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01:24
my professor has written in his notes, in the context of the semiclassical model of electron dynamics that this model breaks down in the free-electron limit because the electron energy can increase without bound, but we have said that we want to forbid interband transitions. he then writes that we must have $eEa << \frac{E_{\text{gap}}^2}{E_F}$ and that this is easy to satisfy for metals but not for insulators, for which [...]
[...] we can see electric fields causing interband transitions. the thing im confused about is dont metals have no band gap, so isn't $E_{\text{gap}}=0$? then how can we satisfy the aforementioned criteria?
 
1 hour later…
02:25
@Relativisticcucumber yeah, that's nonsense; as far as miao miao goes, we now have a mathematically rigorous theory for these things, and so we should avoid all the guesstimations that used to be the only way to get answers.
@NOTEBook You have made a reputation for yourself, routinely coming in with such an attitude, I'm not inclined to help. Also, the question that you linked to, had many correct answers on it. If you cannot recognise that the correct answers would also answer your specific question, then it will take a lot of effort on the answerer's part to dispel your question, and so there is a lack of motivation on everybody else's part.
02:38
@PM2Ring I know. I think I told you before that I bought Carlson's book. Don't understand it much, but it is a wonderful new way to look at functions.
03:00
@naturallyInconsistent What is wrong with my behaviour? I mean i never said something bad to someone. I ask a question and if someone answers i discuss it with them and leave. Maybe my questions are too dumb. Also I didn't intended to say that everybody have to help others, I just wanted to say that if someone knows about this high school problem they should consider helping.
Have you not realised that there has been quite a lot of people replying to you on this topic? If you cannot see that you have done something wrong, nobody can help you.
I asked what is wrong with my behaviour that nobody wants to answer like before this topic started. It all makes sense if nobody answered me after this because they don't like my attitude.
@naturallyInconsistent like the entire semiclassical model is a no go u mean?
@NOTEBook i think you should not self victimize. i interpreted your behavior as someone who was naive in their assumptions. now that it has been explained to you, if you realize that what you did was not a good approach, learn from it, and change, i doubt people will be negative toward you on average. we're all adults, and i assume you're a child, so it's fine. just learn from the experience and adjust your approach so you have a higher chance of getting the help you need.
03:24
@NOTEBook "maybe my questions are too dumb". multiple people have explained why you're not getting help in chat, you don't need to make up extraneous self pitying explanations. and you clearly said much more than people should "consider" helping you, which is why you got the reactions you did. reflect with honesty.
03:48
I need an explanation for a simple mechanics problem. Consider a ball rolling down an inclined plane without slipping. Now consider angular momentum of the ball relative to initial point of contact. For
For that point the angular momentum generated by friction is zero. Does that mean the ball doesn't roll relative to that point?
Can you please give any suggestions about good books on rotational mechanics?
 
1 hour later…
05:16
@Relativisticcucumber no. The issue is that if you have a constant E field over all space, then if you include this E field in V, all quantum states will break down. The only way to do this correctly, is to put this E field in A, and then the theory will give you a beautiful answer.
@DebanjanBiswas you have a few forces, e.g. Weight, Normal reaction force, friction, and maybe more. Considering just the 3 forces, as long as they do not meet at a point, then at least one of them will be providing the angular momentum.
@DebanjanBiswas there is no such book; usually a book just treats classical mechanics properly, and it would automatically include rotation problems.
05:49
@naturallyInconsistent but I don't see any force providing the angular momentum for rolling
@naturallyInconsistent normal and mg•cos theta create opposite torques and cancel out
@DebanjanBiswas if you pick the point of contact as the pivot, so that normal reaction force and friction do not provide torque, then weight will provide the torque. If you pick the intersection between weight and friction as the pivot and so they dont provide torque, then the normal reaction force will provide the torque
the point of application also matters.
Here the torque is provided by mg•sin theta then?
