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9:00 AM
That paper uses $\Lambda TM$ for the space of sections on polyvectors
Lame
That's notation for a bundle, not sections
 
9:16 AM
is "polyvector" what you use if you find "tensor" not pretentious enough? :P
 
9:28 AM
@ACuriousMind Dual of $n$-forms
Also their direct sum, I think?
"a polyvector field, to be precise but in the following we will not bother writing field everywhere"
What kind of lazy hack doesn't write "field" for a field
 
@Slereah It's pretty common to say that something like $T_{\mu\nu}(x)$ is a "tensor" and not a "tensor field", no?
 
I suppose
But vectors and polyvectors are like
I'm used to having both vectors and vector fields being discussed
While tensors are usually only tensor fields
it's rare to talk only about tensors
also this is a fancy math paper, not some physics lecture
 
that's why the author even bothers to admit that technically there should be a field
physicists just call everything tensor :P
unless they call everything field when they really mean "function", but neither is very helpful, really
(I'm exaggerating, but not completely)
 
9:50 AM
It's hard to find an introduction to BV-BRST in between a physicist and Urs Schreiber
Also one that doesn't go into quantization
Also is it me or does the pullback have no other goal than to make something look fancier
 
is that bad
 
Do we really need $\phi^* j$ over $j(\phi)$
This one seems nice, although very bad pagesetting
 
 
1 hour later…
11:19 AM
Ugh
I probably should learn about supermanifolds first
I'll go back to the DeWitt book
 
it's just manifolds with fermionic coordinates, don't worry :P
 
@ACuriousMind Well that explains it fine!
 
 
3 hours later…
2:37 PM
A notebook
I think learning about superspaces will require
 
user434058
@Slereah Ah, you're speaking the "Yoda" dialect...
 
Am I
It's in the proper grammatical order
 
3:28 PM
is raison d'être in English vocabulary?
 
@CaptainBohemian Yeah, although not universally
Many would understand it, but not everybody would be my guess
It's also the name of a pretty tasty craft beer in the US, which they make a completely over-the-top version call 'Raison d'Extra'
 
@tpg2114 only native English speakers and English scholars or students and French understand it?
 
I wouldn't say only scholars would understand it -- it's probably something we've come across in high school at some point in the US. Along with things like deja vu and other phrases from other languages we've adopted.
How many remember it or use it often is what I don't know.
I also can't speak for non-American English speakers, native or otherwise
 
@tpg2114 our English curriculum in high school never taught us deja vu.
 
We definitely had some lessons on loanwords at some point. I didn't take English classes after high school, so I know they came somewhere in the primary school system
 
3:39 PM
@tpg2114 We didn't have English classes in primary school.
our English classes started from junior high school.
 
Raison d'être is in English but nobody pronounces it like French
bc they are awful at French
 
There's some French-named towns near me, Versailles and Bellefontaine. The locals who live there pronounce them like "Ver-sails" and "Bell-fountain"
About as un-French as you can get
 
 
3 hours later…
6:17 PM
I've got an incredibly ill-formed question... if I have governing equations for a deterministic dynamic system, what math tricks do I need to convert it into governing equations for the probability density of the system state?
I'm thinking something like the Burgers' equation
 
6:32 PM
Errr do you mean the evolution of the probability density with time?
 
Yeah
 
Same as everything
Poisson bracket of the Hamiltonian
 
So for example, if it was deterministic, the probability density at the start would just be a delta function at whatever value and it should stay as a delta function
"Same as everything" -- I'm an engineer who does CFD, so this is all outside of my experience :)
 
Write your initial probability density in terms of your canonical variables, and then do its time evolution
Never done Hamiltonian mechanics?
 
Maybe once in a dynamics of vibrations class
But not for fluid dynamics
But it sounds like that's my starting point
 
6:37 PM
For any variable $f(x(t), p(t))$ in classical mechanics, you can write its time evolution as
$$\frac{d}{dt} f(x,p) = \{ f, H\} (x,p)$$
With $H$ the Hamiltonian and $\{,\}$ the Poisson brackets
This is the Liouville theorem, if you need more details :
In physics, Liouville's theorem, named after the French mathematician Joseph Liouville, is a key theorem in classical statistical and Hamiltonian mechanics. It asserts that the phase-space distribution function is constant along the trajectories of the system—that is that the density of system points in the vicinity of a given system point traveling through phase-space is constant with time. This time-independent density is in statistical mechanics known as the classical a priori probability.There are related mathematical results in symplectic topology and ergodic theory. There are extensions of...
 
Okay -- I'll see what I can dig up. Thanks!
I've come at this from a different perspective, where I assume my deterministic variables are stochastic functions of a random variable, and then project onto a polynomial chaos expansion
 
user434058
7:25 PM
Yes! This exactly was my doubt that night! (Funny thing, I had starred bookmarked it for referencing it in the future quite a time ago, though I forgot it when I was struggling with the transition from Lagrangian mechanics to Hamiltonian mechanics :-))
 
user434058
15
Q: Why exactly do we say $L = L(q, \dot{q})$ and $H = H(q, p)$?

knzhouIn classical mechanics, we perform a Legendre transform to switch from $L(q, \dot{q})$ to $H(q, p)$. This has always been confusing to me, because we can always write $L$ in terms of $q$ and $p$ by just taking the expression for $\dot{q}(q, p)$ and stuffing it in. In thermodynamics, we say $U$ ...

 
@FakeMod I pointed you to my answer there about a month ago :P
 
You mention that the configuration space doesn't have a metric, what kind of object is it?
Oh I just found the answer nvm lol
is the topology of the configuration space ever of much interest or is it just "there" for the sake of rigour?
 
@Charlie I'm not sure what you mean by it just being "there" - the configuration space is the space of your generalized positions. If these are really just positions then it's a boring $\mathbb{R}^n$ but if they are e.g. Euler angles because you're describing orientation in space then it's $S^3$.
 
user434058
@ACuriousMind That's when I bookmarked it. BTW, I had upvoted your answer then, but TBH, I couldn't make up more than 30% of what you said there :P
 
user434058
7:57 PM
Heh, funny. Folks have upvoted my comment linking my (related) answer under another question, however my orginal answer hasn't recieved an upvote. Probably the comment was upvoted because of its relevance rather than my answer's quality, probably...
 
Howdy
Mentioned this the other day, but getting quite interested in geometry. Is there any good books that start off broad then develop links to GR and QFT? (Or any other ohysics theories)
 
 
3 hours later…
10:37 PM
Does anyone know why this was off-topic? physics.stackexchange.com/q/439184/134583
 
10:51 PM
@NikeDattani It's closed as HW-like/check-my-work
(I still don't get why the close notice is hidden from low-rep users nowadays :P)
 
@ACuriousMind It says closed as "off-topic"
Can it not be closed as "community-specific reason: HW" ?
I'm only asking because this user recently asked a question about the Berry phase on Matter Modeling SE.
So I checked out her previous network posts and found that one.
 
It is closed as that, but the closing notice is only visible to users with the close/reopen privilege
For some reason SE decided to hide the specific close reasons from low-rep users with the last redesign of the notices. We've already complained about that at the time on meta, but to no avail.
 

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