape into the environment or come into it)
 
@ACuriousMind Hm. So somehow being self-adjoint relates to measurability? Should the connection be intuitively clear?
 
@JohnRennie @Slereah He doesn't know the answer :/
 
Good remark about closed systems, I tend to forget that.
 
$V(x)=2e^{ix}+e^{-2i x}$ :>
 
@0celo7 oh well, at least you know it's a genuinely hard problem.
 
3:42 PM
@BalarkaSen I don't think there's an intuition other than "It's not clear how we're supposed to measure non-self-adjoint operators".
 
@ACuriousMind I see. Interesting.
 
@ACuriousMind that said, then please please please, can I ask what we mean by closed here? (in QM) because it seems to be going back to that argument you didnt like about the electron
 
@ACuriousMind Got it.
 
@0celo7 For the strongly causal thing?
 
then $V(x)^*\neq V(x)$ for real $x$, but $V(-x)^*=V(x)$ for real $x$
 
3:42 PM
Try asking Ellis maybe?
 
@user929304 "closed" means it doesn't interact with its environment in a way that would allow something from the system to get "lost".
 
It's like water sloshing back and forth in a closed container versus what happens if the container has a hole in the bottom
 
@JohnRennie @Semiclassical and @ACuriousMind many thanks again for your time devotion and help. Really appreciate it. It's so valuable to be able to have these discussions, so glad I found out about chat SE. When do we ever get to ask physicists these kinds of questions in real life? ... never :(
 
grad student offices :)
 
I suspect this is related, but not the thermodynamical notion of closedness though?
 
3:44 PM
@Slereah ye
@Slereah He said he'll ask other people about it and now he's genuinely curious
 
@ACuriousMind right, yeah. Sorry for all these questions... I know they are extremely naive :(
 
blah, vector plot 3D is sorta useless for this purpose
 
@user929304 Don't apologize for asking!
 
I think if you want to get a 3D representation of mono/di/quadrupole one usually looks at the electric potential
 
Don't ask to ask, don't apologize for asking...too many rules!
 
3:48 PM
since then it's a scalar not a vector-valued function
 
@ACuriousMind thanks, appreciate it.
@ACuriousMind by the way, did you ever get to check the Schumacher book I told you about? Quantum Processes Systems, and Information by Benjamin Schumacher , Michael Westmoreland
 
@user929304 I'm afraid not
 
@ACuriousMind you can see the contents on amazon for example. Definitely worthy of a check out
@ACuriousMind I think safesphere is doing his/her best to provoke you to write an answer :-)
 
4:06 PM
@JohnRennie I guess the most cores a merge sort can use is 2?
God, currency is a brainfuck
 
@user929304 safesphere has, shall we say, some idiosyncratic ideas. He accuses me of posting nonsense about the Big Bang. These things are sent to try us :-)
 
@JohnRennie haha indeed :)
 
@BernardoMeurer I'm not familiar with the merge sort. Is it the one where you split the arrays into lements greater than the median and less then the median, then recurse to sort each half?
Ah, no it isn't.
@BernardoMeurer currency causes all sorts of hassle in programming. Some systems, e.g. SQL Server, have a specific currency datatype. It's usually handled as a sort of integer.
 
4:29 PM
@ACuriousMind by the way, I had a side question I forgot to ask, regarding the unitarity discussion: does the (conservation of information) unitary time evolution in any way link up to the degrees of freedom of a system? As in, in unitary time evolution, a system's degrees of freedom remain unchanged. I guess also partly related to saying the system's "closed".
 
@JohnRennie Merge sort is different
It's where you split to singletons and then orderly merge
 
4:51 PM
@Semiclassical What is the best way to aggregate large amounts of literature research?
 
@0celo7 Use Jabref?
 
@EmilioPisanty Did you get my facebook message?
 
@BernardoMeurer I did
 
@Slereah what's that?
 
A bibliography tool for Latex
 
4:57 PM
@user929304 as Semiclassical has already explained, those aren't very useful ways to understand multipolarity
there's better ways
The very easiest way to understand them (I think) is to consider charge distributions that are confined to a spherical shell
so you have $\sigma(\theta,\varphi) = \sigma(x,y,z)$
 
@Slereah I'm not writing anything yet. I have 40 papers that I need to keep straight and manage
 
@0celo7 Jabref does that
You can make a database of the papers
with tags, links, files and biblioref
And only at the end of the project, generate a tex bib page
 
in short, a charge distribution (on that shell) is $2^\ell$-polar if and only if $\sigma(x,y,z)$ is a homogeneous polynomial of degree $\ell$ in $x$, $y$ and $z$.
 
@Slereah can I attach summaries with TeX equations?
 