Oh that's right
But as it's passing through COM, should it produce rolling?
it depends solely upon where you picked the pivot
@naturallyInconsistent then suggest the best classical mechanics books
if you picked the CoM as the pivot, then the friction provides the torque
05:57
Hmmm
06:27
I thought @Debanjan said that the friction is zero.
07:02
@PM2Ring how to pure roll with no friction?
07:20
GR computing could be revolutionary like quantum computing
one can, in principle, use time dilation effects to speed up computation
9
A: Relativistic Computation?

Alex LTo quote a comment Scott Aaronson made on his blog: Can you perform an arbitrarily long computation with minimal effort, by leaving your computer on Earth, boarding a spaceship that accelerates to close to the speed of light, then turning around and returning to Earth, where you find civilizatio...

Aaronson talks about SR computing here. GR computing could be more feasible
@RyderRude this is the kind of insanity i can get behind :)
would it be correct that the less mass your computer has, the more difficult it would be to exploit the dilation speedup method?
In the SR method, u have to leave the computer in an inertial frame and accelerate yourself. So the mass of the computer is irrelevant. but ur own mass is relevant
oh i see
but idk about the GR method. black holes are known to freeze time at their horizon
but I think one would still need to freeze oneself and let the computer run normally
this is the naive method. maybe better techniques are possible after we understand black holes better
07:40
interesting
if we're talking about parking at blackholes, can we also talk about production of gravitational waves with an anisotropic wavefront to produce a focal point in which a tiny computer could operate?
idk :P
there r spacetimes in which one can perform infinite time computations. like, u want to verify the twin prime conjecture. u just let a computer run for infinite time
and then u encounter the computer and only finite time has passed for u. but u can just read the result of the infinite time process
Slereah mentioned one such spacetime here
these spacetimes could modify our understanding of computability
07:47
@naturallyInconsistent Exactly. The specification is inconsistent.
66824468 : i think this paper explores relationships between computability and GR
right
@RyderRude Greg Egan's Orthogonal trilogy is set in a universe with a ++++ metric. gregegan.net/ORTHOGONAL/00/PM.html
@Slereah what was the spacetime with infinite time paths and finite time paths between the same two points
@PM2Ring oh
@PM2Ring i haven't read his stories yet
if gravity is polarised would time flow backwards in positive gravity? or just things would repel eachother?
07:55
i think that physics determines math as much as math determines physics cuz math is part of the physical world
some people think that the largest natural number is the number that the universe can store in some sense
@RyderRude You can read the stuff on the page I just linked without spoiling the stories.
@PM2Ring thanks
@antimony time doesn't flow in GR
flow of time is an illusion of consciousness according to GR
but it is a debated topic
oh i see, thanks @RyderRude
since i read this "clocks at higher altitude tick faster than clocks on Earth's surface" (en.wikipedia.org/wiki/Hafele%E2%80%93Keating_experiment)
it made me wonder if you could engineer a region of very very low gravity in a tiny space to fit a small computer chip
or if the gravity wave is more like 'rarefaction' and there's a limit on lower bound. ie. a gravity vacuum i guess you'd call it?
@antimony theoretically, one can have zero gravity
oh i see
08:02
that's what I meant earlier. one has to leave the computer in a low gravity zone, and accelerate one's own body or spend time near a black hole. then the computer will be fast relative to you
@RyderRude malamenthogarth
A Malament–Hogarth (M-H) spacetime, named after David B. Malament and Mark Hogarth, is a relativistic spacetime that possesses the following property: there exists a worldline λ {\displaystyle \lambda } and an event p such that all events along λ {\displaystyle \lambda } are a finite interval in the past of p, but the proper time along λ {\displaystyle \lambda } is infinite. The event p is known as an M-H event. The boundary between events with the M-H property and...
