« first day (1857 days earlier)      last day (3162 days later) » 
00:00 - 19:0019:00 - 22:00

12:49 AM
Hello, I'm rather confused by the answer to my question here: math.stackexchange.com/questions/1420461/…
Is it in fact the case the inner product and orthogonality does not depend on the basis vectors and the coordinate system?
 
Fresh Prince of Bel Air
 
Nice one - unfortunately I'm not related.
 
awww
 
1:27 AM
@FreshAir The RESULT that one gets for the inner product between 2 vectors should not depends on the basis that we choose. This should be obvious in the case of $\mathbb{R}^2$ because the dot product is a purely geometric quantity, it tells you something about the angle between the vectors
@FreshAir But the mechanical procedure for taking such a dot product will depends on the particular basis we choose. It's analogous to choosing a coordinate system.
For example, suppose we have a 2 2D vectors $ \vec{v_1} = a \vec{e}_x + b \vec{e}_y$ $ \vec{v_2} = c \vec{e}_x + d \vec{e}_y$, where the basis vectors are the standard orthonormal basis
Then the dot product is just $\vec{v}_1 \cdot \vec{v}_2 = ac + bd$, as you know
But suppose we change basis and now describe these vectors in terms of a new basis $$\vec{v}_1 = \alpha \vec{e}_1 + \beta \vec{e}_2$$
$$\vec{v}_2 = \gamma \vec{e}_1 + \delta \vec{e}_2$$
Now the dot product is $$\vec{v}_1 \cdot \vec{v}_2 = (\alpha \vec{e}_1 + \beta \vec{e}_2) \cdot (\gamma \vec{e}_1 + \delta \vec{e}_2)$$
$$ = \alpha \gamma \lvert \vec{e}_1 \rvert^2 + (\alpha \delta + \beta \gamma) \vec{e}_1 \cdot \vec{e}_2 + \beta \delta \lvert \vec{e}_2 \rvert^2$$\
It is precisely this 'cross-term' in the middle that you are missing in you posted question @FreshAir
So before you can compute the dot product of other arbitrary vectors, you first have to say how to take magnitudes and dot products of your basis vectors. Since we've alreayd defined how to do that for the 'standard' orthonormal basis, we have to choose a definition for these operations in the new basis that is consistent with that original definition.
 
2:01 AM
@KevinDriscoll Thanks for this. I'll think about it and let you know if I have further concerns.
 
@FreshAir I also answered your question, just fyi
 
Oh okay
 
 
4 hours later…
6:24 AM
hi @Ted
 
Must be morning for you, Balarka ☺️
 
yeah, it is :P
 
No school?
 
nope. exams finished 2 weeks ago.
 
wow, you're retired just
like me!
 
6:27 AM
heh. where are you now? i was surprised at first that you are awake, but then i recalled you were on your road trip
so time zones might have changed a bit.
ah.
 
Agh, can't stand doing this on my phone.
 
hmm. i'm trying to prove that f.g. projective modules over PID's a free. let $M$ be a proj. module. there is some $N$ such that $M \oplus N$ is free. free implies no torsion, so $Tor(M \oplus N) = Tor(M) \oplus Tor(N) = 0$. each factor is zero, so $M$ has no torsion either. invoke classification of f.g. moduels over PID to conclude $M$ is free.
is there no way other than classification theorem to do this?
 
G'night! ..: Be carful
 
'night. yeah, modules are subtle, so i know what you mean.
 
6:54 AM
@BalarkaSen Well, you can shorten it by noting that projective implies flat, and flat implies torsionfree over a domain (and then it is basically the classification in a different disguise)
 
right
 
@BalarkaSen Though I guess to make it completely the classification, you need to wrap back to get that torsionfree implies free (or just that it implies projective)
 
7:32 AM
Hello@Tobias @Balarka
 
@Rememberme Hi
 
@Tobias We have the characteristic polynomials for a linear operator on a finite dimensional vector space $V$. We can always associate with this polynomial a space $F[x]$ where F is a field. Right? What all can we say about $F[x]$ with just the linear operator given?
 
