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12:30 AM
So, an "absorber" is defined an element $a$ of a magma $M$ satisfying that $am=ma=a$ for all $m\in M$. Obviously, you can only have one absorber per operation on the object, but is there a concept of a "second order absorber?" Ie an element $b$ satisfying that $bm=mb=b$ for all $m\neq a$?
 
You mean an absorber that absorbs all but another absorber?
 
Yes, almost exactly. I'd say give each absorber a "weight" and the one with the lowest weight wins when they are combined.
 
I don't expect there to be a name for that
Are you looking for an example?
 
I'm wondering if it's a topic that anyone has studied, or if there are any interesting facts related to them.
 
1:05 AM
If an nth order absorber is two sides, it is also unique
however there isn't a name for these things because the algebraic structure is basically a magma with absorbers extended with some extra elements that does not get absorbed
you still cannot define division or in any way invert such absorbers though because absorbers often means there is some noninjectvity going on
A special cases where you have a hierarchy of "nth order absorbers" is a semilattice, where ab=b if max(a,b)=b
 
2:00 AM
Hi! At end end of a proof I saw this:
Exercise. See if you can refrain from translating this proof into
cohomology. - Does this mean, see if you can think of a proof which doesn't use any machinery from cohomology directly?
 
 
4 hours later…
5:46 AM
@Rithaniel Kinda like how addition works with infinite cardinals?
(Actually - does $X+X=X$ rely on the axiom of choice?)
(I suppose it doesn't work for Dedekind finite sets...)
(And $\aleph_\alpha+\aleph_\alpha=\aleph_\alpha$ seems like a consequence of how ordinals work.)
Revision: Kinda like how addition works with aleph cardinals?
 
6:01 AM
en.m.wikipedia.org/wiki/Cardinal_number#Cardinal_addition says “Assuming the axiom of choice”
 
 
3 hours later…
9:18 AM
Does this Math chat answer statistics questions?
 
9:59 AM
> "The essence of calculus, perhaps, is that an infinitely accurate approximation is no longer an approximation."
 
10:19 AM
@PrashinJeevaganth yes
@AkivaWeinberger inb4 Fabius function
 
@PrashinJeevaganth It depends on whether there's anyone around who knows statistics
which could just depend on who's online
 
 
1 hour later…
11:52 AM
Hmm, http://itarget.com.br/newclients/sbgg.com.br/informativos/28-12-18/5%20Exercise%20type%20and%20activities%20of%20daily%20living%20disability.pdf

This is a research article that talks about finding an association between exercise and disability. I was thinking whether if u reject a null hypothesis: There is no association between exercise and disability for a given population, and perform a 1 tail test(idk if I'm right judging from the context of this article Figure 3), so your alternative hypothesis will be There is a negative association between exercise and disability. If we reject
 
Determine all ring elements that are both nilpotent elements and
idempotents.
I think only such is zero element
because $a^n=a$ for all $n>0$. Am i right?
 
12:18 PM
yes
 
thank you! and on the same line of reasoning, we see that 1 is the only element that is both unit as well as idempotent in commutative ring with unity?
right?
 
12:47 PM
Hi! At end end of a proof I saw this:
Exercise. See if you can refrain from translating this proof into
cohomology. - Does this mean, see if you can think of a proof which doesn't use any machinery from cohomology directly?
 
1:00 PM
@Silent yes
@KonformistLiberal yes
 
1:17 PM
reddit is down :c
 
@LeakyNun But it says refain from translating, not try to translate it
 
well more context would help
or you could just follow your heart
 
1:38 PM
Elements in $\Bbb{Q}[\sqrt{2},\sqrt{3}]$ are of the form $\sum_{i,j=1}^k a_{ij} (\sqrt{2})^{n_i} (\sqrt{3})^{m_j}$ for $a_{ij} \in \Bbb{Q}$ and $n_i, m_j \in \Bbb{N}_0$, right?
I'm trying to show that $1,\sqrt{2},\sqrt{3}, \sqrt{6}$ span the space.
 
yes
 
2:11 PM
How do I argue that $\sum_{i,j=0}^k a_{ij} (\sqrt{2})^i (\sqrt{3})^j$ is spanned by $1, \sqrt{2}, \sqrt{3}, \sqrt{6}$? I can split the sum like $\sum_{i,j=0}^k a_{ij} (\sqrt{2})^i (\sqrt{3})^j = \sum_{i=0}^k a_{ii} \sqrt{6}^i + \sum_{i \neq j}^k a_{ij} (\sqrt{2})^i (\sqrt{3})^j$, but I don't think it makes things any clearer.
 