What's an inertial frame
i meant a free fall frame
what I'm thinking is that an accelerated frame has slower time compared to an inertial frame. In the same way, can one say that inertial frames in high gravity regions have slower time than compared to inertial frames in low gravity regions? @Slereah
in this way, one would get an asymmetry between inertial frames
How would you compare the time between two such frames, you'd need to go through the intermediary parts, breaking the conditions of aninfinitesimal neighbourhood
08:11
yes. i think I don't have a way to compare the time. how about this : i make people sit in the high gravity and low gravity regions. and then I make the people meet at a latter time and compare who is older @Slereah
That's just the same thing
The invariance under Lorentz transform is meant to happen in an infinitesimally small spacetime region
yes
if I start with two twins and make them free fall along different curves. but one of the twins spends time in a higher gravity region, then would that twin decidedly age less when they meet again? @Slereah
high gravity vs low gravity seems like an absolute concept
like, only one twin can claim to be in higher gravity regions, given by stress energy tensor
so it seems like an absolute notion, like accelerated frame is an absolute notion
08:55
@PM2Ring Greg doesn't explore time here
but it is interesting how matter behaves
i think time would behave just like in SR except there would be time contraction
09:15
Are the words "configuration" and "Microstate" equivalent?
Well, it really depends on what is a configuration for you. A (classical) microstate is determined by assigning the position and momentum of each particle
Yes i understand that. But what is a configuration then? i thought it is also "assignment of positions and momenta"
@Madder Sure, that is a microscopic configuration, which is a synonym of microstate
But you can use configuration more broadly. A macroscopic configuration is a macrostate
Btw, very funny name!
It means something like "Mister Softman" or small )
Configuration only means that you have a set of variables and you fix the value of each. Then, the type of variables is what matters: macroscopic variables, macroscopic variables...
@Madder ACM told me that it would be the German version of Mr. Feynman D:
09:24
That would be Herr Feynman.
Fein is the word for "small" or soft . it is however read the same.
Okay so if i understand you, we can write the following.
A configuration: Is either a macro or micro configuration.
A Macroconfiguration is a macrostate, a micro is a microstate.
So the word configuration is equivalent to the word "state"
Oh, I see. The pun was that I originally said that "Feynman--->Feynmann" (which is a common mistake) would make me German, so that's what happened
ACM told me that if I really wanted to change the name it should be so :P
Are you actually called Feynman?
I wish :P
lol! i bet your name is beuatiful as well, i would not want to be feynman. Feynman is already taken. I am something else, and that is my own.
That was the wittiest answer I could think of. A simple "no" would have been plain :P
09:29
:D
So do we agree on the terminology and equivalence between state and configuration
Just wait until i become the "papst" of physics. I am going to decree a unification of used terminology or immediate withdrawl of all diplomas.
Good luck then
@Madder In this specific context, yes
I would be careful though, because for example in the context of lagrangian mechanics, a configuration is just the set of all positions, while what we are calling a state now also includes velocities/momenta
But as long as you understand it here, it's an acceptable choice of words
(Wow, the last line was so German)
09:50
@HerrFeinmann It's surprisingly hard to find a proper etymology of "Feynman", but I assumed it was a Germanic name meaning "fine man" - the modern German version of that would be "feiner Mann", hence: Feinmann. While modern "fein" can mean soft or tender, it can also mean - like the English fine - something like excellent or elegant, though it is usually not used in modern German like that a lot
I think i have some confusion about entropy.

if we consider some lattice of vector orientations at the lattice points. We say that the oriented vectors have lower entropy than randomly oriented.

But what confuses me is this: Let us look at the oriented phase.
If we assume all lattice sites take the same orientation, we still have 360 degrees. So the direction of this orientation, is infinite, it could be 24 degree 23 partial degree .. and so on.
So we have literally infinitely many states in this oriented phase, and similarly in the disoriented. Do i understand entropy then, that the diso
@ACuriousMind Yes, I noticed that it was hard after writing that message. I tried to look it up but I couldn't find much. Actually you made a good guess
@Madder It sounds to me as if the confusion here isn't specific to lattices: Consider simple $N$ particle mechanics, i.e. a classical phase space $X=(\mathbb{R}^6)^N$. Macrostates are probability distributions $f(x,p)$ on $X$, and the (Gibbs) entropy is $\int f \mathrm{ln}(f)$.
