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16:23
hello . how can I show if $||x_k-x_l||\leq 1/k+1/l$ then x_n converges?
What space does $(x_n)$ live in ?
R_n
Do you know about Cauchy sequences ?
R^n
I forgot after graduated :( i tried to show like in this by using triangle inequallity but came up with harmonic series which diverges math.stackexchange.com/questions/490107/…
Well first you can show it's bounded since $||x_k-x_1|| \le {1\over k} + 1 \le 2$
Therefore by Bolzano-Weierstrass, you get that its set of limit points is nonempty
You then simply need to show it's a singleton
Proceed by absurd : suppose it has two limit points $a\lt b$
Take, $\epsilon = {||b-a||\over 2}$
And $N\in\Bbb N$ such that ${1\over N}\le \epsilon$
16:31
thank you very much. Ill give it a try
You'll take it from here ?
yes
Right, have fun :)
Hi Akiva
So, weird math of the day. For reasons, I'm interested in the following integral: $Z(\mu,g)=\int_{-\infty}^\infty e^{-\mu x^2/2-g x^4/4!}\,dx$
This can be written in closed-form using either a modified Bessel function (and some ornamentation thereof) or a confluent hypergeometric function.
There's at least one funny thing about it. If $\mu>0$, then $Z(\mu,g)\to 1$ as $g\to 0^+$.
But if $\mu=0$, then it instead goes to $+\infty$.
16:36
Wut ?
Why does it go to 1 ?
oh, wait. I'm being silly.
first off, forgot to include a factor of $1/\sqrt{2\pi}$ overall.
And $\mu$ also plays a role
Second off, I misread the paper I'm looking at and forgot that it's $Z(1,g)\to 1$ as $g\to 0^+$.
Since you can dominate the integrand you have that the limit of the integrals is the integrals of the limit
16:38
Right that seems more like it
Not sure why I thought it was weirder than that.
Nah.
It shouldn't :p
lol
Anyways. In the limit $g\to 0^+$, one has $Z(\mu,g)\to 1/\sqrt{\mu}$ when $\mu>0$.
So that's consistent.
Hi Ted
hi @Semiclassic and @Astyx
16:40
hi @ted
On the other hand, Mathematica fails to get a limit at all when I have it assume $\mu<0$.
Weird
You mean limit as $g\to 0^+$ ?
That should be $+\infty$
Hi @Ted
Why amoeba?
By restraining to a (sufficiently large) compact
16:42
Yeah, that's what it gives.
The $\mu<0$ case is where things are weird.
Or even by comparing it to the case $\mu = 0$
hi @Alessandro ... Because that's what your shape looks like :)
I apparently did better on my analysis written exam than on my algebra one for Polytechnique
I am confused
The weirdness of it, I suppose, comes from the fact that when $g>0$ the integral converges regardless of $\mu$.
Oh, it's supposed to be seven people looking into a well, seen from the bottom
16:44
So what does that all mean, @Astyx?
But when $g=0$, the integral is only finite when $\mu>0$.
LOL, OK, Alessandro.
It's all meaningless anyway
I might change it sooner or later though
Is it?
16:45
Isn't it ?
Socratic me isn't the best me
(luckily)
Yes, luckily for us all.
@Semiclassical Yeah, you could add some degree $6$ term in there and make things even more weird
Yeah, and the paper I'm looking at even suggests doing that :P
I guess if you want information on degree $4$ you could look at degree $6$ to crush the divergence ?
Not too sure where that would lead you though
$\mu<0$ vs $\mu>0$ is intentionally a bit weird: If $g>0$, the integrand has a single global maximum at $x=0$ when $\mu>0$ but has two symmetric global maxima when $\mu<0$.
16:49
I gotta go now
It's therefore valid to do a saddle-point approximation using the single maximum at $x=0$ so long as $\mu>0$.
Later.
I'd be interested in anything interstig you find, keep me updated !