@Rememberme not sure what space you want to associate to it. The notation suggests just the space of polynomials in one variable
 
@Rememberme hi
 
My notation might be a bit misleading .
 
7:48 AM
how are you associating a polynomial ring given a certain polynomial? that doesn't seem a good thing to do.
 
What I actually want to say is that with the characteristic polynomial of a linear operator on a finite dimensional vector space $V$ (dim=n). We can always associate this polynomial with the space of polynomials in one variable(Can we actually do that? always). Now my question is with just the linear operator given we what can we say about this space of all polynomials in one variable
 
"We can always associate this polynomial with the space of polynomials in one variable" sure, then that'd be just boring.
for every linear transformation on an $F$-vector space, you are associating $F[x]$.
 
Yes.
 
@Rememberme what you are doing does not seem to be dependent on the polynomial
 
it seems a completely uninteresting thing to do, as it doesn't depend on the linear transformation you choose
 
7:52 AM
Okay.
 
why do you want to do anything like that anyway?
 
I want to think of a polynomial ring in terms of a linear operator from a vector space V to V whose characteristic polynomial lies in that ring.
 
why? (btw, you can associate to any polynomial ring F[x] an F-vector space with a linear transformation : it's just what an F[x]-module is, but that seems different from what you're trying to do)
 
Because characteristic polynomials seem very fascinating to me. And to think of a ring which can be thought of using this polynomial might be more interesting in my point of view. But as you say it is boring
 
i don't see why it is interesting, but whatever
 
8:01 AM
@Balarka What are the interesting things we can say if we think of a polynomial ring of the form $\Bbb{Q}[\sqrt{x}]$
 
it's not a polynomial ring.
the only way to make sense of what you wrote is as the quotient ring $\Bbb Q[x, y]/(y^2-x)$.
 
@BalarkaSen Not even that way
 
ah?
whoops, typo
 
More like $\mathbb{Q}[x,y]/(y - x^2)$
 
yep, typo
 
8:04 AM
well, now we certainly agree :)
 
If x is rational and not a perfect square in $\Bbb{Q}$
 
then it's not even a quotient ring of a poly. ring
it's a field
 
Ahh.. Okay
Thanks for that . My internet is a bit slow so taking time to write
 
why can't it be both?
 
Which both @SamuelYusim
 
8:08 AM
polynomial ring over $R$ is a ring of the form $R[x_1, x_2, \cdots, x_n]$ where $x_i$ are $R$-algebraically independent transcendentals.
it's the definition of a polynomial ring.
 
@BalarkaSen Well, it does become a quotient of a polynomial ring
 
ok, fair enough
$\Bbb Q[x]/(x^2 - a)$
 
a quotient of a polynomial ring $F[x]$ by a maximal ideal $M$ gives you a field extension of $F$
in the case of multiple variables it's the same
 
My question :I have been looking at the quotient notation for rings. How do we define quotients for rings. The same way as we did for groups?
 
@Rememberme Yes, though we need to quotient by ideals instead of normal subgroups
 
8:10 AM
@Rememberme read it from somewhere.
you need to know what an ideal is
 
@BalarkaSen That is only for alg. closed $F$
 
the idea is the same though. an ideal is precisely what kernel of a ring morphism is.
@Tobias i'm still sleepy, sorry!
 
Okay . Need to learn that
 
I was gonna say
and regardless, $F$ is a field extension of $F$ in my book
 
it is, but that is just a trivial thing to say. i agree with you that qt. by a maximal idea is a field extension of $F$
this is just because qt. by maximal ideal is always a field, and that field contains $F$ by correspondence of ideals and qts.
 
8:12 AM
@BalarkaSen Well, because nothing but the $0$ from $F$ can be in the maximal ideal
so the composed map becomes injective
 
right
 
8:39 AM
at any algebraic topologists, category theorists, what are the main mailing lists for each one respectively? I did a preliminary search and found quite a few, but would like to just add the main one of each.
 
@RobertCardona Mailing lists for what purpose? conference announcements and such?
 