When $f$ is uniform, i.e. constant on some compact volume $V\subset X$ and zero outside, this becomes proportional to $\mathrm{ln}(\vert V\rvert)$ (where by $\lvert V\rvert$ I mean the Euclidean volume of $V$ in the ordinary sense). Now, every $V$ with non-zero $\lvert V\rvert$ contains infinitely many points of $X$, yet you can have bigger or smaller $V$s!
The idea that entropy is about "counting" states is only really accurate (i.e. literal counting) when the event space $X$ is discrete
10:11
@RyderRude Yes he does, but you have to explore the rabbit holes. ;) The novel involves sending a rocket ship on a high speed journey so that the rocket passengers have time to work on an important problem. See gregegan.net/ORTHOGONAL/02/Motion.html especially Time Without Timelike Directions gregegan.net/ORTHOGONAL/02/Motion.html#ACC
you have to consider the phase space volume
In the ++++ metric, you lose the distinction between timelike, null, & spacelike intervals. So it's rather different to a Lorentzian world. OTOH, the arithmetic is simpler, since it's just plain old Pythagoras.
The quantities of interest tends to also converge faster. However, when we want to convert the results of those Euclidean metric back to our universe that follows the Minkowski metric, then the analytical continuation step is extremely treacherous.
10:26
@naturallyInconsistent Hm? The analytical continuation is "easy": The Osterwalder-Schrader theorem guarantees for every set of Euclidean n-point functions/every well-defined Euclidean path integral there exists a Minkowski QFT with the corresponding analytically continued n-point functions. The difficult part is well-defining the Euclidean path integral in general.
@ACuriousMind well, if you have ever touched numerical, you will know that the errors explode exponentially when we do that, unless we already know the correct analytical form of the Minkowski case, so that we can force the errors out. Analytical continuation is not kind when we have errors.
just don't make errors ;P
but sure, okay, numerically it's hard
tears drop down uncontrollably
10:49
@PM2Ring oh
@PM2Ring i think QM also must choose a time direction, even in Euclidean theories
i don't like entropy based ideas cuz entropy is not fundamental
time is fundamental
i also think there might be a deep connection between the psychological arrow of time and the QM arrow of time and the GR time. all of these co incide
Ok. But there isn't a unique fundamental way of defining time. Years ago, I read a fascinating book with a title something like The Seven Arrows of Time. Unfortunately, I can't recall the author(s) name.
I don't think Egan is trying to claim that the entropy arrow is the ultimate fundamental basis of time. It's just a practical, useful arrow.
@PM2Ring i think, in QM, the wavefunction collapses in a single direction of time, which does pick time asymmetry
entropy should be less fundamental
like, the wavefunction can't collapse bidirectionally without contradictions
also, in practical experiments, the wavefunction collapse is always modelled past to future
where past refers to psychological past and future is psychological future
11:05
@PM2Ring Penrose? Ne'eman?
@naturallyInconsistent I'm pretty sure I'd remember if it had been Penrose.
The book wasn't heavily mathematical, but the author knew his physics, and IIRC, was fairly well-educated in philosophy, too.
Carroll proposes a model in which the entropic arrow changes direction mid-way
Carroll mentions it here
You kinda need something like that if you want an eternal cyclic cosmos. But it's always seemed a bit contrived to me. And the reversal mechanism is no less mysterious than whatever "caused" the initial conditions at the Big Bang.
Of course, causality isn't well-defined "before" time itself exists. ;)
yeah...
@PM2Ring in this model, causality exists before the big bang
the time of the spacetime manifold is taken as more fundamental than entropy time which can reverse direction
Whenever you try to talk about the cause of the Big Bang you have to do something dodgy with time ordering & causality. Invoking some kind of meta-time is a common technique.