@0celo7 use zotero
 
5:00 PM
@0celo7 i don't recall
 
@EmilioPisanty what is that?
 
a reference manager
 
@EmilioPisanty dead link
 
@EmilioPisanty Did it tickle you and make you giggle?
 
5:03 PM
@EmilioPisanty 🙇🏻
 
similar to Mendeley but without the evil
 
That's a worshipping man
@EmilioPisanty evil?
 
@0celo7 Halp
 
Mendeley is part of Elsevier, has been for about half its lifetime
 
5:05 PM
@EmilioPisanty I own 3 Elsevier books. Am I part of the problem?
 
but I hate elsevier!
 
@EmilioPisanty It's a shame it's not pointed out more often that spherical harmonics are just these polynomials.
 
@0celo7 did you explicitly choose those books over functional equivalents because they were Elsevier?
@ACuriousMind 100% agreed
 
Show that for any $n\in\Bbb N_1$ $$\frac{1}{1\cdot 3}+\frac{1}{3\cdot 5} + \cdots + \frac{1}{(2n-1)(2n+1)}=\frac{n}{(2n+1)}$$
 
@EmilioPisanty No. Reed-Simon and Adams have no equivalents.
 
5:07 PM
I forgot how to do induction proofs
 
They are standard references and will continue to be for the rest of our lives, probably.
 
@ACuriousMind the way spherical harmonics are normally taught seems explicitly designed to make people hate them
 
Anonymous
@BernardoMeurer $1=\frac{3-1}{2}$, $1=\frac{5-3}{2}$,...
 
@0celo7 that was kind of a rhetorical question
unless you did, then no, you're not part of the problem
Elsevier is
 
@user929304 Not really - the degrees of freedom of a system are fixed by what you define to be the system, but in an open system, one might say that you chose to ignore some relevant degrees of freedom (for whatever reason). Nothing to do with unitarity, though.
 
5:09 PM
@BernardoMeurer well, you just need to show that if you add the next term the sum simplifies to what it needs to
 
Anonymous
@0celo7 I've started reading the first chapter of Reed-Simon. It's nice so far. :) I got stuck a few times though in that Zorn's lemma stuff
 
Zorn's lemma is false
2
 
@EmilioPisanty it doesn't help that one of the main places you're forced to get good at using them is in graduate level electrodynamics
 
so $$\frac{n}{2n+1}+\frac{1}{(2n+1)(2n+3)} = \frac{n+1}{2n+3}$$
 
which means you're probably going to be using Jackson :P
 
5:10 PM
It depends on evil AC
 
@EmilioPisanty Aaaaah, right!
I have to show for an $n$
and then show for $n+1$
 
@BernardoMeurer actually has a proof that ZFC is inconsistent
 
@BernardoMeurer no, you assume your formula for $n$, and then you use that to prove for $n+1$
 
@0celo7 That is true, ZFC is inconsistent
 
@0celo7 The traditional view-point is that the well-ordering principle is obviously false, the axiom of choice is obviously true, and no one can tell for Zorn's lemma :P
3
 
5:12 PM
that's a fun joke
though my favorite mathematical 'joke' is the following test for whether you're a mathematician or a physicist
 
@ACuriousMind they're equivalent so by basic logic Zorn is false
 
"If $f(x,y)=x^2+y^2$, then $f(r,\theta)=$?"
 
@ACuriousMind aha I see. But isn't for instance the number d.o.f's connected to the dimension of Hilbert space in which our system's state is unitarily evolving?
 
AoC is BS
 
@user929304 Yes, the number of d.o.f. is the dimension of the space of states.
@0celo7 That's the joke :/
 
5:13 PM
@ACuriousMind ok, and isn't the that dimension also preserved by unitary evolution?
 
@ACuriousMind You don't think I know that?
I know the joke, said it many times myself
 
You're the one who insisted on explaining it :P
 
I wasn't trying to explain
I was a bit miffed that ACM tried to joke about a serious issue. @Blue needs to know that many people disregard Zorn
All reasonable people do
 
riiight
 
@user929304 I'm not sure what you mean by "preserving" the dimension.
 
5:17 PM
@ACuriousMind ah, just that the space of states cannot shrink or expand
 
If you mean that it's bijective, i.e. the image is still the entire space, then yes, that's implied by unitarity.
 
"Sov. Math. Dokl."
Crap.
That's not going to be in a language I understand.
 
@0celo7 so, you're OK with the statement "for every vector space $V$ over a field $F$, $V^*=\{f:V\to F : f\text{ is linear}\}$ has at least one nonzero element" being false?
 
@ACuriousMind exactly
 
@user929304 The space cannot shrink or expand simply because there's no way for it to do so in the formalism. The space of states is fixed, always, before we even talk about time evolution
 
5:18 PM
@EmilioPisanty We've discussed AC to death in this room
 
@0celo7 but are you OK with that?
 