Hi
How to write a numbered equation in latex?
 
@Gigili try \tag{#}, for example x^2 \tag{2} gives $$x^2 \tag{2}$$
 
It's \gather in normal latex, but asking a question I dont know how to make the equation numbered so that I could refer to it later
@AntonioVargas Ah OK, thanks
Wait a minute
No, that's not what I need
$$||Y-DX||_F^2\\=||Y-\sum_{j=1}^K d_jx_T^j||_F^2\\=||\big(Y-\sum_{j \neq k} d_jx_T^j\big)-d_kx_T^k||_F^2\\=||E_k-d_kx_k^T||_F^2 \tag{1}$$
 
Ah, you want the whole thing numbered, rather than just one line?
 
8:50 AM
The other way around, I want every line of the above formula to be numbered
 
I would recommend using align then
just add \tag{#} at the end of each line
before the \\
also, use \| instead of ||
$\|$ vs $||$
 
@AntonioVargas Noted, thank you
 
I would probably format it something like $$\begin{align} &\|Y-DX\|_F^2 \tag{1} \\ &\qquad = \left\|Y-\sum_{j=1}^K d_jx_T^j\right\|_F^2 \tag{2} \\ &\qquad =\left\|\big(Y-\sum_{j \neq k} d_jx_T^j\big)-d_kx_T^k\right\|_F^2 \tag{3} \\ &\qquad = \left\|E_k-d_kx_k^T\right\|_F^2 \tag{4} \end{align}$$
@Gigili glad to help :)
 
Thank you very much
What difference does it make if you use \qquad instead of \quad?
 
@Gigili Bigger space
 
9:04 AM
Ah, interesting
@AntonioVargas Your formatting looks much better than mine
$$\begin{align}
\|Y-DX\|_F^2 \tag{1}\\
=\|Y-\sum_{j=1}^K d_jx_T^j\|_F^2 \tag{2}\\
=\|\big(Y-\sum_{j \neq k} d_jx_T^j\big)-d_kx_T^k\|_F^2 \tag{3}\\
=\|E_k-d_kx_k^T\|_F^2 \tag{4}
\end{align}$$
Couldn't you do something so that the first equation will be center aligned?
hmm, never mind! Spent enough time on formatting, enough for asking a question on main
Thanks again
 
 
1 hour later…
10:25 AM
hi ! may I ask quest . here ?
0
A: First order logic expression of "Each finite state automaton has an equivalent push-down automaton"?

Kevin QuirinIn your second formula, x is not even bounded in the second part, so $$(∀x~ fsa(x))→(∃y~ pda(y)∧equivalent(x,y))$$ contains a free variable. Even considering its universal closure, it would not mean what you want.

 
 
2 hours later…
12:25 PM
@Gigili Here's the difference $\varepsilon\quad \delta$ & $\varepsilon\qquad \delta$, the difference is that /qquad gives more space
 
3 hours ago, by Tobias Kildetoft
@Gigili Bigger space
 
1:12 PM
@Chris'ssistheartist
6
Q: How to calculate the limit that seems very complex..

smallsmalliceSomeone gives me a limit about trigonometric function and combinatorial number. $I=\displaystyle \lim_{n\to\infty}\left(\frac{\sin\frac{1}{n^2}+\binom{n}{1}\sin\frac{2}{n^2}+\binom{n}{2}\sin\frac{3}{n^2}\cdots\binom{n}{n}\sin\frac{n+1}{n^2}}{\cos\frac{1}{n^2}+\binom{n}{1}\cos\frac{2}{n^2}+\binom...

Interesting one.
$$I=\displaystyle \lim_{n\to\infty}\left(\frac{\sin\frac{1}{n^2}+\binom{n}{1}\sin\frac{2}{n^2}+ \binom{n}{2}\sin\frac{3}{n^2}\cdots\binom{n}{n}\sin \frac{n+1}{n^2}} {\cos\frac{1}{n^2}+\binom{n}{1}\cos\frac{2}{n^2}+\binom{n}{2}\cos\frac{3} {n^2}\cdots\binom{n}{n}\cos\frac{n+1}{n^2}}+1\right)^n$$
 
@IWantToRemainAnonymous it's limit of $e$ at the big fraction multiplied by n. Euler formula should be useful. All reduces to boring calculations.
OK, the limit is $e^{1/2}$.
 