11:22
@PM2Ring i would say it is not dodgy. at the fundamental level, there is nothing fishy. It is just the GR equations. but at he emergent level, entropy changes direction
I like the idea that the "precursor" to the spacetime manifold was in some symmetrical state. But the symmetry was broken, thereby putting the manifold into a -+++ state.
i like the idea of explaining the initial conditions using some beauty argument about symmetry..but it cud also be that the initial conditions have no explanation
if physics is able to explain initial conditions, that wud be a huge achievement
Which reminds me of Mirror Universe theory physics.stackexchange.com/a/487304/123208
@PM2Ring yes
if we assume psychological arrow is reduced to entropic arrow, then the people in the mirror universe and our universe have mirrored time
Yes. That restores the symmetry.
And explains where all the antimatter went.
11:28
I think psychological arrow may be related to QM time and may require deep understanding of consciousness and quantum gravity
@PM2Ring lol
@PM2Ring there is a movie called Tenet where they reverse their psychological arrow by converting their body to anti particles
I've heard of that movie, but I haven't seen it. But we get questions about it from time to time on the Scifi stack.
It appears to be a bit paradoxical, with numerous plot holes.
how do we answer the question "why can we choose to move forward and backward in space but not in time"?
@PM2Ring i think it says in the movie to not think about it too much
@PM2Ring i recommend it 7/10
it doesn't have plot holes. just unexplained things
It's pretty hard to do any kind of time travel story without creating paradoxes. But Tenet sails full steam ahead into paradoxical territory. ;)
11:36
lol
it has unexplained stuff
The psychological arrow of time seems pretty fundamental to us, because it's ultimately how we experience time. OTOH, it's just what our mind/brain has managed to cobble together in its attempt to model time.
@PM2Ring miao miao cant know; just suggesting
12:04
@ACuriousMind Thanks for you reply. So in the case of continous event space, what would be the proper interpretation?
@Madder well, it's still "counting", but in the figurative sense that computing a Euclidean volume is "counting how many points are inside the volume"
more or less exactly like an integral is "like a sum" except it's not :P
Do you guys know any long, detailed videos on the interpretations of QM? Something on the level of the classical papers. I want to listen to it in my dead time
Talks at conferences et similar are good as long as they have decent audio
@ACuriousMind Oh i see.
@GroveRover hi. if ur goal is to learn interpretations, i think best way to learn interpretations would be to read books/papers about them
some interpretations have their math equations and stuff, e.g. Pilot wave theory and Many worlds. so listening to videos wouldn't be ideal
this is a debate between QBism and Many Worlds
 
1 hour later…
13:31
@RyderRude I'd like to watch while eating and stuff like that so papers are not suitable (I agree they would be better)
Equations can be shown on video
What about printing papers and eating those?
These younglings...
@HerrFeinmann 💀
Now guys it's about time I prepare the dreaded superconductivity exam
oha
good luck
13:48
@HerrFeinmann gl
@GroveRover oh
i found a lecture presentation on many worlds youtu.be/Rtaq1DJPhBI?si=LkVc9xSLAJvlrRNV
I will need something stronger than luck: interest :P
cmon, superconductivity is quite interesting, no?
@TobiasFünke is it a kind of qft
@TobiasFünke Oh sure it is, that's why I chose the class. The bad thing is that the class turned out to be one of the worst experiences I've ever had with physics. Total scam :P
14:02
whut :( oh no
@HerrFeinmann magnetise the exam paper
No written exams anymore
Most of Master's degree exams are oral here
this is another QM interpretation but not a big one. youtu.be/sshJyD0aWXg?si=zlKkNW_ck_rCpRWF .
@HerrFeinmann do you like this more?