Try splitting up your sums over I and j into even/odd parts?
 
@user193319 Hint: write $(\sqrt2)^{35}$ in terms of that basis
 
2:29 PM
My book says:
"If a function $f(z)$ is analytic on a bounded domain $S$ and continuous and nonvanishing on the boundary of $S$, then $f(z)$ can
have at most finitely many zeros inside $S$."
From above observation, it also follows that an entire function in any bounded part of the complex plane can have only a finite number of zeros.
I can't understand how latter follows from former.
 
2:50 PM
they both follow from the more "general" theorem that the limit points of the zeroes of a holomorphic function is relatively clopen
@KonformistLiberal you're right
 
3:41 PM
@AkivaWeinberger $(\sqrt{2})^{35} = 131072 \sqrt{2}$...I'm not sure I see how that helps with the general case.
 
@user193319 I'd put Akiva's hint differently: Compute the first few powers of $\sqrt{2}$ and see what you get
in particular, consider what you get in relation to the basis {1,sqrt(2),sqrt(3),sqrt(6)}
 
Basically you just need to show that $(\sqrt2)^i(\sqrt3)^j$ can be written in terms of that basis for all $i$ and $j$
 
(personal compulsive habit: editing my statements here so that they fit onto one line)
bleh, trying to write up an abstract for a talk
 
None of these fit into one line
 
@AkivaWeinberger yes, it's pretty silly when you consider the mobile chat
but that's not the view I'm seeing, soooo :P
(and actually the issue is not so much "more than one line" as "a line consisting of one word")
 
3:46 PM
"Everthing is relative" - Albert Einstein
 
ask me about the math i'm working on, and I'm happy enough to say it
ask me to say what I'll be talking about? urgghhh
 
anyone know any good books on functional analysis?
 
I like Rudin's book.
 
Thank you. Is there a consensus on this book, or is it purely your personal preference?
 
Rudin's books on analysis are generally highly regarded.
 
3:50 PM
Newtonian gravity is the limit of general relativity as $c\to\infty$, yeah?
 
Oddly, I feel like his book on functional analysis is a little bit gentler than his real and complex analysis book; but you do need to know a fair amount of general topology.
 
@AkivaWeinberger That seems like a poor description of it, but as someone who doesn't do GR I'm not qualified for the question

 The h Bar

General chat for Physics SE (physics.stackexchange.com). For M...
ask there instead :P
 
i don’t like how concisely sobolev spaces are treated in rudins functional book
 
@JoeShmo If I were you, though, I would just study operator algebra and pick up the functional analysis you need as you go along, because operator algebras is the coolest branch of mathematics (specifically von Neumann Algebras and $C^*$-algebras)
 
@user193319 i was going to say. his real analysis book is a classic, but people are more cautious to praise his complex analysis book. thats why im asking about the functional analysis book
gentler in what sense?
rudin's real analysis is pure joy. haven't read his complex analysis book
 
3:59 PM
He doesn't have a separate complex book.
Real and Complex are together.
Are you thinking of Royden?
@JoeShmo
 
@LeakyNun What do you meant by relatively clopen?
 
clopen in the domain
 
ok
 
Am I being a knucklehead, or is it difficult to show that $1,\sqrt{2},\sqrt{3},\sqrt{6}$ are linearly independent in the $\Bbb{Q}$-vector space $\Bbb{Q}[\sqrt{2},\sqrt{3}]$?
 
Well, if it were false, you'd have $a+b\sqrt{2}+c\sqrt{3}+d\sqrt{6}=0$ for rational $a,b,c,d$
Hmm.
 
4:24 PM
Hmm indeed.
 
Yuck, rationals.
 
