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21:07
1
Q: Commensurability of Subgroups

user193319Let $G$ be some group, and let $S_1$ and $S_2$ be some subgroups. Then $S_1$ and $S_2$ are said to be commensurable iff $|S_1 : S_1 \cap S_2|$ and $|S_2 : S_1 \cap S_2|$ are finite. I am trying to show that this is an equivalence relation on the collection of all subgroups of $G$. Reflexivity an...

This problem has been giving me too much trouble...
All right guys, either I'm about to point out a glitch in the matrix or I'm extremely dumb
If I perform partial integration on $\operatorname{Li}_s(x)/(x+\alpha)$ for example, and I pick the polylog as the function I'm integrating in both terms, I get on the RHS the following
@Shaun Perhaps you got the point already, but I don't like either answer, since they don't seem to tell you what's really going on.
$$
\int \frac{\operatorname{Li}_s(x)}{x+\alpha} dx = \frac1{x+c_1}(-1)^s \left[x\sum_{i=2}^{s} (-1)^{i}\operatorname{Li_{i}(x) - (1-x)\log(1-x) -x\right] + \sum_{i=2}^s (-1)^{s+i} \int dx \frac{x}{\left[x+c_1\right]^2} \operatorname{Li_{i}(x) + (-1)^{s+1} \int \frac{1-x}{\left[x+c_1\right]^2}\log(1-x)dx +(-1)^{s+1} \int \frac{x}{\left[x+c_1\right]^2} dx
$$
Umm it's not formatting?!
An element of S_n may be written by partitioning {1, 2, ..., n} into smaller sets, and applying a cyclic permutation on each of them. This is usually written like (134)(256)(7), say.
The content compiles just fine in my tex editor:(
21:14
A cyclic permutation on k letters has order k, so we should understand what that says about products of cyclic permutations (where the sets they act on are disjoint).
@1010011010 see LaTeX in chat on the sidebar.
\begin{equation}
\int \frac{\operatorname{Li}_s(x)}{x+c_1} = \frac1{x+c_1}(-1)^s \left[x\sum_{i=2}^{s} (-1)^{i}\operatorname{Li}_{i}(x) - (1-x)\log(1-x) -x\right] + (-1)^s\int dx \frac1{\left[x+c_1\right]^2} \left[x\sum_{i=2}^{s} (-1)^{i}\operatorname{Li}_{i}(x) - (1-x)\log(1-x) -x\right]
\end{equation}
@MikeMiller Yeah thanks I know about that, there was just a bug in the code somewhere, I guess the other comment can be deleted
Gotcha
@Shaun Let me write some notation to simplify what I want ro say.
The above appears to have the same integral on both the RHS and LHS (just take the $i=s$ term of the summation under the integral sign on the RHS)
Does this automatically mean I cannot take the polylogarithm as the function to be integrated?
@Shaun Let $\sigma_1, \sigma_2, \cdots, \sigma_k$ be cyclic permutations on some subset of $\{1, \cdots, n\}$. We say that $\text{Supp}(\sigma_i)$ is the set of elements so that $\sigma_i(x) \neq x$. We demanded above that $\text{Supp}(\sigma_i) \cap \text{Supp}(\sigma_j) = \varnothing$ for all $i \neq j$.
(I am introducing notation instead of specifying the subsets because the latter would make the notation way more hellish.)
Now, let's say $|\text{Supp}(\sigma_i)| = s_i$. Then $\sigma_i$ has order $s_i$, and $\sum_{i=1}^k s_i \leq n$. We have equality iff none of the $s_i$ are zero.
Now, taking $(\sigma_1 \sigma_2 \cdots \sigma_k)^j = \sigma_1^j \sigma_2^j \cdots \sigma_k^j$. This is because the domains of these permutations are disjoint (so they all commute with one another).
Therefore, the order of $(\sigma_1 \cdots \sigma_k)$ is the least $j$ so that all of the $\sigma_i^j = 1$.