@TobiasFünke Complex question. I have less performance anxiety than for written exams, because I have more control over the situation. On the other hand, the kind of questions is different and I have the impression that acing an oral exam is not nearly as impressive as getting a perfect score on a written exam, which surely doesn't help with the impostor syndrome :P
14:11
I see
An oral exam is more about acting than knowledge :P
well, yes, oral exams are more "forgiving" in the sense that the lecturer can immediately correct you or help you to notice you did something wrong/have a misunderstanding. On the other hand, I think in oral exams you can better see if a student really understood the subject (to a certain extent)
@HerrFeinmann nah, I would disagree
You know, dramatic pauses, delivering lines at the right moment, using the right amount of pathos
much like a TED talk :P
At my uni we had for all "big" subjects (which were 2 semesters long) written + oral exams in fact. You needed at least 50% of the exercises to be correct to be allowed to write the exam (each semester), but there was no grade. The oral exam was then over the two semesters and was graded.
it was like that during the undegrad
or bachelor's, whatever
14:16
ah yes, I meant Bachelor
I'm completing my Master's
In masters this was different. but except the defense of the thesis (of course) and one big and one small oral exam, everything was a written exam, if I remember well
I guess it is quite normal
Also because the classes are, usually, and in my experience, much smaller. But this may also depend on how large the faculty is
Small faculty in my case
yeah... so oral exams can be much less work for the lecturer lol
I think that some lecturers wouldn't be able to solve an exercise :P
14:19
or you use the exact same written exam over and over. this might be the most economically procedure
haha
There was my analytical mechanics professor that would prepare like 5/6 written exams per year. The fact is that he has been doing that for decades and those exams are all the same but different
He's been exploring every possible combination of rods/disks attached to springs on rotating planes
Or rods attached to other rods
and disks rotatings inside circles lol
Connected to the origin by a spring
xD
what the...
Typically the computations are standard (although stability typically requires a lot of algebra for the secular equation) but sometimes you get a kinetic energy with 14 terms (guess who was the lucky guy?)
14:24
xD
I mean...the last time I did such a computation (perhaps not that complicated anyway), was like several years ago
but yeah, I guess with a bit of practice it is manageable (?)
@ACuriousMind Apparenly Lawvere typically asked that a topos would be sufficiently cohesive, which is like that every space can be embedded into a contractible space [which fine] but also every function space on that larger space is contractible?
Any idea why that requirement
Basic example being that Set is cohesive but not sufficiently cohesive since only the terminal set is contractible
@Slereah What do you mean by "function spaces"? The "standard" definition (cf. nLab) would just be that the subobject classifier is contractible. This implies the embedding of all objects into contractible objects, but nothing about "function spaces".
Well what nlab says comes from the original paper, but Lawvere's original definition is that one, ie tac.mta.ca/tac/volumes/19/3/19-03abs.html
apparently an equivalent statement to the contractibility of the etc
@Slereah but where is there a statement about contractibility of function spaces here?
(d) just defines in one line 1. what contractibility means and 2. that all objects should embed into contractible objects
$p_!(Y^A) = 1$
@Slereah That's just the definition of $Y$ being contractible
15:03
Wouldn't that just be $p_!(Y) = 1$
no, that's $Y$ being connected
a space is contractible if all mapping spaces into it are connected (which normal topology would express as "all maps into $Y$ are null-homotopic")
Hm
Ah I guess in more normal circumstances it would be with $A = S$
But for everyone
or $S^n$
So it's the existence of a boring space that can contain the other spaces
@Slereah no, it's a normal theorem of topology that $X$ is contractible iff for every other space $A$ you have that every function $f: A\to X$ is null-homotopic
that's what $p_!(X^A) = 1$ means
alright thx
had to look into that because technically Set is a cohesive category but it feels weird to claim such a thing :p
The codiscrete functor is just the identity and they don't feel very codiscrete
btw one thing that I have not seen so far is, are codiscrete objects typically contractible?
Feels like they should be but I haven't seen any property for the interaction of $\int$ and $\sharp$ so far
It is true of the trivial topology and the coarse diffeology [I think?]
