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7:40 AM
morgen
 
@EmilioPisanty it looks as if there might be hope after all. Bojo the clown just got a bloody nose in parliament!
 
$$S[\Phi(\vec{x}(t))] = \int_{\alpha(t_a)}^{\alpha(t_b)} (\frac{ds}{dt} \frac{d}{dt}\vec{f}(\vec{x}(\alpha^{-1}(s)), \alpha^{-1}(s)) \cdot (\frac{ds}{dt} \frac{d}{ds}\vec{f}(\vec{x}(\alpha^{-1}(s)), \alpha^{-1}(s))) \frac{dt}{ds} ds$$
plz kill me
I am in a hell of my own making
Now to show that this contains the Galilean group
gonna be a bit tough
With just $f$ or just $\alpha$ it's alright, but both at the same times
Who knows what kind of weird transformations could occur that I have to rule out
All the FORBIDDEN SYMMETRIES
Forbidden by the Coleman-Mandula theorem
Hm
I have to deal with something like $$\int \left[ f(x) g(x) + h(x) \right] dx = \int f(x) dx$$
If this is true for all $f$, does this imply $h(x) = 0$?
Not quite the fundamental lemma of the calculus of variation
@ACuriousMind @bolbteppa halp
I'm 99% sure this is true but as usual
Never trust an obvious statement
 
8:35 AM
Oh wait
Obviously not for $h$
Can just be a function that integrate to $0$ on that range
BUT IS IT TRUE IF THE EQUALITY IS TRUE FOR EVERY DOMAIN OF INTEGRATION
 
9:25 AM
Can be rewritten as $\int f(x)[g(x) - 1]dx = - \int h(x) dx$
 
Does this help
 
In mathematics, specifically in the calculus of variations, a variation δf of a function f can be concentrated on an arbitrarily small interval, but not a single point. Accordingly, the necessary condition of extremum (functional derivative equal zero) appears in a weak formulation (variational form) integrated with an arbitrary function δf. The fundamental lemma of the calculus of variations is typically used to transform this weak formulation into the strong formulation (differential equation), free of the integration with arbitrary function. The proof usually exploits the possibility to choose...
Version for 2 functions
Maybe you can write it in this way
 
Second part doesn't depend on $f$ tho
 
$\int \{ f(x)[g(x) - 1] + h(x)g'(x) \} dx = 0$
hmm
 
I need to work out the full integral of this rly
it is an unpleasant one but it shouldn't be too hard
 
9:34 AM
@JohnRennie counting chickens?
I mean, it's good and all
But not enough on its own, yet
 
@EmilioPisanty yes, it could still go in lots of different ways. BoJo wants to call a general election, but that needs to be agreed by parliament and the opposition have said they'll vote against it.
Plus as I understand it the motion was to ask for another three month extension in the event of no deal being approved, but the EU may not agree to another extension on the grounds nothing will change in three months.
But it's still good to see that mendacious scumbag get a kicking :-)
 
9:50 AM
BoJo's bizarre adventures
 
Bizarre is exactly the word I'd use. Possibly also incredible in the literal meaning of the word.
 
If I'm not fucking up, the final transformed action is something along the lines of $$S[\Phi(x)] = \int_{\Phi(t_a)}^{\Phi(t_b)} \dot{\alpha}(\alpha^{-1}(s)) \left[ (f'(x, s))^2 \dot{x}^2 + 2 \dot{x} f'(x, s) \dot{f}(x, s) + \dot{f}^2(x,s) \right] ds$$
And the end result should be $$\int_{\Phi(t_a)}^{\Phi(t_b)} \dot{\alpha}(\alpha^{-1}(s)) \left[ (f'(x, s))^2 \dot{x}^2 + 2 \dot{x} f'(x, s) \dot{f}(x, s) + \dot{f}^2(x,s) \right] ds = \int_{\Phi(t_a)}^{\Phi(t_b)} \dot{x}^2 ds $$
Obviously this works all fine for $f'$ a Galilean transformation and $\alpha$ a time translation
But showing that these are the unique transformations seems tricky
Wait is it even correct for a Galilean transformation
\begin{eqnarray}
f(x(s), s) &=& \pm x(s) + vs + a\\
\dot{f}(x(s), s) &=& v\\
f'(x(s), s) &=& \pm 1
\end{eqnarray}
Hm
I guess the terms don't cancel out but they are total derivatives?
and therefore bla bla bla
 
10:52 AM
@JohnRennie so the opposition's plan is a vote of no confidence but only if it doesn't lead to an election?
That's bonkers
@JohnRennie it's three months? Yeah, good luck with that =/
 
@EmilioPisanty It's because the fear is that BoJo will drag the election out to leave not enough time to sort out what to do before the Oct 31st deadline.
 