5:13 PM
@user193319 my guess is that, since you're using relatively few roots, there's probably a reasonable if tedious way to show by hand that they're linearly independent
but the fact that 2,3,6 are not pairwise relatively prime seems to kick out the proofs I've seen so far online
 
@user193319 I'd show that $\{1,\sqrt{3}\}$ is a basis of $\Bbb Q[\sqrt{2},\sqrt{3}]$ over $\Bbb Q[\sqrt{2}]$ and that for tower of finite extensions you can just multiply the bases pf the intermediate extensions together to get a basis of the biggest one
 
definitely above my head
field extensions is where my understanding of abstract algebra peters out :P
 
 
1 hour later…
6:21 PM
Rudin's real and complex analysis is widely considered a good book for the subject, right?
 
Meh.
I'm not sure it's a widely used text for separate courses, which is what most universities offer. However, it is carefully written and it's nice to have a text that treats the two courses in tandem (sort of like the rarity that is an integrated text at the undergraduate level in linear algebra and multivariable calculus/analysis — which also go very naturally together).
 
That's a nice reason
I was just looking over it today and liked how "complete" it was
 
6:43 PM
hi chat
@TedShifrin looks like I'll be giving a talk for the math-physics seminar in the math department in a month
so that's neat
 
Hi everyone
 
Hey y'all
 
I know a method of finding $\int_0^\infty \frac{\sin u }{ u} du$ but how to proceed for $\int_0^\infty \frac{\sin^2 u }{ u^2} du$
oh double integral?
 
No, that's not really going to help
@jeea But what is your method for finding the first integral?
 
@Semiclassical I use the property of laplace transform $\int_0^\infty \frac{f(u)}{u} du = \int_0^\infty L\{f(u)\} ds$
 
6:56 PM
If you can find the first one, then just use trig to change the numerator, then you get two pieces, one which you integrate easily, the other which you integrate by parts and breaks down into your first integral.
 
Well, when I see a product of functions like that, what I immediately think of is the convolution theorem
And since you're using the Laplace transform, that still seems like a good idea
Namely, if $h(t)=(f\star g)(t)=\int_0^\infty f(\tau)g(t-\tau)\,d\tau$, then $H(s)=F(s)G(s)$
Not totally sure that's going to help here tho
I guess another line of attack is to write $\sin^2 u = \frac12 (1-\cos \frac{u}{2})$
 
U mean $\cos(2u)$
 
yeah, you're right. I knew that looked wrong
 
integrate $\cos^2(x)/x^2$ by parts so that you get something in terms of your other integral.
 
I guess another thing to try is to write $g(u)=\frac{1}{u}\sin^2 u$
So then you can write $\int_0^\infty \frac{g(u)}{u}\,du = \int_0^\infty G(s)\,ds$
bleh, ignore me, I'm not going anywhere
 
7:05 PM
ya don't ignore me :(((((((((
 
@anakhro Yes I try your method also! but what to do with the term $\frac{1}{u}|_{0}^{\infty}$
 
cry, maybe
 
But, more seriously
 
I guess that doesn't exist.
So my solution is bunk :(
 
7:09 PM
Let me just follow by ear for a moment. If we can manage to compute the Laplace transform $F(s)=\int_0^\infty e^{-s u} \frac{\sin^2 u}{u^2}\,du$
Then $F(0)$ will be the result we're looking for.
So we want to Laplace transform $u^{-2}\sin^2 u$.
To move things along, I'll first use the following result: The Laplace transform of $g(u)/u$ is given by $\int_s^\infty G(s')\,ds'$ where $G(s)$ is the Laplace transform of $g(u)$
So that pushes the problem to finding the Laplace transform of $g(u)=u^{-1} \sin^{2}u$
Applying that result again, we get $G(s)=\int_s^\infty H(s')\,ds'$ where $H(s)$ is the Laplace transform of $\sin^2 u$
 
If we find fourier integral of $f(x)$ defined as $x$ for $0<x<1$ and 0 elsewhere and compute $f(1)$ using $\frac{f(x^+)+f(x^-)}{2}$ we will get $sin^2u/u^2$ integral as $\pi/2$ but I needed to verify using other method ...
 