That is, the order of $\sigma_1 \cdots \sigma_k$ is the greatest common denominator of the orders of the $\sigma_i$.
The question "what are the orders of elements of $S_n$", then, is the same as "if $p = \{s_1, \cdots, s_k\}$ is some sequence of numbers with $1 < s_i$ and $\sum s_i \leq n$, what is $\gcd(s_1, \cdots, s_k)$? If we allow $p$ to vary over all partitions of numbers at most $n$, what are the possible numbers this produces?"
Then in those questions, people carried out this number theoretic calculation.
Mostly it is a matter of brute computation. The fact that $1 < s_i$ reduces the amount of computation somewhat.
In particular, if you want an element of order exactly 2n, the discussion in one of those posts shows that this cannot be any prime power n. This reduces us to 6, 10, 12 as our first possible examples.

It is not true of n=6: there the possible partitions as above are {2,2}, {2,3}, {2,4}, {2,2,2}. The gcds in each case are 2, 6, 4, 2: never 12.

For n=10, take the partition {5, 4}.
I do not see a good reason to star all of these. I'm going to remove every star but the first one (which I guess can serve as a marker to find this conversation later), unless somebody objects.
21:31
Sorry, just keeping track - I'll stop. Thank you for answering
No worries. BTW, there is a feature that lets you save conversations to check for later. But I am having trouble figuring out how to use it.
I was thinking about this problem over the last couple of hours (in the back of my mind). Partitions did occur to me. I don't think I could make my thoughts on it any more precise than yours, so, yeah, thank you.
I was pretty disappointed in those answers for not just saying this explicitly.
The annoying think with that feature is that they're not saved privately
Do you know how to use it? I can't find the button
Anonymous
21:35
FWIW, you can bookmark conversations from the transcript. You need to select the starting and ending messages. (Click on "bookmark a conversation".)
I used to know, let me see if I can figure it out again
I unfortunately only see the permalink button...
permalink | history
It's on the right, a blue button "bookmark a conversation"
See the Group Theory chatroom . . .
in Group Theory, 1 min ago, by Shaun
in Mathematics, 18 mins ago, by Mike Miller
@Shaun Let me write some notation to simplify what I want ro say.
Anonymous
21:36
And all bookmarked conversations can be seen in this tab‌​, which is what I don't like about this feature: it's public
OK, @Shaun, if you want you can go to the transcript (using Blue's link above), click a button on the right that says "bookmark conversation", and then choose the sequence of messages to be saved. As Alessandro said this will save it publicly for anyone to check back on if they want.
Anonymous
@AlessandroCodenotti Yeah, that's unfortunate. :/
I will leave up the first star from this conversation so that you can click that to return to the thread, if you want.
I don't mind people seeing conversations I bookmarked, but it makes them way harder for me to find than if I could have a tab on my profile or somewhere listing all the stuff I bookmarked
21:38
Yes, I don't really care to look through other people's bookmarks!
@MikeMiller That sounds like a great idea. I hope I can access it on the mobile site, though, as that's pretty much all I use; it's okay if not.
I mostly use mobile, and for a lot of featueres you need to quickly change to the full site to reach them. It's a hassle.
You can access it, but usually through a little bit of pain.
Anonymous
@AlessandroCodenotti The individual bookmarks have permalinks. So could save them in a local file (as a workaround).
@Blue There is a question in the associated chat you made, that you would have a quicker answer to than me. I didn't find the right thread in a half minute of googling.
Anonymous
I think someone had written a script to save individual bookmarks on the site itself (visible in a separate page). I'll let you know if I find it.
21:39
Sure, but I'm saving the permalink to the message starting the conversation I'm interested in in a local file directly instead
Nevermind!
Is there an element of order $80$ in $S_{20}$?