It's still not enough time
 
An election could easily mean Parliament was dissolved for a month.
 
And the result could well be a strong mandate for a second referendum
@Slereah I think I like de Pfeffel better than BoJo
 
I wonder where on earth the negative sign in the third step comes from?!. The anticommnutation relations implies a positive sign since we have pair anticommutations
$\begin{aligned} C \overline{\psi} \psi C &=\left(-i \gamma^{0} \gamma^{2} \psi\right)^{T}\left(-i \overline{\psi} \gamma^{0} \gamma^{2}\right)^{T}=-\gamma_{a b}^{0} \gamma_{b c}^{2} \psi_{c} \overline{\psi}_{d} \gamma_{d e}^{0} \gamma_{e a}^{2} \\ &=+\overline{\psi}_{d} \gamma_{d e}^{0} \gamma_{e a}^{2} \gamma_{a b}^{0} \gamma_{b c}^{2} \psi_{c}=-\overline{\psi} \gamma^{2} \gamma^{0} \gamma^{0} \gamma^{2} \psi \\ &=+\overline{\psi} \psi \end{aligned}$
 
10:58 AM
Brexit: raising the bar on knuckle whiteness since 2016
 
@EmilioPisanty the thing is that there is simply no acceptable deal. The land border between Northern Ireland and Ireland makes that impossible.
The EU will not consider any deal that doesn't allow free traffic across the Irish border. End of story.
And that's unacceptable to the Ulster Unionists because then there would have to be a traffic control between Northern Ireland and the mainland.
In effect it would be a step (a large step!) towards the reunification of Ireland.
 
11:43 AM
Is space times time info entropy?
 
12:30 PM
Is Nick Bostrom's simulation hypothesis on topic, or do we VTC as non-mainstream? physics.stackexchange.com/questions/500176/…
 
I'm tempted to VTC that one as unclear or something. It's not clear to me what types of differences they expect
 
Whether mainstream or not doesn't matter much
it's not a physical hypothesis
more of a philosophy stack exchange question
 
@JMac Sure, but there's a possibility of the OP clarifying that. Whereas if it is off-topic, then no amount of clarification or other editing will help.
@Slereah I tend to agree. OTOH, you could say the same about most questions asking about the various interpretations of QM. ;)
 
0
Q: Robust ways to find zeros of the Tricomi confluent hypergeometric function as a function of its parameters

Emilio PisantyI'm solving a quantum mechanical problem, and the quantization condition requires me to solve the equation $$ U\left(\frac12(\ell+1-E), \ell+1, r^2\right) = 0, $$ where $U(a,b,z)$ is the confluent hypergeometric function of the second kind, $r>0$ is a fixed positive real number, and $\ell\geq0$ i...

@Semiclassical any insights appreciated =)
 
@PM2Ring Right, but if I can't even really understand if question relates to physics, it's hard to actually say it is off topic, and not just a poorly worded physics question.
 
12:42 PM
The last time I was here I had some funky Bessel function combinations and this package saved me. I'm afraid that with this one I won't be quite as lucky.
 
This is the step I missed,

$\begin{aligned} C \overline{\psi} \psi C &=\left(-i \gamma^{0} \gamma^{2} \psi\right)^{T}_{ab}\left(-i \overline{\psi} \gamma^{0} \gamma^{2}\right)^{T}_{bc} \\ &= \left(-i \gamma^{0} \gamma^{2} \psi\right)_{ba}\left(-i \overline{\psi} \gamma^{0} \gamma^{2}\right)_{cb} \end{aligned}$
and the fact that only gamma's with "same index" anticommutes
 
@EmilioPisanty This is way out of my league, but I suspect that if Mathematica can't handle it, things may be grim. Does it help if you use more precision? In Python, I use mpmath for arbitrary precision maths. It's got some good root solvers, and it supplies a bunch of hypergeometric functions. mpmath.org/doc/current/functions/hypergeometric.html
 
@PM2Ring Get rid of them too
I don't mind
At least interpretations of QM usually come with some physical theory behind it
This is has no possible prediction
 