But if you trust that approximation for $\mu<0$, you'll run into a nasty surprise :)
Seeya
16:58
hi @TedShifrin
oh no, Ted is here
oh noooes
I got really sick past 2 days. Maybe I overworked myself. I was studying for 13 hours for 2 weeks straight. I have been having migraine for past 2 days :S
it's tough to find a balance of work/play
yeah
17:00
but stress headaches indicate you're not at equilibrium
Yeah I will try find a better equilibrium
17:14
studying for 13 hours?? what?
The latest PHD Comics is pretty good: phdcomics.com/comics/archive.php?comicid=1963
so tempted to make a closed curve of this
but then it is impossible to turn a tenured professor into an grad student
Well... one unlikely way that will happen is the foundation of a research field need to be revised from the ground up, sending all experts back to the drawing board I guess...
maybe a dashed arrow from tenured prof to grad student signifying "convinces undergrads to go to grad school"
17:19
hmm, that might work
Meanwhile, a new [random] sounds quite physical:
Consider the scenario where you are at a platform and the train is preparing to leave
Suppose the train accelerates at 1 unit s-2 (because maths people don't worry too much about units when going abstract)
Is this the whole "how fast do you have to run to catch the train" business?
nice, I landed an internship with my gf's father with an operations research thing
oh, cool.
optimizing network connections
17:23
paid or unpaid?
nope. it's more subtle than that, it's about the geometry of the space abstracted form this scenario, we'll get to that
paid :)
find the best way to connect computers to all other computers
sounds like graph theory stuff
spanning trees
Now you are prepared to hop onto the train. Assuming you only move horizontally from platform to train with no vertical motion, you can choose to hop at any time t onto the train
17:24
I imagine you also want to do so in a way that's somewhat flexible i.e. you don't have to change the network a lot if you just add/remove one computer.
a stable solution, so to speak.
Now the modelling part is this. Devise a time dependent eucledian metric tha describes the increase in distance between train and platform at different time t
Another way to put this question is as follows: Suppose you are on the train and the train is preparing to leave. If you hop off the train at t=0, then the horizontal distance between the point you want to land on the platform and the starting point should be effectively zero (or some small number)
Do you mean "between a given point on the train and the platform"?
Because if you just want to reach the train it'll always be the same distance (supposing you don't miss the train).
Yeah, a fixed point on the train (where you jump off) and the point that you expect to land when the train just prepared to left the station at t=0. Inspired by missing a station, it makes me curious on what the effective geometry of the space look like the later you hop off the train
@Semiclassical good point
Observing the fact that the vertical distance increases in an accelerated manner as the train left the platform, I am trying to convert this scenario into a metric so that the vertical distance with time becomes a geometric structure like a grid
17:32
@GFauxPas It's a trade-off, of course. If you pick a network configuration which is truly optimal for the given set of computers, it may require a lot of 'fine-tuning'. That'll be a problem if you add/remove a computer, since that fine-tuning will be different for each configuration. But one has to be willing to make some adaptations if the circumstances change.
right
@Secret Could also work in the train's reference frame.
(one could even ask what this scenario would look like if you assume Lorentz invariance rather than Galilean invariance.)
I am guessing any coordinate grid of spacetime in the lorentz case will be contracting along the direction of motion
Another variation: Suppose that the train is passing by a wall and you throw a ball out the window.
If you throw it horizontally, I'd think it'd bounce back to you (assuming that the collision is elastic so that none of the kinetic energy is lost in the bounce)
The lorentz case I suspect will be very complicated, the Galilean case will have the ball flying horizontally in the train's frame but forming a v shape trajectory in the platform's frame (not sure how the grid of spacetime will look like for this scenario, though, which is one of the thing I am interested in)
The ultimate reason why I want to get a metric to describe the whole scenario in a "timeless" manner is because any metric will induce a topology, and inspired from me forget to alight at a station and observing the increase in distance from my destination as the train left with me still on the train, I am interested in how the topology between the pair of blue points changes with time as the train leave the station
It will be interesting if I can represent the motion from all reference frames of these two relatively moving objects as a "static" geometric object, so that the metric give me information on how distance between any pairs of points of interest will vary with time
17:44
Well, one should keep in mind that what will be the same in either the train or the platform's reference frame is the horizontal velocity of the jumper.
nor will the horizontal distance to reach the platform change. so the time $T$ spent in air isn't a function of the train's velocity.