@0celo7 actually, Doklady usually has English translations
 
I don't LIKE any of the weird shit you get without AC
But I refuse to believe well ordering
 
not always easy to find online, but your math library likely has them in their collected periodicals
 
@ACuriousMind Did you like my DRM essay? :P
@dmckee Are you around?
 
5:19 PM
@0celo7 you might be surprised. I was hunting a Danish paper the other day and it turned out to be in German
 
@EmilioPisanty I also don't claim to understand infinity and if you do I think there's an issue
Cantor went insane because of this shit
 
I understand infinity.
 
@0celo7 I'll cop to not understanding infinity but I'll keep that fact under the rug if you don't mind
 
@0celo7 Cantor was born insane
@ACuriousMind You're not human
 
@ACuriousMind thanks, understood.
 
5:20 PM
@ACuriousMind Are you parodying a certain Duffield?
 
@0celo7 No, just playing the contrarian to you :P
 
Anonymous
@0celo7 Proof? :P
 
mary mary quite contrary
 
@Semiclassical The physicist replies "$r^2$" while the mathematician complains about undefined and overloaded symbols?
 
@ACuriousMind and we thought 0celo7 was in a joke-explaining mood
 
5:22 PM
well, or the mathematician insists that $f(r,\theta)=r^2+\theta^2$
 
I'm not. I'm srs
@Semiclassical Hey! Don't I get any credit here?
 
@Semiclassical Ah, heh
 
I agreed with you!
 
heh
yeah, and I do appreciate that
i mean, I can understand the objection: $f(r,\theta)=r^2$ is not sensible if we insist on $f$ as a mapping from $\mathbb{R}\times \mathbb{R}\to \mathbb{R}$
but if we're talking about an experiment, what matters (for instance) is what electric potential would find at each point in space.
the particular coordinate system we use to represent that relation really does not.
and insisting that one nevertheless use different symbols to denote the same output is in that respect just silly
blah blah blah
 
@Semiclassical just come up with a name for the function that takes polars to rectangular and then precompose
That's mathematically correct
 
5:34 PM
yeah.
this is one place where I really do like bra-ket notation, namely being able to write $\langle x|\psi\rangle =\psi(x)$ with $|\psi\rangle$ being the fundamental object
 
anyone ever seen a zebra centaur?
 
that looks like something out a SCP story
 
@Semiclassical Now that I vehemently object to.
 
Bra-ket notation is NOT fundamental, it's a mnemonic system.
 
5:36 PM
meh
 
@0celo7 depolar
 
my point is that notationally it treats $|\psi\rangle$ as more basic than $\langle x | \psi\rangle$
 
@Semiclassical so does $f$ and $f(x)$
(just saying)
 
hmm
i suppose the comparison is that no physicist would expect that $\langle x|\psi\rangle = \sin x\implies \langle p|\psi\rangle =\sin p$
and moreover that the rule for how the latter is obtained from the former is 'suggested' by the notation itself: $\langle p |\psi\rangle = \int \langle p | x\rangle\langle x|\psi\rangle \,dx$
but I think that reflects how comfortable I am with $\int |x\rangle\langle x|\,dx=\mathbf{1}$
 
mnemonic means what?
 
5:42 PM
memory
 
@Semiclassical and you have to do a lot of analysis to make sense of that. If you do QM like in Reed and Simon, you never need it though
 
I sorta object to it being called just a mnemonic system, but I'm not sure what else to call it
 
Rigged Hilbert spaces are for people with strong emotional attachment to bra-ket notation
You can (and should) learn how everything works without it
 
lol
tbh I largely agree with that
 
The best solution is as usual to like both notations and be able to switch immediately.
 
5:44 PM
i feel like, for instance, one could do QM just as well by a form of index notation
 
That's true, but I think it's immoral
 
pff
and actually I take that back a little. when one is doing finite dimensional Hilbert space stuff, then all that's happening is ultimately just matrices/row vectors/column vectors
in that context, index notation would make sense.
but when you're working with position and momentum representations, that doesn't make a lot of sense.
 
@ACuriousMind Love it. These kinds of "oh, well all know the notational conventions so I don't have to say what I mean" things are (a) really bloody convenient and (b) a potential source of vast confusion.
 
ugh. Maxwell keeps spamming MSE chat with the same Schrodinger equation problem
@dmckee my own reaction the first time I saw it was that it was ambiguous
 
And L^2 of a finite set is just R^n. Everything is better with functional analysis.
 
5:48 PM
which isn't quite right. the point is that it depends on context
being able to recognize that notation is ultimately a matter of conventions---and, therefore, context---is to me a pretty important research skill
 
@Semiclassical It is. And it is one that becomes so ingrained that when you return to the classroom as a teacher it is easy to forget that beginning students don't have it yet.
That lack of understanding caused some trouble with my first few upper-division tests.
 
yeah.
i can understand an insistence avoiding such conventions in that context.
i just think that getting upset at them in practical use is silly.
 