I'd like to have a hint please
@Eran what is the order of $(1~2~3~4~5~6)(7~8~9~10)(11~12~13~14~15~16~17~18~19~20)$? (don't worry it isn't 80)
Seems like you should read the above discussion.
lcm of it's cycle lengths
21:48
there you go
@Shaun the most recent comment makes me realize I mistakenly said "greatest common divisor" instead of "least common multiple" up above :P

Permutation on finite set

35 mins ago, 16 minutes total – 20 messages, 2 users, 0 stars

Bookmarked 8 secs ago by Leaky Nun

@Eran ^
So I should consider all possible partitions of 20 and then check it's lcm sounds like too much work
thanks
@Eran I'm sure you can come up with a better method
you probably don't need to think about literally every partition.
21:52
you don't need to think about any partition at all
Only partitions to primes maybe, this way ill minimize the gcd and maximize the lcm ?
idk
you're closer
also @Mike hi!
Is it true that $H^n_{dR}(M) = \Bbb R$ for smooth connected compact orientable $M$ of dimension $n$ just by Poincare duality?
without boundary
'just'
I mean...
"as a trivial corollary of"
yes of course
21:55
@LeakyNun Closer primes or closer gcd haha
?
@MikeMiller and then as a corollary that every top form that integrates to zero is exact?
that's not a corollary, that's the definition of what you just said
well, i guess you don't start with the integration functional at hand.
you still have to do a tad bit of work to show that $\int : H^n_{dR}(M) \to \Bbb R$ is surjective hence injective
but yes.
what's the dimension of the empty manifold? is it even a smooth manifold? and why on earth am I thinking about edge cases again?
21:58
the third question is the most important
also can this observation be generalized? "every vector field on R^2 that integrates to zero along every closed curve is the grad of some function"
the definition that makes dimension additive under product is $\dim \varnothing = - \infty$, the definition that lets you make sense of null-cobordisms as a cobordism from one manifold to another says $\dim \varnothing$ is whatever you want it to be today
@LeakyNun exercise
think about surfaces and de rham's theorem
I don't know de Rham's theorem
22:00
mild irritation in sufficiently large dimensions
meh
ok I googled
how do you find Whitney approximation? @MikeMiller
what does that mean?
Whitney approximation theorem: any continuous map between smooth manifolds is homotopic to a smooth map (or something like that)
do it in charts or use convolution
to do it in charts without using convolution appeal to stone-weierstrass
@loch!
22:06
@MikeMiller It happens t' best of us :)
Suppose we have a vector field $f : \Bbb R^3 \to \Bbb R^3$ that integrates to zero along the surface of every sphere ($S^2_{r,c} = r S^2 + c$). Let $g = \nabla \cdot f$. Divergence theorem says $\displaystyle \int_{B(c,r)} g = 0$, so $g = 0$, so $f$ is the curl of some function... @MikeMiller does this sound right?
sounds plausible
good argument
ok so I need to generalize this using de Rham's theorem
NOPE drop that last thing I said
more subtle in general as you observe
I mean this argument works for at most $n-1$ forms
the most straightforward generalization is a criterion for exactness for $n-1$ forms in $\Bbb R^n$
or actually more generally for closedness
I only used the cohomology being 0 for closed => exact
I drop that step and so I can generalize it
however de Rham's theorem talks about closed forms
22:18
@LeakyNun disagree, your argument will show that if $\omega$ is a $k$-form on $M$ that integrates to zero on every closed $k$-submanifold, then $d\omega = 0$
ok more generally it's a identity theorem
ok you sniped me
it's much the same except instead of determining that it's zero at every point you see that the value is zero on every k-plane
hmm
yeah I realized Stokes theorem isn't the crucial (i.e. new) step
it's the identity theorem bit
@MatheinBoulomenos!
i do not know what the identity theorem bit means
i.e. a criterion for a function to be zero
22:20
hi @LeakyNun
I... copied the name from the "identity theorem" from complex analysis
@MatheinBoulomenos we're discussing (i.e. I'm thinking about) how to generalize the observation that any 2D vector field that integrates to zero along any closed curve is a grad of some function
i really disagree with that choice of notation
your deleted comment was on the right track, in some sense - this is a two-part problem
and what you described is part 1
wait what did I say?
ah I said it needs to be a boundary
that was when you were talking about integrals over bounded manifolds
that gives you $d\omega = 0$
also, i can see every deleted comment now
:O
oh right...