But in the platform frame, the person is moving forward with the same velocity $u$ of the train. Hence they'll travel forward a distance $uT$ during that jump.
If I take the speed of the jumper to be $v$ and the distance to the platform to be $l$, then $T=l/v$. So they'll land a distance $ul/v$ forward from where they jumped.
If you ask for the total distance they travel in the platform's frame of reference, then that'll be $\sqrt{l^2+(l u/v)^2}=(l/v)\sqrt{v^2+u^2}=T\sqrt{v^2+u^2}$, which makes sense as that square-root is the magnitude of their velocity.
That expression looks familar, it so reminds of the lorentian metric in special relativity
So I am guessing we already have done something like that when in SR courses the minkowski metric is first introduced, usually motivated by consideration of light travel
18:03
Let vectors be $(x,y)$ and the Galilean metric for this scenario has signature $(+,+)$. Under the standard basis, the metric has coordinates:
$$\begin{pmatrix}Tv & 0\\0 & Tu\end{pmatrix}$$
where $T=\frac{l}{v}$
and in the case of acceleration of the train, we have in general:
$$\begin{pmatrix}Tv & 0\\0 & T\dot{u}\end{pmatrix}$$
Nice. suddenly metric become a lot more visual. Looks like accepting that the more accurate analogy of the expansion of the universe as distance between things literally increases without moving away from each other does help to visualise motion in terms of an array of time varying distances
18:24
Now I am starting to wonder, whether a metric of this form represents some kind of generalised comoving frame so that everything is rendered stationary relative to some box we draw in the scene, and whether it can always be found for any arbitrary motion
@Secret Are you using metric in some other meaning than the mathematical one? Because none of that looks like the metrics I know.
uh, semi and I have ran through the calculations above on determining how distances are measured between two points and from trigonometry we have found the expression of the distance and thus we canconstruct a metric on that by sqauring that expression and writing it in the standard basis as shown by the 2x2 matrix?
This guy should have d (x,y) > 0 d(x,y) =0 <=> v=0 and triangle inequality. But let me check that real quick...
@Secret I don't see how it gives you a number rather than a vector
Well, metric tensors are symmetric bilinear maps, thus two vectors can be fed into it and it spits out a scalar, which is the squared distance in this case
Let the vector be a=(x,y)=b under the standard basis) and let the metric tensor $\begin{pmatrix}Tv & 0\\0 & Tu\end{pmatrix}$ be $g(-,-)$
1. d(x,y) > 0 and $d(x,y)=0 \implies a=0=b$ holds as long u,v > 0 since $g(a,b) = Tvx^2+Tuy^2$ means (x,y) has to be positive or zero
Triangle inequality holds trivially since the outcome is the eucledian distance
18:44
I'm not paying too much attention right now, so don't expect me to weigh in :P
but there is indeed somehing very strange about this symmetric bilinear map: If u and v have values in other quadrants, it can potentially become indefinite
I suppose, however that it should be independent of basis transformation, though so it has the requirement of a metric tensor, which is a metric function
In conclusion, if u and v > 0 (which we can choose it to be so by picking a basis, which is the same as choosing a reference frame) then we have a metric tensor which give us a metric
19:13
Hello. In a rooted tree, is there any name for the rooted tree formed by the descendants of a node?
I think any subtree would have this property, no?
If you had more than one ancestor, it'd be disconnected, and thus a forest
You are right, thank you.
19:38
Hi, i need help about something;
i need to get an additional bank commission from my customers purchase but always im losing some money. if i sell $1000 item, i need to pay $10 to the bank(as a commission of credit card payment system. rate is x0.01 ) so if i add commission like (itemprice+itemprice*0.01), still bank gets more commission because last price is changin to (itemprice+itemprice*0.01)*0.01 and it continues forever. so are there any formulas to solve this issue easliy? I am very happy if someone can help. thanks.
19:51
@AjnaSarut what is the issue youre trying to solve?