1:31 PM
$$\lim_{n\to \infty } \, \exp \left(\frac{n \Im\left(e^{\frac{i}{n^2}} \left(1+e^{\frac{i}{n^2}}\right)^n\right)}{\Re\left(e^{\frac{i}{n^2}} \left(1+e^{\frac{i}{n^2}}\right)^n\right)}\right)=e^{1/2}$$
As lab bhattacharjee, Moivre gives immediately the way to go, and to get rid of that ugly power in $n$ use that $1+\cos(x)=2\cos^2(x/2)$ and then place that $n$ in power in the arguments of sine and cosine in brackets.
That's all.
Well, not immediately since you have squared cosine, it doesn't work the foregoing operation.
With twice the argument it works as lab did it $1+e^{2iy}=2\cos y(\cos y+i\sin y)$. to have it nicely arranged.
or otherwise write that $\sin(x)= 2\sin(x/2) \cos(x/2)$ to factorize $\cos(x/2)$ such that you can place the power in argument (then you can keep the form $1+\cos(x)=2\cos^2(x/2)$)
There is nothing amazing in these limits, but only boring stuff, that is a classical limit of the type $1^{\infty}$ that reduces to $e^{\lim \text{something}}$. Play with Euler and Moivre formulas and you're done.
 
1:51 PM
Boring?
I've never heard you use that word with limits :P
 
@Rigor I did tons of them. :-)
I would like to see an unusual approach, something like slaying the limit from one single shot.
 
Like David meets Goliath?
 
@Rigor Yeah :-))))))))
 
:-)
 
@Rigor I see such a way now.
 
1:57 PM
Cool.
 
My way
0
A: How to calculate the limit that seems very complex..

Chris's sis the artistWith rough approaximations, we can avoid the use of trigonometric stuff, that is $$\lim_{n\to \infty } \, \left(1+\frac{2^{n-1} (n+2)}{n^2 2^n}\right)^n=\lim_{n\to \infty } \, \exp\left(\frac{2^{n-1} (n+2)}{n 2^n}\right)=\sqrt{e}$$ where $\displaystyle \sin\left(\frac{k}{n^2}\right)$ behaves lik...

Initially I let things unsimplified in the fraction such that my way is better understood. Now I see another answer using the idea in my answer.
To make it rigorous, use Taylor with error term and bla bla. It's not for me this kind of job now.
 
2:23 PM
@Balarka?
 
come over to the room
 
My way allows you to calculate the limit WITHOUT PEN AND PAPER, but this might not be useful for MSE users.
Back to my research.
 
2:41 PM
nothing beats pen and paper
what if i told you, the hardest problems i have solved using a pen and paper away from my laptop screen ?
 
@Agawa001 If you wanna do the hardest stuff in integrals, series and limits you need to push your mind extremely hard.
 
one cant focus with all these screen radiations targetting his faceskin
 
@Agawa001 Maybe. :-)
 
@Chris'ssistheartist especially with a cup of coffee and fresh air
 
@Agawa001 :-) yeah, especially fresh air :-)
 
2:51 PM
especially the sea breeze :)))
 
ohhhhh, don't say it ... :-)
 
lol why ?
 
@Agawa001 I miss it, I didn't see the sea for some years ... :-(
 
@Chris'ssistheartist thats not same, i was born in the coast, i cant imagine a nature without sea :D
 
@Agawa001 nnniiiiiiiiiccccccccceeeeeeeeeeeee :-)
 
2:57 PM
i m looking up romania at the map
 
@Agawa001 and the Black sea. :-)
 
you have still a little opening to the sea :)
 
@Agawa001 I live in the other side of the country. :-)
 
@Chris'ssistheartist it looks much like a basin than a sea , well i guess streams and whirls are hardly found there isnt it ?
 