22:24
the raw power courses through my veins
@MikeMiller and is there a name to the thing we found?
what thing did we find?
well... if something integrates to zero along any closed submanifold then it's zero
you have not proved that yet
you have proved that if something integrates to zero along any closed submanifold, then $d\omega = 0$
this is probably best known as "exercise left to the reader", whose proof you supplied above
Could you please master tell me an example of a PID which is not Euclidean domain besides $\mathbb{Z}\ [\frac{1+\sqrt{-19}}{2}]$?
22:32
it would be pretty silly if that was the only PID which wasn't a euclidan domain, wouldn't it
the full statement is best known as 'the de rham theorem', but actually proving it requires extra technology I will point out once you write a proof with a hidden subtlety
until I see a near-proof I will stay quiet
@Mi
@MikeMiller
by near-proof you mean near-proof of de Rham's theorem?
near proof of the statement "if $\omega$ integrates to zero on every closed oriented submanifold of appropriate dimension, then $\omega$ is exact"
ok let's see...
@Eran $\Bbb{Z}[\frac{1+\sqrt{-44}}{2}]$, $\Bbb{Z}[\frac{1+\sqrt{-67}}{2}]$, $\Bbb{Z}[\frac{1+\sqrt{-163}}{2}]$
22:36
@MatheinBoulomenos did you google that?
@MatheinBoulomenos what's with this form?
@LeakyNun I knew that there were more among ring of integers of imaginary quadratic fields, but I had to look up the exact numbers, yeah
rings of integers of the field $\Bbb Q(\sqrt{n})$, where $n \in \Bbb Z$, are always of the form $\Bbb Z[\sqrt{n}]$ or $\Bbb Z[\frac{1+\sqrt{n}}{2}]$ depending on parity
-163 is a famous one though
@MatheinBoulomenos then you should have told him to google
depending on whether $n \equiv 1 \pmod 4$ @Mike
Why didn't you tell me to gooogle yourself licky noun?
22:38
I like licky noun
Lmao
everyone loves licky noun
thanks, @LickyNoun, I remembered it was something mod 4 but not the precise condition (so parity was the wrong word to use! I should have said depending on a congruence condition)
hahahah awesome, licky noun you're the smartest guy here
even smarter than the owner of the room
Let $\eta = \mathrm d\omega$. Suppose $\eta_p \ne 0$. Let $x : U \ni p \xrightarrow\sim \tilde U \subseteq \Bbb R^n$ be a chart, and then WLOG suppose $\eta_p > 0$ (otherwise look at $-\eta$). Pick $\varepsilon$ such that $\eta|_{B(x(p),\varepsilon)} \ge \varepsilon/2 > 0$. Integrate $\omega$ along the boundary of a ball with appropriate dimension to get a contradiction @Mike
22:42
Sorry, you just keep showing that $\omega$ is closed
You want to show that it is exact too
oh wait what
that was your goal
that's... interesting
For determining half-lives of radioactive isotopes, it is important to know what the background radiation is in a given detector over a specific period. The following data were taken in a γ -ray detection experiment over 98 ten-second intervals:
               58 50 57 58 64 63 54 64 59 41 43 56 60 50 46 59 54 60 59 60 67 52 65 63 55 61 68 58 63 36 42 54 58 54 40 60 64 56 61 51 48 50 60 42 62 67 58 49 66 58 57 59 52 54 53 53 57 43 73 65 45 43 57 55 73 62 68 55 51 55 53 68 58 53 51 73 44 50 53 62 58 47 63 59 59 56 60 59 50 52 62 51 66 51 56 53 59 57
Assume that these data are observations of a Poisson random variable with mean λ.
