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12:41 AM
Last night dream, somewhere in a dark coloured theme version of h bar, couple of people are discussing about an esoteric theory called flow string theory. A cutscene showed an animation consists of circular objects being guided towards some kind of ring attractor and following trajectories in the process
I then argued about how I dislike them using the word "quantum" in anything that is not even physics. Another user who is some kind of astroparticle physicists then pointed out that the trajectories are way too precise than those allowed by quantum mechanics, even if we assume each circular object and their vibrations give rise to elementary particles and their interactions
i added onto this point that the closest physical analogue to this esoteric model is bohemian trajectories (which is called quantum bom theory in the dream) but even those are probabilistic and not that precise
One of the spiral trajectories which is said to have a slope of a transcendental number, which is way too precise for the model to be a physical theory
Reality check: In the dream, Flow String Theory postulates that every field and particle is generated by both the vibrational modes of the individual strings and the trajectories they are being guided on as well the ring attractors they are guided to. Whether the real life counterpart of string theory and M theory can exhibit such complicated fluid like turbulence I don't know
 
 
5 hours later…
5:48 AM
@SirCumference when you open Word it briefly displays a banner that tells you what version it is
 
6:23 AM
@JohnRennie Guess it doesn't on mac :/
thanks for trying tho
 
Ah, the Mac version. I don't have a Mac to hand to test it on I'm afraid.
@SirCumference use the system information?
If you look in the Software section I think it should show the version of the apps.
 
@JohnRennie Not sure why it seems harder to find the software version on word than most other software
But granted it still looks the same, I probably redownloaded the 2016 version. Weird but kind of expected since I clicked "get the latest Office" only 2 weeks after it was released
 
@SirCumference does this help?
 
@JohnRennie "the version number is 16.18 and the license is a one-time purchase of Office 2019 for Mac."
Huh, that matches what I have. But I'd assumed "16.18" meant "Office 2016"
not to mention the lack of design changes, weird
 
16.18 is Office 2019/365 ...
 
6:35 AM
Welp guess I'm updated
thanks for the help btw
 
7:00 AM
@Johnrennie are you around.
 
 
4 hours later…
11:20 AM
hey
3
 
 
4 hours later…
2:55 PM
@Slereah hey
 
Gotta write a personal statement for that Cambridge PhD
 
Just talk about how you want to flee the EU :P
 
God save the Queen!
I'm trying to convey my enthusiasm for the field without coming off as deranged
 
3:26 PM
"There are certain things best left out of personal statements. For example, references to experiences or accomplishments in high school or earlier are generally not a good idea. Don't mention potentially controversial subjects (for example, controversial religious or political issues)."
I'd better not say that 9/11 was an inside job
 
Well...if your prospective supervisor agrees, you'll instantly have the job :P
 
4:17 PM
How can I show that the following equations are mathematically consistent $\cosh \alpha = \gamma,\space \sinh \alpha = \gamma\frac{v}{c}$
 
@Yashas Hyperbolic identity
 
Those were guesses but there I have assigned values to $/coshh$ and $/sinh$ (i.e. did not get one from the other). I need to show that these definitions are mathematically consistent.
 
$\cosh^2 - \sinh^2 = 1$
Or whatever
 
@Slereah Is that sufficient to claim that it's mathematically consistent?
 
You can look up what $\sinh(\arccosh ())$ is, if there's such an identity otherwise
Also better tip : go to exponential forms
Things are usually simpler
 
4:20 PM
Hmm, wait. I think I could've simply got $\cosh$ using $\sinh$ from that identity. Silly me.
 
@ACuriousMind Hi, where can I look up the chat rules?
 
There are no rules
it's a wild wasteland
 
"In above question show that the Lorentz transformation corresponds to a rotation through an angle $i\alpha$ in a four-dimensional space."
 
4:25 PM
I am not comfortable with hyperbolic functions. Where do I start?
 
@Yashas convert to exponentials
it should be easy to see then
 
4:42 PM
Suppose that a particle with energy E and impulse p is decaying into 2 photons. Is it possible to determine the minimal angle between 2 photons?
 
@JohnRennie I need your stiff british upper lip
From Fewster regarding funding :
"I suggest you write that you would hope to obtain a Departmental studentship; if you know of other funding opportunities [e.g. scholarships from France] that you could apply for then you could also list them."
"Departmentla studentship" isn't a listed choice on the application, though
 
Departmental studentship presumably means the university provides the funding ...
 
yeah but I have to pick an option from a big ass list on the application
 
It's hard to comment without seeing the application form and the options available.
 
not sure which one to pick
Lemme get it
Sorry I meant big arse list
 
4:49 PM
Your English is improving already :-)
 
I appear to have understood hyperbolic rotations in 2D. How do I extend this to 4D? I have managed to show that with the way I defined $\sinh$ and $\cosh$, it corresponds to a Lorentz transformation in a hyperbola defined by $1 = x^2 - (ct)^2$. How do I extend this to 4D?
 