@reuns I like say to you a thing about a previous comment where you are saying that you've no access to a paper of Michael Rubinstein (A Simple Heuristic...). But notice that if you search the article in Google you find it in JSTOR. An account MyJSTOR is for free, you can read up to 3 articles every 2 weeks (if you need any detail about it tell me or contact with the site). Maybe Michael's paper isn't interesting for you question, but this service of MyJSTOR provide you a large database.
Is not required a response of this message, good day.
:38883281 im selling some items. and im using a banks service to get money from customer in my website, as an example; im selling $1000 carpet, bank says i will get 0.01 of the price as a commission. so when i sell the carpet i get $990, and banks get $10. so i dont want to lose money. i need to get $1000. i tried to sell the carpet to $1010 but then bank gets $10.1. there are $100 and $100.000 products. so this lose is heavy with a $100.000 product. so i need a formula or an aproach to lose less money. but i cant figure it out.
maybe you want to know, "how much should I charge, to keep 100 dollars?
don't use dollar signs here, it messes up the TeX
okey, so how?
20:18
I'm saying you need to decide and write exactly what your question is
So you want ${99\over100}p= 1000$ ? (Where $p$ is the price)
One of the golden quotes from atop: "We can do calculus on R^n, but we want more. Now, we should know why we want more, for funding reasons. For instance, some people care about something called physics"
5
20:49
@Secret I don't know the context but I like this picture. I wonder if there's a notion of continuously deforming a metric space (in such a way that its homeomorphism class never changes).
Probably a special type of homotopy, of maps $X\times X/{\sim_{\rm cyc}}\to\Bbb R_+$ ($\sim_{\rm cyc}$ quotienting out by permutation)
(and no, $\sim_{\rm cyc}$ isn't a real notation, but it should be)
(That's probably not the best choice. I dunno)
Dumb question, but its late: Is a free and graded module a free graded module?
(asked differently: given a free and graded module, can I always find a basis of homogeneous elements?)
@Bubaya I don't think so, but my intuition is not very good here
@Bubaya Ahh, as usual the answer is already on the site math.stackexchange.com/questions/557402/…
@TedShifrin Mr. Shifrin, I will write the solution tomorrow. Best regards, Kirill
@TobiasKildetoft: Ah, thank you a lot. The statement of the reply indeed astonishes me.
How would you write the set of unordered pairs of elements of $X$? I'm thinking $(X\times X)/S_2$
Or like $X^2/S_2$
I mean, I'm sure there's no standard, but if you had to choose a notation
Above I suggested $X\times X/{\sim_{\rm cyc}}$ but that doesn't generalize to higher powers
Oh, there's a similar idea for vector spaces, right?
21:04
I think the notation for that is that of the symmetric space. $S^2 X$, maybe?
Is that even called the symmetric space? I think it has a name\
For vector spaces, $S^2(V)$ is like $V\otimes V/(v\otimes w-w\otimes v)$
Ok, it's "symmetric product"
$SP^n(X) = X \times \cdots \times X/S_n$ is the standard notation
@Akiva Yeah, the "symmetric algebra"
Hm, this gives the name $SP(X)$ to the "infinite symmetric product"
21:07
It's missing the index
I think the infinite symmetric product is the direct limit of all the SP^n(X)'s
It's kinda $X^\infty$ but all but finitely many entries have to be the basepoint, and you quotient by permutations
There's a theorem which says $\pi_k(SP(X)) \cong H_k(X)$
for a CW complex $X$
I'm not finding the notation $SP^n(X)$ online, but this 1931 paper by Borsuk and Stanislaw calls it $X(n)$
Thanks, by the way
$\text{Sym}^n(X)$ also seems popular
Oh I found an ncatlab page with it
Yeah thanks @BalarkaSen
21:11
No problem
In any case, I was wondering, @BalarkaSen
We could define a notion of continuously deforming metric spaces
in such a way that the *homeomorphism type never changes
homotopy type, you mean?
Like, a homotopy of maps $X\times X\to\Bbb R_+$ such that, at every instant, it's a metric space, and any two instants game the same homeomorphism type
@BalarkaSen Whoops. Homeomorphism.