(a) Find the values of x and s2.
it's the verbatim generalization of your original claim!
22:44
Is there a way to find $x$ bar and $s^2$ without using a calculator?
well I would need some global lemmas... since every closed form is locally exact
I have said the name of the relevant theorem a few times
oh sorry
I am not asking you to prove that theorem - I am asking you to see that what we want is (almost) a quick corollary of it
I'm a bit slow
22:45
Nothing to be sorry about
If I was frustrated I probably would have stopped talking a while ago :D
I do need Whitney approximation though don't I
I mean, I need it to even state the de Rham theorem
whatever
@LeakyNun do you?
so we know that $\omega$ is closed. Consider the corresponding element $W \in \operatorname{Hom}(H_p(M;\Bbb R), \Bbb R)$ that sends $[c]$ to $\displaystyle \int_c \omega$. By hypothesis that integral is zero, so $W = 0$, so $W$ is exact, so $\omega$ is exact
@MikeMiller because otherwise $\int_c \omega$ makes no sense
Pullback on charts + partitions of unity, no?
he's saying that $c$ is a continuous simplex
but usually the de Rham theorem is stated for the chain complex of smooth simplices
and it is a lemma that the inclusion of this into the chain complex of continuous simplices is a homology iso
(indeed, a Whitney-type result)
22:51
how's my near-proof?
@LeakyNun what is $c$, precisely? I am skeptical of the phrase "By the hypothesis, that integral is zero"
It's the right idea but will need a little nudging
$W$ sends $[\sum a_i \Delta_i]$ to $\sum a_i \int_{\Delta_i} \omega$
I hope $\Delta_i$ is orientable
22:53
... is it a theorem that only taking injective simplices gives you the same homology groups?
doubt it
iirc akiva asked about that once
this is not good
don't worry about injectivity right now too much
pick an atlas, do barycentric subdivisions, do everything locally, boom
you can replace the statement with "if for every smooth map $f: N^k \to M$ from a closed oriented $k$-manifold to $M$, $\int_N f^*\omega = 0$
where is the submanifold, in the end? why don't these simplices meet (say) orthogonally at the boundary?
(you are seeing the point! the injectivity comment was good)
22:56
I mean, if I do barycentric subdivisions enough times, all of my smaller simplices fall inside one of the charts
why does that help?
so I can do everything locally
can I use your strengthened hypothesis?
sure, but I don't see how this helps you find a closed manifold with boundary
I don't actually know how you define $\int_{\Delta_i} \omega$ to start with
smooth simplices, as above
(can you prove the desired result for surfaces?)
22:58
so we're pulling it back?
yeah
which is the same as your barycentric subdivision idea
since restriction to a chart == pullback
I don't know if this is what you're looking for, but $\Delta_i$ is the closed manifold (without boundary)?
what is the boundary of a simplex?
more simplices?
of a triangle? of an interval? :p
yeah, it's not closed
sorry, is the issue in my terminology 'closed'? that is topologist language for compact without boundary
22:59
oh that's what you mean
homotope the simplex to a sphere locally
you can't do that for one simplex at a time - you need all the boundaries to cancel out
or your $c = \sum a_i \Delta_i$ is not a cycle
(If you get frustrated, let me know and I will say the point - I am enjoying the nudging)
ok I need some notations to tell apart the simplex and the image of the simplex
let's say $c = \sum a_i f_i$ where $f_i : \Delta^k \to M$
really strongly suggest thinking about oriented surfaces to start
that case you can prove (I think, I am not sure what calculations you know) and you will see the issue in general
I need to show that $\displaystyle \sum a_i \int_{\Delta^k} f_i^\ast \omega = 0$ right?
yeah, what is your idea/approach?
