« first day (2366 days earlier)      last day (2563 days later) » 

9:02 PM
@Slereah I think I have to use AC for this proof
why should PDE require AC
 
Because the axiom of choice is true
 
Actually maybe I don't need a Hamel basis
This is just a messed up vector space
 
Do all Hausdorff smooth manifolds have global unique solutions to the geodesic equation?
 
Certainly not global!
 
People always say that they have local solutions but what manifold doesn't admit global ones?
 
9:06 PM
You know darn well there are incomplete manifolds
@Slereah $\Bbb R-\{0\}$
 
Well I don't mean the "at least one", I mean "at most one"
Is there any manifold that has two solutions
 
Oh, any solution is uniquely determined by $\gamma$ and $\gamma'$ at one point along the trajectory
 
Ah yes
So only non-Hausdorff manifolds fuck that up
 
I shouldn't think so
 
what else would
(that is also a smooth manifold)
 
9:08 PM
the proof doesn't require hausdorffness, just local coordinates
 
But there's pretty obvious examples for non-Hausdorff manifolds
 
Let $\mathcal H'(M)$ be the space of functions spanned by the set of harmonic functions $f$ that have the property that when restricted to each unbounded component of $M-D$ it is bounded either from above or from below for some compact subset $D\subset M$.
 
For the line with two origins, the line that passes through $0$ and the line that passes through $0^*$ are two valid solutions
 
are they?
have you actually proved that
I'm thinking there's some issue with the notion of curve in such a space
 
Well it's certainly the case if we consider the equation on each of the two coordinate patches
The issue might be related to the non-unicity of limits
 
9:12 PM
I thought you couldn't have metrics or somthing
@Slereah aha
that's getting closer to the issue
 
Yeah you have sequences with two limits
$$\lim_{n \to \infty} \frac{1}{n} = 0$$ $$\lim_{n \to \infty} \frac{1}{n} = 0^*$$
both valid limits
 
So I'm not sure that a curve even makes sense in that space
 
our quantum professor was sick and I just got back the results of a chest xray confirming I have pneumonia
 
Well it makes sense, but they may get weird
 
our notion of continuity makes no sense
 
9:14 PM
when can I fairly say my quantum homework is killing me
 
yeah that's why I'm having big doubts about how to define vector fields on 'em
Since that involves derivative and that may get delicate
 
wait, do I lose rep for downvoting things?
 
The line with two origins and the splitting real lines aren't too bad, but then you have weird manifolds like the complete feather, where every point has a branching point
 
@Phase answers, yes
 
How do you define anything there
 
9:15 PM
@GPhys oh geez
 
You need to use the ol' $f^{-1}$ definition of continuity.
Good luck.
 
of course I could answer questions on physics.SE, but I will quickly relose the rep downvoting the endless swath of garbage answers
 
yeah, quite so
hopefully derivatives will be unique and be the same on all patches
 
There should be a rule that when a post has -2, you get the rep loss refunded
 
Otherwise, I'm not sure what happens
 
9:17 PM
So you lose rep for -1 on random posts
But if someone agrees with you then it's likely shit
 
at least some answers are so bad that I can just report them instead of wasting vote rep physics.stackexchange.com/a/329470/10908
 
the only thing even close to calculus I found on the topic is that for a non-Hausdorff manifold, if $p$ and $q$ are adjacent point, then $f(p) = f(q)$ for a continuous function
 
sure
I believe it
hence they're terrible
why are you doing this to yourself?
 
it is an intriguing topic
non-paracompact manifolds less so, for some reason
I guess because they're less easy to visualize
 
...fundamental theorem of calculus?
 
9:26 PM
It does not seem fairly obvious
 
16=4^2
is that the hint?
This is so cryptically written
Where the hell did the $4$ come from anyway lol
 
David Gauld is the guy who's way into non-paracompact manifolds
He loves everything long
 
I mean, TFC is $f(x)=\int_0^L \gamma'(t)\cdot\nabla f\,dt$, where $L=r(p,x)$, $x\in B_p(4)$ and $\gamma$ is the geodesic from $p$ to $x$.
Ah yes
FTC
Crazy!
 
why the 16 though
oh, i guess it is $4^2$
 
9:43 PM
yeah $L$ is at most $4$
So that integral is $\le 4\sup |\nabla f|$
 
And I suppose that $\gamma'$ is always of norm $1$
 
Yeah I'm picking arc length param
 
Hm
I should try to find Krasnikov's email again
he was last seen working at the observatory of Pulvoko
In Mother Russia
he's not listed on the staff page
 
Is he alive?
 
his last paper was in 2016
ah, found an email
S.V.Krasnikov@mail.ru
This one seems more modern as it's not in the soviet union
Let's try again
In that paper there's $B \star C \in \mathrm{Bd} N_1$
 
10:06 PM
It's definately a function that outputs a manifold point
Mail is sent, hopefully it's not dead
it's slightly annoying that Carroll, HE and Wald all use a different version of the Riemann tensor
gotta keep track of what indices are what
 
...what?
Oh
There's also two sign conventions
be careful
I think Wald has $G=-T$, no?
Weinberg has $G=-T$
 
Oh bother
 
10:41 PM
Wald says that the trace of the EFE gives $R = T$, but what happens to the Ricci scalar term?
Isn't the trace of the metric tensor $g_{\mu\nu} g^{\mu\nu} = n$?
Or the signature or something
 
halp
set theory
what is $(M-A)\cap U$
@Slereah it's 4
So $R_{ab}-\frac{1}{2}Rg_{ab}\mapsto R-\frac{4}{2}R=-R$
 
Ah, I see
But of course that's only valid in 4 dimensions
 
spacetime is 4-dimensional
 
Says you
I think that would be $(M \cap U) \setminus (M \cap U)$
 
that's $\emptyset$
 
10:48 PM
The algebra of sets defines the properties and laws of sets, the set-theoretic operations of union, intersection, and complementation and the relations of set equality and set inclusion. It also provides systematic procedures for evaluating expressions, and performing calculations, involving these operations and relations. Any set of sets closed under the set-theoretic operations forms a Boolean algebra with the join operator being union, the meet operator being intersection, the complement operator being set complement, the bottom being ∅ {\displaystyle...
$$(B\cap C)\setminus A=B\cap (C\setminus A)$$
 
Set Theory is too hard
 
Set algebra is like the easiest part
you can just draw circles to figure it out
 
The latex glossary works like shit
I don't know how I managed to work it out during my last thesis
I think I'm gonna use the nomencl package instead
 
11:20 PM
@0celouvskyopoulo7 I just read the monotone class stuff. "We
leave it as an exercise to the reader to show that **S** is a monotone class that contains **A**. I suppose I will be writing a proof. hehe. I should be able to do this.
 

« first day (2366 days earlier)      last day (2563 days later) »