12:58 PM
@EmilioPisanty yikes
Though, I think the usual clever thing to do for finding roots is the argument principle
 
the function is real-valued though
 
Sure, but that just means you draw a contour which wraps around the real line
It may be real on the real line, but it’s presumably not if you analytically continue it
 
@Slereah not sure what you're trying to do
 
the most basic question for me, though, is what exactly is causing things to go haywire
 
@bolbteppa regarding what
 
1:12 PM
as in, what feature of U(a,b,z) is making mathematica unhappy in that parameter range
 
@Slereah this stuff
(and in life? :p)
 
@bolbteppa Trying to find the most general symmetry group of the action
Although I think I fucked up the reparametrization
Not sure
From taking small bits at a time, I'm pretty sure it's the Galilean group
But it's hard to actually prove it
 
@EmilioPisanty hmm, take a look at this (with $\ell=0$, $r=10$, $x=(E-1)/2$): wolframalpha.com/input/…
something is clearly going haywire there
 
it's just big
look at it in log scale
 
big and oscillatory i guess
 
1:19 PM
If the charge conjugation is defined as
$Ca_pC = b_p ; Cb_pC = a_p$

How to prove that $\overline{\psi} \gamma^{0} \psi$ substracts the infinite constant
that appears from anticommutation relations of creation and annihilation operators?
 
my point is more that if mathematica is struggling to plot it out there, it's probably also struggling to find the roots out there
but I'm not including the 1/Gamma(1-a) factor you had
lemme see what happens then
that's better for a up to 75 or so, but mathematica struggles beyond that
 
@Slereah in Landau they say that Galileo is the most general "additive" symmetry group (I assume this means linear), but no comment on non-linear and I highly doubt they are not in there!
@Student404Mus what page of P&S
 
@bolbteppa p71
 
my impulse would be to find some identity which relates U(-a,n,z) at large a,z to U at smaller values
 
I could not understand which expression we take to conclude such a result
 
1:32 PM
Kummer's transformation seems like it might be particularly useful, if rearranged as follows:
 
@bolbteppa Well if you consider specific nonlinear symmetries, it seems to still be Galilean
But I don't know if like
 
$$\frac{1}{\Gamma(b-a)}U(a,b,z) = \frac{e^{\pm a \pi i}}{\Gamma(b)}M(a,b,z)-\frac{e^{\pm b \pi i}}{\Gamma(b)}U(b-a,b,e^{\pm i \pi}z)$$
 
nonlinear spatial transformation + nonlinear reparametrization could be a symmetry
Seems tough to prove
 
What it means is that charge conjugation sends $\psi$ into $\overline{\psi}$ (i.e. interchanges particles and anti-particles) but in bilinears it does not interchange the order of creation and annihilation operators, so it wont force you to correct any expressions using anti-commutators the way you do around 3.113 when you get that infinite constant. What it then says is that if you defined your fields initially so that this constant never appeared, it will not suddenly appear
 
@bolbteppa Means if we ignored that inf. constant, it will never appear because of C. Right?
 
1:40 PM
Yeah
It's basically just a side comment that the C's are good operators
 
I see.
 
those $\pm$'s are kinda throwing me tbh
 
P&S comments sometimes are tricky
 
i guess it's because of branch cut shenanigans
oh, dangit. the second $\Gamma(b)$ in the above should've been $\Gamma(a)$
 
I don't believe nonlinear will still end up being galilean!
 
1:50 PM
@bolbteppa Any counterexample in mind?
Or just a hunch
 
I will think about it, I'm pretty sure I seen something on this ages ago
 
Do we have a canonical Q&A about gravity that's basic enough for this OP? physics.stackexchange.com/q/500170/123208 Or do we just VTC as Too Broad?
 
2:18 PM
@Slereah is the free action conformally invariant
 
2:30 PM
Do you mean like $x \to \Omega x$?
No metrics here
All classical
It's not going to be any simple symmetries, as I said
If there's any remaining symmetry, it's going to be a bad bad one
Like $x \to x'(t) = x^n(\alpha(t))$ or something
$x \to x'(t) = x^{f(t)}(\alpha(t))$
The horror
Any symmetry left has to be a combination of time dependant field symmetry and reparametrization
 
Guys, is it possible in today's time to find a domain that is not similar to any other?
I bought anastir.com and there's a website alastyr.com and I'm quite pissed :(
 
2:50 PM
@NovaliumCompany those two names seem different to me.
I think you're worrying unnecessarily.
 