6:10 PM
@Semiclassical what triggered you again?
 
someone else indicating that such notation was garbage and to use it was to spew crap
 
6:57 PM
@BalarkaSen My advisor just sent me a Gromov paper. I'm scared
 
7:11 PM
@0celo7 Is this the new paper
 
@BalarkaSen there's a new new paper
 
oh?
 
@BalarkaSen on psc conjectures
@BalarkaSen I'm already doing one presentation on psc in the spring, I bet he thinks I want to do another
problem is it's all ggt/mg or kt
 
7:27 PM
psc?
 
lol, the title of this paper:
it includes the word 'isogaloisian' which is fun
 
@EmilioPisanty I'm gonna waste hours sorting papers in this damn app
@EmilioPisanty this isn't exactly user-friendly
@EmilioPisanty So I found the place for summaries, can I not put TeX there?
 
8:03 PM
Hi guys
I see quite a few textbooks and websites saying that "beta decay needs to be explained by the weak nuclear force"
But I don't understand why the weak nuclear force is needed for beta decay
I would be immensely grateful if anybody could explain this to me
 
Anonymous
6
Q: The role of W bosons in the weak nuclear force and beta decay

daljit97I am a beginner Physics student and I am studying the weak nuclear force and how particle interactions work. Now, from my book and the Feynman diagram, I learned that a neutron can change into a proton when it interacts with a neutrino, this happens because W$^-$ bosons are exchanged between $\nu...

 
Anonymous
16
Q: Weak contribution to nuclear binding

SimonDoes the weak nuclear force play a role (positive or negative) in nuclear binding? Normally you only see discussions about weak decay and flavour changing physics, but is there a contribution to nuclear binding when a proton and neutron exchange a $W^\pm$ and thus exchange places? Or do $Z$ exch...

 
@Blue Ok, thank you for the links
 
8:32 PM
@EmilioPisanty Am I mistaken or is there no option for subfolders? Because that's a deal breaker for me.
 
8:48 PM
wtf it wasn't there a few minutes ago
found it
@BalarkaSen I was made fun of in the topology seminar for being a physicist
 
Anonymous
@0celo7 wut
 
Anonymous
Since when are you a physicist?
 
I was reading about conformal structures in spacetimes
that makes me a geometer, not a physicist
 
Anonymous
@0celo7 Ya. Lol
 
Anonymous
You should have countered with the GDP argument though
 
9:00 PM
@EmilioPisanty Wow the free storage size is tiny!
 
9:12 PM
@Semiclassical pch $r^2 + \theta^2$ be gone...
I've never seen something so unlikeable (in math)
$dr^2 + r^2 d \theta^2$ for $r = 1$ however...
Isogalosian makes up for it
 
9:27 PM
What is an ellipse with big eccentricity factor called?
 
Anonymous
degenerate ellipse
 
Not that big
 
Anonymous
@lılostafa I've never heard of a term for that. What's the context anyway?
 
I remember they call ellipses like the rightmost one here with some specific term....:
Those that deviate a lot from a circle (but still not a line)
 
Anonymous
No idea
 
9:35 PM
I think I can just say a very eccentric ellipse
@Blue The context is optics. I want to refer to elliptical polarizations that are very close to a linear polarization (but still elliptical)
 
Anonymous
Invent your own term for that and put it in your thesis. It might just become popular. :P
 
9:51 PM
Good suggestion :)
 
 
1 hour later…
11:08 PM
@0celo7 they're not folders, they're collections
 
Yeah I figured that out
@EmilioPisanty please be a fortran god
 
And yeah, you can make sub-collections
@0celo7 yer barkin up the wrong tree
 
Ask @JohnRennie, he's an old man!
He probably knows Fortran
 
If it's fortran then you probs want @KyleKanos
 
he hasn't used it since I've been alive
@EmilioPisanty he's not pingable
 
11:10 PM
What FORTRAN do you need, anyway
 
Step size in x, <0.0001,1>, negative to exit:
Step Size: 0.600000 Numerical Result: -3.13600 An. Res.: -1.6667 Err[%]: 88.16000

Step size in x, <0.0001,1>, negative to exit:
Step Size: 0.100000 Numerical Result: -1.96000 An. Res.: -1.6667 Err[%]: 17.60000

Step size in x, <0.0001,1>, negative to exit:
Step Size: 0.010000 Numerical Result: -1.68660 An. Res.: -1.6667 Err[%]: 1.19600

Step size in x, <0.0001,1>, negative to exit:
oh dang
this doesn't display whitespace, damn
I can't figure out how they arranged the whitespace
the whitespace on the 1.19600 is messed up
 
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