Ok. We could, probably, yeah.
And then that gives us an equivalence of metric spaces
where you ask if you can deform one into (something isometric to) the other
and I guess the question is, is this a trivial equivalence?
21:16
Sounds like an interesting question. I doubt it.
Like, can you always do that for any two homeomorphic metric spaces?
I kinda feel like a circle and a knot, given the metric inherited from $\Bbb R^3$, might be a counterexample
Oh, wait, they're not.
Unknot them in $\Bbb R^4$ and give them the metrics inherited from there.
I can isotope them in R^3 x R right?
Dang, sniped.
I don't know what I should do first, try to prove it or look for counterexamples.
(I feel like there's a decent chance it's either trivially true or trivially false)
Also, I wonder if this is, like, what Ricci flow is
Or at least if this is related
Ya Ricci flow is a 1-parameter deformation of the Riemannian metric, but with some differential equation it's gotta satisfy
I think, at least
@AkivaWeinberger (*metric, not metric space)
*have, not game
Hm. Would each such deformation define a metric on $X\times I$?
Where, for two points with the same $I$-coordinate, you define it to be like the metric of the space at that instant
anf for two points with a different $I$-coordinate, you do… something, I dunno
Probably easiest to do a Manhattan-type thing
21:26
I want to extend your knot idea somehow. Are any two knots in a 3-manifold $M$ isotopic to each other in $M \times I$?
I don't think so.
Like, take the longitudinal circle in $S^2 \times S^1$ and a circle in a chart :P
But you could embed that manifold in some $\Bbb R^n$
and then unknot them there
Yeah fair.
(we can assume $n\ge4$)
@Balarka The only invariant should be the image in $\pi_1$
Barring that they are.
@PVAL-inactive That sounds super believable.
21:28
Is that a response to this discussion or something else @PVAL
it's a response to when two knots in $M$ are isotopic in $M \times I$
Oh, yeah, OK
Take an immersed cyllinder bounding them.
So I want something that embeds in $\Bbb R^n$ super-messily.
By transversality you can assume the intersections are isolated
21:30
Surely a very bad space is needed
So I think this is equivalent to asking if there's always a bigger metric space we can embed these in in which they are isotopic
now shorten the cyllinder a little and push off those intersection off the edge of the boundary.
The converse part of that is given by the stuff I said before, with the metric on $X\times I$ defined by the deformation
(Weird, "in in" ^)
Do you really get a metric on X x I
I believe so
though I need to elaborate on what "Manhattan-type thing" means probably
Wait
Can't we just average the metrics
$\lambda d_1(x,y)+(1-\lambda)d_2(x,y)$
We need to check that it satisfies the metric axioms
21:35
Isn't any positive linear combination of metrics a metric ?
Is it?
Does the triangle inequality work?
It should, shouldn't it
it does
Yeah OK
So it's true and kinda trivial
Wait
We also want to check that it preserves the homeomorphism type at every instant
should be true, because d1 and d2 give same homeo type
and we're just taking linear combination
We probably specifically want the identity map from $(X,d_1)\to(X,d_2)$ to be a homeomorphism
but I think we can assume that
I need to walk home
but it's probably some routine-ish calculation on open balls
21:40
What are we doing ?
Now I want to know the 1-homotopy type
aka does every loop of deformations starting and ending at $(X, d)$ "contract" to the zero loop?
whatever that means
I gotta run now. Have to travel 1843 kilometers.
Running ?
Good luck
I have to sleep 14 hours in 8 hours
Yeah, it does follow routinely
Hm, I have a new question
Say $(X,d_1)$ and $(X,d_2)$ both define the same metric space
and they both can be embedded in $\Bbb R^n$
Then can $(X,d_1+d_2)$ be embedded in $\Bbb R^m$ for some $m$?
Hm. $(X,\sqrt{{d_1}^2+{d_2}^2})$ can.
Speaking of which, $\sqrt{(\lambda d_1)^2+((1-\lambda)d_2)^2}$ would be another answer to the last question
22:10
Oh. No. Duh. Take $\Bbb R$ and $\Bbb R$ themselves.