@Agawa001 Yeap.
 
3:01 PM
that makes it safer than other seas
 
@Agawa001 you live in US?
 
lol no
norrth africa
 
@Agawa001 Ah, OK. Hot places there. :-)
 
no not hot, just in summer
 
Algeria has a nice anthem
 
3:06 PM
@Agawa001 Nice anyway. :-)
@Agawa001 Have you ever visited our country?
 
@Chris'ssistheartist no, i just visited italy and france
my sojourn there was limited
 
I see. I lived in Italy for some time.
 
3:23 PM
@DanielFischer Would I be right in stating that for a unital Banach algebra the spectrum $\sigma(0) = 0$?
 
That's correct.
 
@MikeMiller Thanks. Could I ask for a hint regarding something. I want to prove that for idempotent members $a^{2} = a$ in a unital Banach algebra, it follows $\sigma(a) = \{0,1\}$. So in order to this I will use the Spectral Mapping Theorem. Hence I will consider the analytic function $f(x) = x^{2}-x$ on some neighbourhood of the spectrum of $a$. Then the Spectral Mapping Theorem yields $\sigma(a^{2}-a) = \sigma(a)^{2}-\sigma(a) = \sigma(a) -\sigma(a) = 0$. Is this the correct approach so far?
 
3:41 PM
Yeah, that's good. The point being that an element of
the spectrum would have to be idempotent, and there are only two idempotents in $\Bbb C$.
So you've proved that the apectrum is a subset of $\{0,1\}$.
 
@MikeMiller Yeah that's what I proved. Do you have any small hint on how to proceed?
@MikeMiller Why can't it be the full interval $[0,1]$? Since you would have $[0,1] = [0,1]^{2}$
 
3:58 PM
Upvote (and provide with an amazing solution)
0
Q: Calculating in closed form $\int_0^{\pi/2} \arctan\left(\sin ^3(x)\right) \, dx \ ?$

Chris's sis the artistIt's not hard to see that for powers like $1,2$, we have a nice closed form. What can be said about the cubic version, that is $$\int_0^{\pi/2} \arctan\left(\sin ^3(x)\right) \, dx \ ?$$ What are your ideas on it? Differentiation under the integral sign? Other ways?

 
@Moses: 1) For a nontrivial idempotent you can prove those are both in the spectrum by the definition, basically.
I think the holomorphic function calculus is point wise. That is, when you say $f(\sigma(a))$, you mean $\{f(s) \mid s \in \sigma(a)\}$.
@Moses: So in particular this means that if $s \in \sigma(a)$ then $s^2 = s$. This is must stronger than saying that the set $\sigma(a)$ satisfies $\sigma(a)^2 = \sigma(a)$.
 
4:19 PM
Hi there!
Given two rings $A,B$, homomorphism $f$ between them, and an $A$-module $M$,
how do we give $B\otimes_A M$ the structure of a $B$-module?
I think I got it, thanks anyway...
 
4:39 PM
hello can someone shortly write or give me a link about why is if S is transition matrix from base $V=\left[ \left[ v_1\right] ,\left[ v_{2}\right] \right] $ to
base $W=\left[ \left[ w_1\right] ,\left[ w_{2}\right] \right] $ then $S=W^{-1}.V$
 
@MikeMiller I'm not following you reasoning regarding the conclusion of your statement:
"That is, when you say $f(\sigma(a))$, you mean $\{f(s) \mid s \in \sigma(a)\}$. So in particular this means that if $s \in \sigma(a)$ then $s^2 = s$."
 
Do you agree that that is the definition of $f(\sigma(a))$?
 
@MikeMiller Yes that is just the image of $f$ on $\sigma(a)$. Are you saying that because we have $\sigma(a)^{2} = sigma(a)$ we have that $s^{2} = s$ or that we always have $s^{2} = s$ for any $s \in \sigma(a)$?
 