@Yashas In 4D you can always rotate your axes so that the rotation is in the t,x plane, so the proof for 2D is all you need.
 
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Do I just pick "Other" and write what he said
 
Ah, I just realized the question asked me to prove by a rotation by $i\alpha$ and not $\alpha$ which I think is for Euclidean space since the minus disappears off the time component?
 
@Slereah I can't see anything that's a match. I think you're going to have to choose "other"
 
4:52 PM
Alright thanks
 
Oh my. The hyperbolic ones get converted to regular trig functions and it works for 2D!
I learn more mathematics solving physics assignments than math assignments 0o
 
Hi
 
Are rotations always in a plane?
 
I was wondering how diffusion current hapeens in semi conductors?
Does that happen the moment we put two parts together?
I know that happens when the carrier density is uneven and carriers are not uniformly spread, but what causes that form of uneven spreading?
 
5:29 PM
So who are the crazy people starring my "hey"
 
So the canonical example of an adiabatic invariant is allowing $\omega$ in the Harmonic oscillator Lagrangian $L = mv^2/2 + m\omega^2 x^2/2$ vary slowly during a time period $T$ ($d \omega/dt << \omega/T$)
It's just a small step from this to superintegrable systems, gateway math :o
 
vzn
5:57 PM
@bolbteppa lol rats missed all the tumultuous energy fun yesterday wrt hossenfelder, really wanted to say something at the time :( fyi there is not exactly a cabal or conspiracy but there is something called groupthink among scientists, studied in psychology/ sociology, and its hossenfelders main point! & history tells us scientists are not immune ... hossenfelder is really much like woit/ smolin who criticized string theory over a decade ago, not really a new story....
 
@parvin fun fact, one of the profs at my uni is a superintegrability guy
 
vzn
@Secret lol bohemian mechanics luv it! :P =D (that wasnt a typo was it?)
 
@vzn it's just lukewarm iconoclasm
The Lisi comments section is Hilarious, the guy who wrote the paper destroying his paper back then was commenting
 
vzn
@bolbteppa lol its grade A iconoclasm face it. you just cant stand iconoclasm of any type, youre highly allergic... have you looked at hossenfelders credentials? ok she does sound shrill and burned out lately! "siren", lol! was also thinking femme fatale :P
 
@parvin oops, that was supposed to be a reply to bolbteppa
 
6:04 PM
@Semiclassical ah, this stuff seems to get pretty nuts fast alright
 
Apparently there's an analogue of the LRL vector for the Harmonic oscillator and it's a tensor because of this stuff (Goldstein comment)
 
I never got into the subject myself
 
@vzn words like shrill are another example of yesterday's issue, you know the dealio
I'm now wondering whether the whole $SO(4)$ hydrogen atom stuff is a false way to look at it, seems like degeneracy and superintegrability are the answer, maybe they are related not sure
 
As regards the subject at hand, I’m cynical about string theory, but I’m also cynical about most of the supposed alternatives
i find it hard to take Lisi very seriously for instance
 
vzn
@Semiclassical honestly not a lisi fan either but think his "heart is in the right place™"... fluid dynamics paradigm still needs a few yrs to catch on it seems :)
 
Search 'Dist' and just bathe in it
'I am shocked that you have still not understood this after more than a decade.'
 
@bolbteppa ?
Oh
 
Hi @JohnRennie , can you please take a look at this question ?? physics.stackexchange.com/questions/442562/…
 
The Distler comments seem to be the end of his latest ideas too, seems like Lisi really has no idea what's going on
 
6:19 PM
Alright, this has gone on long enough. Everyone stop insulting people. To be clear: This includes, but is not limited to, statements questioning an author's mental health.
5 messages deleted
 
It's amazing how people seem to go for decades in physics getting basic things wrong and don't respond to hints at trying to correct things, in this case he seems to be trying to fix his false intuition on $E_8$ by finding a way to 'deal' with mirror matter and seems to not realize how it's all linked to real, pseudoreal and complex reps and even seems to admit in his post he misunderstood the paper he thinks answers everything
9
A: Why do we need complex representations in Grand Unified Theories?

Edward HughesThis can be explained by thinking about the coupling of fermions to the $SU(2)$ weak gauge field. Let's recap what we know Weyl fermions necessarily appear in two complex representations of the Lorentz group $L$ and $R$. Only fermions in the $L$ representation of the Lorentz group couple to the...

Seems to be related to the issues described here
'You have spent more than a decade attempting to start with fermions in a real representation of the gauge group, wave a magic wand, and end up with fermions in a complex representation.'
 
What does rotation by an imaginary angle mean?
 
6:35 PM
@Yashas context?
 