But $\sin^2 u =\frac12 (1-\cos 2u)$, so its Laplace transform should be $$H(s) = \frac12 \left(\frac{1}{s}-\frac{s}{s^2+4}\right)=\frac{2}{s(s^2+4)}$$
So we deduce $$F(0)=\int_0^\infty \int_s^\infty H(s')\,ds'\,ds = \int_0^\infty \int_s^\infty \frac{2}{s'(s'^2+4)}\,ds'\,ds$$
In which case we do have a double integral. Real question, of course, is whether this is any more tractable than what we started with :/
I guess since $H(s)=\frac12 \left(\frac1s-\frac{s}{s^2+4}\right)$ we have $$\int_s^\infty H(s')\,ds' = \left[\log s-\frac12 \log(s^2+4)\right]_s^\infty=\frac12\log(s+4/s)$$
So then we're just left with $\int_0^\infty \frac12 \log(s+4/s)\,ds$...yuck
meh, that integral was wrong.
 
Yes I think it diverges
 
Well, the actual one doesn't
I just did it wrong :p
 
@Semiclassical I think earlier hint is best, integration by parts we will get
 
7:22 PM
$$\int_s^\infty H(s')\,ds'=\frac12\left[\log s'-\frac12\log(s'^2+4)\right]_s^\infty$$
 
$\frac{\sin^2u}{-u}|_{0}^{\infty}+\int_{0}^\infty \frac{\sin 2u}{u} du$
 
Yeah, that's a good thought
since that at least makes sense as $u\to 0$
 
Ovi
Hello
 
@Semiclassical @anakhro thanks a lot, also semiclassical ill try the laplace way
 
good luck
sounds like you're well on your way
 
Ovi
7:27 PM
Sorry to interject, but does anyone know a software which I can use to help visualize complex functions? Like maybe input a path or a region of the domain, and have it show that image of that path/region?
 
The integral you end up with my way is $\frac 14 \int_0^\infty \log(1+4/s^2)\,ds$, btw
Which...neat? But not exactly trivial :P
Probably integration by parts does the trick
@Ovi Simplest solution I can think of is mathematica, since what you're describing amounts to a parametric plot
i.e. you express z=x+i y parametrically, and then do a parametric plot of (u,v) where u=Re f(z) and v=Im f(z)
@Ovi also, do you have a specific example of what you'd like to see visualized?
 
Ovi
@Semiclassical Thanks! But do you know of any free software that I could use? I don't have any specific example right now, I think I would just benefit from playing around with it.
 
Not really. But that's just a failure of imagination on my part, I'm sure it's out there
 
Ovi
@Semiclassical Alright thanks! I'll keep looking
 
Is there a name for a field with an inner product?
Let me rephrase: is there a name for an inner product space with a "multiplication" operation?
I know that a linear space with a "multiplication" operation is called an algebra.
I know that a normed linear space with a "multiplication" operation is called a normed algebra.
etc.
 
Ovi
7:40 PM
What other multiplication is there other than the inner product?
 
I guess I mean multiplication in the algebra sense.
I want an algebra with an inner product, in other words.
 
Ovi
Hmm I don't know sorry
 
@Ovi do note that any software which allows you to make parametric plots should suffice, on the grounds that I previously articulated
 
8:01 PM
Question: Given an isomorphism between $R$ and $S$, how would you construct an isomorphism between $R^{op}$ and $S^{op}$ out of it? I first thought of trying $f(a+b)=g(a+b)$ and $f(ab)=g(b)g(a)$ but that seems to be causing issues.
 
8:23 PM
What are the definitions of those?
Rings?
 
Yeah, rings. $R^{op}$ is the opposite ring of $R$. So the additive group is the same, but if $\circ$ is the multiplicative operation of $R^{op}$ then $ab=b\circ a$.
 
Gotcha
what I notice is that $b^{-1}\circ a^{-1}=(a\circ b)^{-1}$
Or $b\circ a =(a^{-1}\circ b^{-1})^{-1}$
 
Ovi
@Semiclassical Yup got it, thanks!
 