@Slereah no idea, this isn't the kind of category theory I like :P
15:12
what's your favorite category
rings are nice I guess
answer is probably in Schreiber's monstrous book somewhere
but it is all entirely for $\infty$-categories so it's a tough read
$\infty$-categories seem to have more fun discrete and codiscrete objects since apparently they correspond to types of connections in some categories?
instead of being "points" and "blobs"
the least fun objects
Parmenides would have loved codiscrete objects
15:39

 Backup Room – The h Bar

A backup room for when The h Bar is busy. (chat.stackexchange....
RIP
 
1 hour later…
17:03
in lecture notes talking about landau levels where the levels are described by quantum number $\nu$, my professor has stated that electrons near the fermi surface have very high quantum numbers. why is this so? i thought $\nu$ is just an index in the same way that $n$ is in standard qm
@Relativisticcucumber well, the surface is the "top" of the part of the states that are occupied, so it has higher quantum numbers than all the completely filled states below it, no?
oh i think i see
hm
but he goes on to say that for this reason we can use the correspondence principle to treat this as a case where orbits reproduce classical mechanics
i am just uneasy about this statement
i mean i guess that is just what the principle says :P ok i accept
17:19
Echoing Arjun, is there a standard reference for tensor calculus? At a mathematical level that is consistent with how practicing physicists use it?
I think someone has suggested the beginning of Wald before for this purpose.
@SillyGoose What kind of questions would you expect such a reference to deal with?
"tensor calculus", from where I'm at, is just a silly name for the rules of index notation, nothing you'd write a book on
@ACuriousMind Sorry, what do you mean by this?
@SillyGoose As I said right after - I don't understand what content you expect this supposed reference to have
what is "tensor calculus" other than knowing how the index notation works?
or, somewhat more generally, doing differential geometry in index notation
I think that is the question I'd want such a reference to deal with: precisely what is index notation, including 1) the definition of the objects it manipulates and 2) the rules of manipulation and possibly 3) its shortcomings and 4) alternatives and 5) its various forms (e.g. different people using slightly different conventions).
you just want a differential geometry text :P
17:27
do diffeg texts go into index notation? I guess I didn't know that.
I mean, some of them may not (just like some physics texts like Straumann conversely generally don't use index notation)
Do you have a favorite diffeg book?
I have Lee smooth manifolds open and I think I see that chapter 12 has some index notation.
I guess maybe it is time to sit down and learn diffeg.
@SillyGoose nope (because I haven't really read any so much that could judge it)
do you have any diffeg resource recommendations?
but really I think focusing on "tensor calculus" as this obscure separate thing that manipulates objects with indices or whatever is misleading, it's really just doing differential geometry in coordinates where you declare some summation signs to be implicit
There are really only two golden rules: 1. No index may occur more than twice, once upper and once lower. 2. Both sides of an equation must have the same free indices (i.e. indices that occur only once). If you break them, you know you did something wrong, but apart from that I struggle to think of many things to say about it.
But I guess Wald is a good recommendation if you want someone to talk about the indices at a little more length since he does that "abstract" index notation where he doesn't want to "work in coordinates" but wants to have the same kind of index expressions
17:48
@ACuriousMind Stuff like writing the "transpose" of a tensor or etc. continues to trip me up.
@SillyGoose well it depends on what you mean by "transpose" - are you not just being "tripped up" because some text uses the word without defining it properly?
Now that is another possibility that I was hoping to solve by finding a good resource.
@SillyGoose but "transpose of a tensor" is not really some general concept that's being hidden from you here
it's just some text being imprecise :P
I can see an obvious way to define the transposes of tensors with 2 inputs/indices, but not in general
I guess you could do it with 2n indices too, treating it as an operator on $V^n$?
@SillyGoose i think it is because the transpose of a tensor is a basis dependent operation in general
one should replace it with a notion like the adjoint
the adjoint involves a metric and it is a well defined notion in the abstract
17:59
@Slereah I had an entirely different generalization via the symmetric group in mind briefly, but I guess that just shows it's not a common notion with an established definition :P
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