@Semiclassical Lorentz transform
 
I had expressed the Lorentz transform as a hyperbolic rotation with real angles. When I tried to express it as a Euclidian rotation, I had to rotate by an imaginary angle.
 
but one of my axis is $-ict$ but I can't relate it to angles being imaginary
 
From $ds^2 = - dt^2 + dx^2$ if you set $t = i t$ this becomes $ds^2 = dt^2 + dx^2$ and you can derive Lorentz transformations using rotations instead of hyperbolic rotations
 
6:37 PM
$t=it\implies 1=i$ ? :P
(I know what you meant)
 
haha
tilde...
 
@bolbteppa but what does it mean to rotate by an imaginary angle?
 
We need the primes separate
I don't think you're rotating by an imaginary angle here
 
I rotated by $i\alpha$ to derive the Lorentz transform with $\sinh$ and $\cosh$ as parameters
Well, I eventually used $i\sinh \alpha = \sin i\alpha$
I am actually not sure what I just did
I ended up with the expressions derived using hyperbolic rotations by using regular rotations except that I multiplied the angle $\alpha$ (the angle that would be used in hyperbolic rotation) by $i$ and used it in the regular rotation
 
If $\cos(x) = \frac{e^{ix} + e^{-ix}}{2}$ and $\cosh(x) = \frac{e^x + e^{-x}}{2}$ then setting $ix = y$ we see $\cosh(y) = \cosh(ix) = \cos(x)$
 
6:42 PM
\
 
So rotating a trigonometric function with an imaginary angle is equivalent to a hyperbolic rotation, $\cos(ix) = \cosh(x)$
I think that's what's going on
 
Anonymous
See the last paragraph
 
Yeah you just show that the cos and sin functions with an imaginary number in there results in the cosh and sinh functions
 
6:44 PM
I don't know how to interpret what I just did though
it feels more like I hacked to get the answer
 
Replacing a purely real angle $\alpha$ with a purely imaginary angle $i \alpha$ converts the trigonometric cos and sin functions to hyperbolic cosh and sinh functions by doing what I just did above, the exponentials get extra $i$'s (or get eliminated), that's all
@Semiclassical the fascinating thing about superintegrability to me is you can get the LRL vector theoretically and explicitly i.e. predict it should exist and it's form
In classical mechanics, the Laplace–Runge–Lenz (LRL) vector is a vector used chiefly to describe the shape and orientation of the orbit of one astronomical body around another, such as a planet revolving around a star. For two bodies interacting by Newtonian gravity, the LRL vector is a constant of motion, meaning that it is the same no matter where it is calculated on the orbit; equivalently, the LRL vector is said to be conserved. More generally, the LRL vector is conserved in all problems in which two bodies interact by a central force that varies as the inverse square of the distance between...
 
I imagine part of it is simple unfamiliarity
Angular momentum conservation is familiar and therefore not surprising
 
Vaguely, if a system allows separation of variables in more than one system of coordinates, then because you end up getting non-trivial expressions being equal to separation constants, you'll have new invariants, so the Kepler problem separating in spherical (as usual) and parabolic (as in that post) results in the parabolic separation constants, the LRL vector comes from playing with the parabolic separation constants as in that post, which is cool
 
Whereas LRL is not
@bolbteppa yeah
 
I think that's just so cool, took so long to see
So the question is, when does a problem separate in more than one coordinate system, at least for finite motion systems it's related to action angle variables and from this you find concrete conditions when it will happen (end of Landau)
 
6:59 PM
iirc, one basic difference between the spherical vs. parabolic solution is whether the motion is a rotation or a libration
which i think in turn is why the quantization condition is different when working in spherical coordinates vs. parabolic coordinates
 
I don't see how to apply this to the harmonic oscillator though, let alone end up with a conserved tensor :p
 
8:00 PM
Making sure I'm not insane: the only proper subfield of $\mathbb{C}$ containing $\mathbb{R}$ is $\mathbb{R}$ itself, right?
 
@SirCumference Right. $\mathbb{C}$ is a degree 2 extension of the reals.
 
Yep. Sometimes I feel I'm losing my touch with basic algebra :/
 
 
1 hour later…
9:25 PM
@danielunderwood cuda10 came out in August I think...
@danielunderwood high order optimizers exist, but are generally too computationally intensive to use for neural nets
 
Ahh I see. Just finished up the tuning course that for whatever reason contained stuff about softmax...so now I actually know what softmax is
 
11:14 PM
@JohnRennie While the joke remains funny, I actually asked a few theorists about their funding situations. In addition to the classical requirements they seem to need computing support (lots for some of them), and to attend more conferences than experimenters ( per capita travel budgets ran about the same as the experimenters, but they didn't have to do on-site work so the money all went into conferences and the like).
Still cheep compared to buying 1 kiloton of LOS or 500 bespoke DAQ boards, but more than just wastepaper bins.
 

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