Well, we know $f(\sigma(a)) = 0$, like you pointed out. So, by the definition of $f(\sigma(a))$, we have for $s \in \sigma(a)$, $f(s) = 0$. Well, $f(s) = s^2-s$.
It is not true that $C^2 = C$ implies that $C^2 - C = 0$. You can't subtract sets wildly, unfortunately.
We have the latter statement. It's stronger.
(The point being that $C - C$ is not actually zero if $C$ is not a singleton. If $C = [0,1]$, then $C - C = [-1,1]$.)
Hi @Ted.
 
Goodnight @Mike ... Inconsistent wifi here ...
 
4:53 PM
RIP.
 
RIP?
 
hi chat
 
No wifi sounds fatal, @Ted
2
 
Hi @Semiclassic
 
hi @ted
@mike still want that link i mentioned a while back?
 
4:55 PM
Oh, sure, I can't read it now but I can bookmark it
 
It's life 'n death, huh?
 
sure
...crap, now i need to find it again :/
 
I didn't get an answer to that $\Bbb{CP}^{2n} \# \Bbb{CP}^{2n}$ question yet, @Ted. Oh well.
 
@MikeMiller Yes I understand, thanks. I overlooked that we could use both $f(s) = 0$ and $f(s) = s^{2}-s$ to imply that $s = s^{2}$, hence I was trying to work from the weaker result that $\sigma(a)^{2} = \sigma(a)$.
 
OK, great.
 
5:00 PM
okay, the notes i was linking before were part of a learning seminar at Northwestern
with the pdf i linked being Introduction to $N=2$ Gauge Theory
of which i really only have in mind the first page, since the rest is technical
 
great, thanks
 
i fear it's more on the 'physics' side than the math (albeit not physics i understand) but eh
you might recognize some of the words, anyways
for example, on the first page you see sentences like
"Before moving on to explaining what the $N = 2$ theory is, let me say approximately what the Nekrasov partition function is. The Nekrasov partition function is a stand-in for the partition function of the twisted $N = 2$ theory which one can define mathematically rigorously. The partition function of the twisted theory can be computed by a localization procedure as the volume of the moduli space of vacua, which in this case will be the moduli space of instantons."
 
these are all math people and they're talking in a language i don't understand
darn
 
dang
i suspect that a key phrase in there is "moduli space of instantons"
 
Hello!!
I want to prove the following lemma:

Assume that the characteristic of $F$ is $p$ and $p>2$.
Then $(t^m-1)/(t^n-1)$ is a square in $F[t, t^{-1}]$ ($F[t,t^{-1}]$: the polynomials in $t$ and $t^{-1}$ with coefficients in the field $F$) if and only if $(\exists s \in \mathbb{Z}) m=np^s$.


I have done the following:

$\Rightarrow : $

Let $a \in F[t, t^{-1}]$ such that $\frac{t^m-1}{t^n-1}=a^2 \Rightarrow t^m-1=a^2(t^n-1)$.

Let $m=m_1 p^l $, where $p \nmid m_1$. Then $t^m-1=t^{m_1p^l}-1=(t^{m_1}-1)^{p^l} \Rightarrow a^2(t^n-1)=(t^{m_1}-1)^{p^l} \ \ (*)$.
 
5:05 PM
sure, that's the only phrase i understand
 
which makes the phrases 'instanton-counting' and 'partition function' sound plausible, even if they're beyond me in this context
but yeah, it's a language issue
there might be still be stuff in there you appreciate, though, or at least is suggestive
alas, me giving references on this stuff feels like the blind leading the blind
what's (mostly) surprising to me is that the stuff i'm seeing has a tendency to link Seiberg-Witten theory to random matrix theory
which is something i've been butting up against for quite different reasons lately
 
5:25 PM
@AntonioVargas speaking of random matrix theory, how're things with you?
 
Argh, I never get on when @Ted is on
 
hi @Kaj
what's up
 
Hey @MikeMiller
Just got back from algebra and the gym
 
at the same time?
 
haha, nope. Just one right after the other. Today, we discussed normal series, composition series, and Jordan-Holder.
 