23:03
so my idea is that WLOG (barycentric subdivision) suppose that $f_i(\Delta^k) \subset U_i$
where $x_i : U_i \xrightarrow\sim \tilde U_i \subseteq \Bbb R^n$ is a chart
For determining half-lives of radioactive isotopes, it is important to know what the background radiation is in a given detector over a specific period. The following data were taken in a γ -ray detection experiment over 98 ten-second intervals:
58 50 57 58 64 63 54 64 59 41 43 56 60 50 46 59 54 60 59 60 67 52 65 63 55 61 68 58 63 36 42 54 58 54 40 60 64 56 61 51 48 50 60 42 62 67 58 49 66 58 57 59 52 54 53 53 57 43 73 65 45 43 57 55 73 62 68 55 51 55 53 68 58 53 51 73 44 50 53 62 58 47 63 59 59 56 60 59 50 52 62 51 66 51 56 53 59 57
shoot, i have 10 minutes left - tell me your idea and then I will sketch what I have been thinking
@MikeMiller Hello. Long time no see.
@MikeMiller and then I need to prove $\displaystyle \sum a_i \int_{\Delta^k} f_i^\ast \omega = 0$ for the new $i$
23:05
and then since each $\Delta^k$ falls inside $\Bbb R^n$, I can homotope them to spheres
and the integrals should be the same
the issue is that when you do that, you move the boundary of each simplex - when you perform your homotopy, you need to do it on all simplices at once, so that at each stage of the homotopy $\partial c_t = 0$
(where $c_t$ means the cycle you get by performing your homotopy along all the simplices up to time $t$)
otherwise $\int c_0 \neq \int c_1$, or at least you can't prove that
hi yall
ok what's your idea then?
none leak , I just came in
let me clarify the situation for surfaces first
$H_1(\Sigma_g; \Bbb Z) \cong \Bbb Z^{2g}$, each factor generated by a certain loop
assuming $\int_M \omega = 0$ for every smooth submanifold $M$ of $\Sigma_g$, we see therefore that the map $\int \omega: H_1(\Sigma_g;\Bbb Z) \to \Bbb R$ is identically zero - it vanishes on the generators
and therefore, we may apply de Rham's theorem
now the way one should really think of $H_k(M)$ (imo) is that elements are "bordism classes" of "singular" manifolds, where the singularities arise in codimension 2 - I have written about this a few times before, and this is certainly how Poincare was thinking in the early 1900s
23:10
5
A: invariance of integrals for homotopy equivalent spaces

Kevin CarlsonYour expression doesn't make sense. If $\omega$ is a form on $\Sigma$, then it's not a form on $\Sigma'$! You need a map $f:\Sigma'\to \Sigma$ to compare them. So a better version of your claim would be $\int_{\Sigma'} f^*\omega=\int_\Sigma\omega$ when $f$ is a homotopy equivalence. This is now f...

> Theorem If $f,g:\Sigma'\to \Sigma$ are homotopic maps and $\Sigma'$ a smooth $k$-manifold and $\omega$ a closed $k$-form on $\Sigma$, then $\int_{\Sigma'}f^*\omega=\int_{\Sigma'}g^*\omega.$
to be clear, Kevin is being lazy and means that $\partial \Sigma ' = \partial \Sigma = \varnothing$
now there is a big question - what classes of $H_k(M;\Bbb Z)$ may be represented by submanifolds?
this was a big question in the 50s and 60s, and there are examples where homology classes cannot be represented by submanifolds, or even by smooth maps from a smooth manifold
@LeakyNun Do you know why {1/n} does not converge in the metric is all the positive reals?
that is not a metric
with d(x,y) = |x-y|
why not
it doesn't converge because it would have to converge to 0
but 0 is not a positive number
recall that "converge" means "there is a point that it converges to"
it is an existence proposition
23:13
so what I have to tell you is that to get the final result you need a big machine ;) Thom proved in the 60s via cobordism theory that every class of $H_k(M;F)$ can be represented by a smooth manifold if $F = \Bbb Z/2$ or if $F = \Bbb Q$
since when converge to an element is required that the elemnt is in the set?