I wonder if there’s a way to use that
 
Hmmmm, so $ab=(a^{-1}\circ b^{-1})^{-1}$. Maybe I can do something with showing that if $R$ and $S$ aren't isomoprhic then $R^{op}$ and $S^{op}$ cannot be isomorphic?
 
8:29 PM
Well
Preferably you’d display an actual iso
 
If an isomorphism cannot exist then either there is a cardinality mismatch or a structure mismatch. Cardinality obviously carries over. The fact that structure also would be carried over in a way is obvious on the surface, but tricky to show.
If an isomorphism exists then attaining an "opposite" isomorphism from that isomorphism should be possible.
 
@user193319 I am clearly thinking of baby Rudin :-) Principles of Mathematical Analysis. A marvelous book.
 
It feels like it should just be a quick thing to switch, but if $f(ab)=g(b)g(a)$ then my efforts end up showing that $f(ab)=f(b)f(a)$, which means that it's an anti-isomorphism, if anything.
 
The notation here isn’t helping
Maybe try this. Instead of writing products implicitly, do so like this: the product of a,b in the ring R is $(a,b)_R$
Similarly for S
Then $(a,b)_{R^{op}}=(b,a)_R$
And similarly for S, S-op
Then the isomorphism from R to S satisfies $f((a,b)_R) =(f(a),f(b))_S$
So now we’re looking for a mapping that works when R, S are replaced with their opposites
With the most obvious thing to check first is whether f itself still suffices
$$f((a,b)_{R^{op}})=f((b,a)_R)= (f(b),f(a))_S=(f(a),f(b))_{S^{op}}$$
That certainly seems to work
 
Hmmmm, so $f$ is legitimately the isomorphism for both.
 
8:44 PM
Seems like it
 
I had ruled that out early on. I forget why. Probably something about it being "too easy."
 
Main point being that you need to reverse the multiplication at the level of both R-op and S-op
If you only do one or the other, then it won’t work
In your original notation:
$$f(a\circ b)=f(ba)=f(b)f(a)=f(a)\circ f(b)$$
 
Excellent, danke for the help, Semi.
 
No problem
 
8:59 PM
I'm having trouble applying $(\vec R \cdot \vec R)' = 2\vec R' \cdot \vec R$. When I plug $\begin{bmatrix}t + 2 \\ 3t^2\end{bmatrix}$ into the LHS I get $20t + 4$, but for the RHS I get $36t^3 + 2t + 4$. I know I must be doing something insanely stupid.
Plugging the vector in for $\vec R$ of course.
 
9:18 PM
Do points around a unit circle form a ring?
 
Yeah, that's actually related to the origin of the term. Consider the integers adjoined to an nth root of unity.
 
9:53 PM
I’m not seeing it as a ring. A (cyclic) group, sure
 
Yeah you need to have addition different from multiplication, and there is no zero there. But it is related for sure.
 
Wikipedia has some of the history here: en.m.wikipedia.org/wiki/Ring_(mathematics)
Interestingly, it links it more with the ring of algebraic integers than anything else
Though the long answer here casts doubt on that: mathoverflow.net/a/117314/55904
 
10:13 PM
Hey everyone. Does anybody know a short proof that expressing a real set as finite union of pairwise disjoint, closed intervals is, if possible, unique (up to reordering)?
 
11:11 PM
@Thorgott my instinct is to say that it know the boundary of such a set
 
11:29 PM
Oh yeah, that's a pretty nifty solution. Thanks!
 
11:43 PM
hey
 
Hola
 
@Thorgott: I don't believe it. How do I get an open interval? Or $\{1/n\}$? Am I missing something.
hi @Rithaniel
 
How's it going, Ted?
 
You might be missing the "if possible"
 
Going great, thanks.
LOL, OK, Thorgott. I thought you and Demonark were thinking it was true.
 
11:51 PM
@TedShifrin hi
 
hi Karim
 
I am just solving Folland book I am stuck in something small
 
Hey, how's it going?
 
Hi Demonark
 
hi @Daminark
@TedShifrin Do you know David Cox ?
I am attending a workshop organized by him this July
 
11:56 PM
We met once years ago.
 
how is he ? Is he nice ?
 
I have no recollection.
 
I see. hopefully he is nice. I have a lot I would like to discuss with him.
 

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