3:09 PM
@JohnRennie I think I've turned it into a mania :(
I want to find the most unique, good name, that there isn't anything similar to it, but I guess it's not possible.
@JohnRennie My father's words.
I thought of a few other names but there are similars to them as well.
I've read in sites that it's important for me to be happy with the name, but I feel like I'll never be happy as long as there are similar names to mine. What do I do? :(
 
@EmilioPisanty this looks relevant but also horrible: dlmf.nist.gov/13.8#E14
in appealing to that, I have in mind: fix some $r$ and $l$ (say, $r$ in the vicinity in the zone of bad behavior and $\ell=0$) and see how $U$ varies with $E$
 
 
1 hour later…
4:33 PM
@JohnRennie (or anybody) Can you suggest some intro material on gravity for this guy? physics.stackexchange.com/questions/500170/…
 
@PM2Ring to be honest I would just answer the question ...
 
@JohnRennie But where do you start? Forget about the equilateral triangle. He doesn't understand that 2 objects attract each other.
But if you do write an answer, there's a very good chance that I'll upvote it. :)
 
@ACuriousMind did you have a chance to check if VS2019 has that code search feature built in?
 
4:49 PM
@enumaris I realized I only have the option to get it but that it'd still cost my cost center additional money, so no, sorry :/
 
@enumaris I cannot find it. Where should I look?
 
Ah...
@Loong it would be like part of the intellisense tab that opens up
there would be a normal intellisense autocomplete, and also a tab for bing code search "how do I..." something like that...
@ACuriousMind no worries :)
 
5:37 PM
@Semiclassical that's for $a\to \infty$, though
I'm already using asymptotics from that limit
they work for the higher eigenvalues, but they're brittle for the first few eigenvalues of each configuration.
 
5:52 PM
@Loong What is up with SE lately? Seems like a consistent streak of questionable decisions
3
 
Lately? Since about April 2018
 
Well that's still rather recently
 
@enumaris makes sense. I do think mathematica is running into trouble because its numerics are not able to properly approximate HypergeometricU in that regime due to it being oscillatory with growing amplitude
Dividing by 1/Gamma should tame that, but it doesn’t seem to work
i nevertheless think that’s the right thing to do. It just may be necessary to do some more massaging to get that ratio in a form which Mathematica is numerically comfortable with
Hence why I was looking at some of the transformation properties. But finding info about U(a,b,z) for integer b is remarkably annoying
 
I've talked to some guys on an entrepreneur forum and I'm proud to say that I've settled on Anastir. I really shouldn't put so much time and energy on the name, when I actually have a unique, easy to write, easy to say and not-taken one.
 
Is this theory renormalizable?

$\displaystyle {\mathcal {L}}= \alpha{\bar {\psi }} \psi$
P&S said that self-interacting fields are not Lorentz-invariant such as $\psi^3$ but what I have written is Lorentz-invariant
taking into account $\alpha$ has one-mass dimension
 
6:09 PM
@Semiclassical sorry, I'm not following exactly...which message of mine were you replying to?
 
Oops. Should’ve been to @EmilioPisanty
 
@Student404Mus that's part of the Dirac action
Adding that would simply change the value of the mass
 
XD
 
6:58 PM
@Slereah definitely would like to see a theorem or discussion about this point tbh
 
7:25 PM
@JohnRennie I bought coin holders and put water with NaOH and TiO2 particles but the particles seem to stick to the container and I can't see what's going on. What do I do?
I think I should put less TiO2 particles?
 
7:42 PM
Also the water with NaOH concentration hasn't been changed for about a month and a half. Is that a problem?
Yep, I'm pretty sure I've put too much TiO2 particles.
But bedtime now.
 
8:05 PM
@Semiclassical that sounds overcomplicated to me
The function is mostly well behaved
It looks mostly like a matter of finding good seeds for the root finder
 
8:21 PM
eh. it may be well-behaved, but I'm not sure mathematica knows that. I'm judging that based on WA results, tho, which may be misleading
even if it is, though, some analytical massaging may make choosing those seeds easier
 
 
2 hours later…
10:38 PM
@JohnRennie How can I test for a magnetic field storing another magnetic field in the form of a magnetic field inside itself? I am wanting to carry out an experiment to test for that.
 
11:00 PM
This question originates from physics but i'm not sure if it belongs here or on math.stackexchange: physics.stackexchange.com/questions/500262/…
thoughts?
 

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