5:38 PM
Ah, that's fun. And what'd you do in algebra?
 
hahaha
 
@Semiclassical pretty good, progress is slow though
I'm spending some time on some side projects until I can get back into it
How are things with you?
 
@TobiasKildetoft, yes.
@MikeMiller do you know what the main alg. topo. mailing list is?
 
5:53 PM
@MikeMiller What do you think of my proof that if $a \in \mathcal{A}$ is a non trivial idempotent then $\{0,1 \} \subset \sigma(a)$. Assume that $0 \in p(a)$ (where $p(a)$ is the resolvent set of $a$) then $a \in \mathcal{A}^{-1}$. Thus there exists some $b \in \mathcal{A}$ such that $$ab = 1 = ba.$$ Then also $a(ab) = 1 = (ba)a \implies a = 1$. Contradiction.

Assume now that $1 \in p(a)$. Then $a-1 \in \mathcal{A}^{-1}$. There exists a $b \in \mathcal{A}$ such that $$(a-1)b = 1 = b(a-1).$$ Since $a$ is idempotent it can be shown that $a^{2}b-b = 1 = ba^{2} -b$. Thus $$(a-1)(a+1)b = 1 = b(
 
@RobertC: I don't know any mailing lists.
 
k! thanks anyway
 
@Moses: I'm not reading carefully, but zero divisors cannot be invertible, and $e$ and $e-1$ are zero divisors.
 
@MikeMiller Oh...Well that shortens the proof I guess.
 
6:11 PM
rehi @RobertC, morning @MikeMiller
 
@AntonioVargas well, semester is starting up again, and i'm having to go back to TAing for reasons
so that's a thing
as far as research goes, similarly kind've slow
i'm trying to put together some notes for my collaborators (i.e. my advisor and another of his grad students)
on orthogonal polynomials and stuff. but ugh, tedious
 
gah, nothing worthy of answering in my tags
 
@Semiclassical we live a glamorous life as grad students :)
 
right now I'm trying to put together a set of notes on what I've learned
it's kinda fun
nothing too deep in it but at least I can give my own perspective on the material
 
6:16 PM
sure
i forget what part of it you were after
 
It's just notes on integral asymptotics, including some linear riemann-hilbert techniques
 
ahhh. that's what i'm heading for, actually
which means i may want to borrow them :P
 
most definitely. Once I get to that part I'll just share it with you on dropbox or something if you'd like
(might not be any time soon)
 
gotcha. i'll do the same with my stuff; my coworkers wanted something that gives the definitions of various OP/RHP stuff, along with why they should care about it :P
so you can probably detect if i say something utterly wrong :/
 
yeah I'd definitely like to read that too. I feel like it must start to click eventually if I read it enough times.
 
6:21 PM
sure
i forget, actually. had you run into any stuff involving tau-functions in your readings?
 
Hm, no. On wiki they have a Ramanujan tau function, is that the same thing?
 
nope.
 
Hah, I was wondering, didn't think you were that into number theory
 
it's related to the RHP stuff, insofar as one has a story in there about isomonodromy
though damned if i can understand it :(
 
You know, they can keep adding prefixes to "monodromy", but it doesn't make it any cooler
 
6:23 PM
haha
the OPRL story i know about tau-functions goes like this
suppose i start with a spectral measure $d\mu$, and then define $d\mu(\mathbf{t})=e^{-\sum_{k=1}^\infty t_k x^k}d\mu$
with the 'multi-times' $t_k$ serving as deformation parameters.
so now i have a whole infinite-dimensional parameter space available, with trajectories in there being families of continuous deformations of the initial measure
similarly, there will be 'time-dependent' moments $\mu_k(\mathbf{t})=\int x^{k} \,d\mu(\mathbf{t})$
which, owing to the form of $d\mu(\mathbf{t})$, have a neat property: $\partial_{t_j}\mu_k(\mathbf{t}) = \mu_{j+k}(\mathbf{t})$
 
Morning @Balarka.
 
so differentiation wrt to the times just shifts the moments around
the tau-function is then introduced by forming the (Hankel) matrix-of-moments $(\mu_{j+k})_{j,k\geq 0}$ and takings its determinant
and, apparently, it's a nice object to study
 
interesting
Is the idea to go from properties of the Hankel matrix back to properties of $d\mu$, e.g. the OPS?
 
tbh, i'm not sure. what i'd really like to get out of it isn't the OPs themselves, but their asymptotic density of zeros
 
right
zeros are always the goal
 
6:35 PM
right
 
@IWantToRemainAnonymous great name!
 