You end up with the Manhattan metric, which can't be embedded in $\Bbb R^n$ for any $n$.
(Trying to remember the proof of the above fact…)
@BalarkaSen bill wurtz voice Time to fly through all of India
Most of India
22:32
Hey everyone!
hi Demonark, @Alessandro, DogAteMy
wonders how Astyx will do sleeping 14 hours in 8
How's it going @Ted and @Alessandro?
I've just been shopping and starting to cook. A former UGA colleague is here for a month and he and his family are coming for dinner tomorrow.
Where are you in complex analysis now, Demonark?
22:39
I'm on holiday, so quite well
Where on holiday, Alessandro?
I screwed up and slept through the lectures today
Woke up at like, 1:45
But in complex, today was Cauchy's inequality, Liouville, which I know, followed by Morera and some stuff on zeroes of an analytic function
At home, I just meant holiday as in "no exams nor lectures"
I'm sure you'll still do fine, Amin.
You're a smart lad.
@Dodsy I mean it's not like I'll get hit by a lightning bolt, more like, today was a day I was looking for to for the lectures since the two people were really good
(At least I don't think I'll get hit by a lightning bolt...)
22:43
Time to un-Balarka your sleep schedule, Demonark.
Hi, Nate!
Oh, ok, @Alessandro.
You should stay up a whole night to reset your schedule @Dami
I'll go to Tuscany in August probably @Ted
Hey Ted, how are you?
I get confused about "home" versus "school" for you, @Alessandro.
Good idea @Ted, might try @Alessandro's shtick
:(
I'm sorry about your misfortune, Daminark.
22:45
Yeah, I'm not using "holiday" properly, but after 2 months packed with exams that's good enough :P
Glad to hear that lightning will not strike you, any time soon.
My mom went to a native pow-wow and this shaman did a ritual on her and said that she would be safe for a single day.
Which I found funny.
Oh Morera is just that for continuous functions, Cauchy is iff
What's Cauchy's inequality?
Morera is actually very powerful.
But it's just the FTC in disguise.
In the proof I've seen it wasn't even a very good disguise
22:48
I like math.
@Alessandro Cauchy's inequality says that if $f(z) = \sum a_nz^n$, then $|a_n|r^n \le \max_{rS^1} |f(z)|$
Ah, ok, I didn't know it has a name
No, that's not right, Demonark.
Cauchy's inequalities are the bounds on the derivatives.
I mean, the $a_n$ would be derivatives, no?
Hi folks
22:51
Hey PVAL.
Well, multiples of them
But yeah I mean, that's what we had referred to as Cauchy's inequality
Can we construct a function on a not simply connected domain that has zero integral on every null-homologous chain yet it's not holomorphic?
Oh, I see. I've never seen it that way ...
I am always disturbed at seeing endless chains of theorems, most of them of no interest, and without any stress on the main points.
Good complaint, Nate. Some books don't motivate/explain what's important and what's meh.
Hi @PVAL.
@Alessandro: This is a local question, not a global one.
22:54
What do you mean?
@Ted Lol, I've checked Narasimhan and it mentions both ways of looking at it
As long as $f$ integrates to zero on every curve in a neighborhood of a point p, f is already holomorphic at p.
Topology introduces non-zero integrals that are zero locally.
If that makes sense to you.
I think I learned the stronger version of Morera.
where the assumption was only for triangles.
Yes, I've taught that version. Rectangles. Whatever.
22:57
I also found, especially in analysis books, that the way proofs of theorems are phrased can be, not in the way that you'd approach it
What books are you currently reading, Ted? For leisure or otherwise.
Nothing at the moment, although I have a small pile I should be.
As an example for which this is slightly less of a problem but still demonstrates it, proving that if $a_n \to L \ne 0$, that $\frac{1}{a_n} \to \frac{1}{L}$. The way you'd ideally present it is say okay, let's look at $|\frac{1}{a_n} - \frac{1}{L}| = |\frac{L - a_n}{La_n}|$. The numerator converges to $0$ and of course the denominator is bounded away from $0$!

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