The latter is enough. While we start with a functional $H_k(M;\Bbb Z) \to \Bbb R$, it clearly factors through $H_k(M;\Bbb Q) = H_k(M;\Bbb Z) \otimes \Bbb Q$
aint this like limit ?
in fact we use the same notation
well in limit you worked in $\Bbb R^n$ presumably
and since this group does have manifold representatives for every class, we see that the integration functional vanishes here
23:14
(or worse, just $\Bbb R$)
where this issue doesn't occur
but more generally your limit point needs to be inside your set
our sequence is always positive
(I did not expect you to come up with this, of course; I thought it would be a good idea to struggle with it for a bit so as to see where the many issues come in)
okay thanks
because points outisde the sets do not exist in the point of view of the set itself
I really liked when you caught the injectivity problem
23:14
it doesn't even know that 0 exists
seems fair as a point
@MikeMiller thanks :)
but we never did it that way
because you only did it for $\Bbb R^n$
where this issue doesn't occur
23:17
and Cauchy noticed that at least in $\Bbb R^n$, an equivalent way of formulating that the statement "$a_n$ converges" without referring to any point of convergence
is that the sequence is, what we today call, Cauchy
however this "Cauchy implies converges" is unfortunately false in general metric spaces
for example in the space of positive reals as you've seen
cauchy converge is the better criteria
it does not care what happen in the "end"
only at certain concecutive points
cauchy was a genius :D
but, the upshot is, that you can complete any metric space to get a new metric space where every Cauchy sequence converges
cool stuff
so the statement is that for any metric space $(X,d)$ there is a metric space $(\overline{X}, \overline d)$ and a continuous injection $f : X \to \overline X$ with dense image and that commutes with the metric, such that every Cauchy sequence in $\overline X$ converges
and for the case of $\Bbb Q$ with the usual metric it gives you $\Bbb R$ with the usual metric
(please, can someome verify)
2
Q: What is the Cauchy completion of a metric space?

Jalil CompaoréI was wondering what the "Cauchy" completion of a metric space is. I can't find any helpful information on Google. Feel free to post any links to sources you find relevant.

the answer that is not accepted is surprisingly nice
there's a universal property with the Cauchy completion
in fact it has quite some analogy with the case of algebraic closure
if $i_1 : K \to L_1$ and $i_2 : K \to L_2$ are field homomorphisms such that $i_1$ is algebraic and $L_2$ is algebraically closed, then there is a field homomorphism $L_1 \to L_2$
if $f:(X,d_X) \to (Y,d_Y)$ and $g:(X, d_X) \to (Z,d_Z)$ are continuous isometries such that $f$ has dense image and $(Z,d_Z)$ is complete, then there is a continuous isometry $(Y,d_Y) \to (Z,d_Z)$
and furthermore, given $i : K \to L$ such that $L$ is algebraically closed, we can construct an algebraic closure of $K$ (one that is both algebraic and algebraically closed) as the integral closure of $i$
and furthermore, given $\varphi : (X, d_X) \to (U, d_U)$ such that $(U, d_U)$ is complete, we can construct a completion of $(X, d_X)$ (one that both has dense image and is complete) as the closure of (the image of) $\varphi$
I see I'm being ignored by @KasmirKhaan
23:36
@LeakyNun No no sorry, was reading my book
@LeakyNun thanks for the answer, I only wanted basic answer for the moment , still not there in the reading material
23:49
@AkivaWeinberger you might be interested in this: so there's this age-old problem of "how many times in 12 hours do the hour hand and the minute hand overlap?" and it corresponds to counting the number of intersections of the (12,1) knot and the (1,1) knot around the torus: so given coprime pairs (p,q) and (r,s) what is the number of intersections of the (p,q) knot and the (r,s) around the torus?
"the (4,1) knot and the (1,1) knot intersects 3 times"
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