@AntonioVargas :D
 
to see why it might be a nice object, remember that one way to compute a scalar derivative of a matrix is to differentiate just the first row and take the determinant, then differentiate just the 2nd row and take the determinant, etc. and then sum all of those determinants
but, for instance, $\partial_{t_1}( \mu_0,\mu_1,\cdots)=(\mu_1,\mu_2,\cdots)$ which is just the second row
 
ok, so the scalar derivative is 0?
 
not sure, actually: it's the determinant of an infinite matrix
 
6:40 PM
Ahh right
 
and if you only consider truncations of it, then when you do that not all of the rows will be 'cloned' under differentiation
but it does tell you that there should be nice properties under derivatives. in particular, one can hope to get differential equations out of it
 
Oh, that's cool
 
in playing around with it in mathematica, it seems to be that if the matrix is taken as finite, and one does partial derivatives, what one gets is something that's exponentially asymptotic to zero
(that i slipped from mathematica to excel is a sign of me anticipating TAing intro classes this semester :/)
now, tbh, i'm not sure i understand that story. but there is something interesting about it
 
@Chris'ssistheartist so your so scary limits are treated using taylor series !
 
my main goal with it is to appreciate the linkage between OP stuff and integrable systems stuff
 
6:45 PM
i thing i lack this level of knowlegde
 
which does show up very briefly in Deift's notes, but not in a really helpful way (page 25, to be exact)
 
heya @Ted
 
@Kaj: Did you summon me?
 
hi @Balarka
 
6:47 PM
@Semiclassical Do you like TAing?
 
@antonio the paper you should read if you find that interesting is this: mathstat.concordia.ca/faculty/bertola/Research/MomentTau.pdf
 
Waiting to have dim sum with a former student who now works for Google.
 
I'm curious how to define tangent space on algebraic varieties, now that I can do it for surfaces (real algebraic varities?), @TedShifrin.
 
i like the teaching/communicating aspects of it, namely of coordinating student discussion and lab activity
the administrative side, though---attendence, grading, etc.---is a pain in the ass :/
 
Hypersurfaces aren't bad (except for singularities), but when you have more equations than codimension it's interesting.
 
6:50 PM
Oh man attendance
 
or to put it another way: Assisting students is fun, assisting the course is not
 
Luckily we only need to take attendance during quizzes
 
@Agawa001 You don't even need to use Taylor series idea. :-) Knowing that $\lim_{x\to 0} \sin(x)/x = 1$ and $\lim_{x\to 0} \cos(x)=1$ is enough.
 
well, i'm only responsible for some portion of the class---say, 40 students in two sections
 
that's good
 
6:51 PM
so that makes it easier. but lab report grading? gags
 
any kind of grading
I lean more toward the "abolish grading" side of things
mainly because I don't want to do it
 
yeah. quiz grading is a lot easier on an individual basis (especially since the prof, if i remember from an earlier semester TAing under him, tends to be pretty formulaic in his long problems)
 
Abolish learning, too.
 
@TedShifrin That's the spirit!
 
it's just that there's a ton of students
 
6:53 PM
@TedShifrin It sounds weird that you can define an infinitesimal tangent vector at a point in your algebraic variety.
I have completely no idea how to do that.
 
No infinitesimals unless you're playing with dual
 
hmm. what if i look at covectors instead of vectors? hmmm.
 
13 sections total, at 18 seats max, gives...
 
numbers and schemes. Then it's language.
 
@TedShifrin haha. had the same thought.
hmmm.
 
6:54 PM
234, i guess
 
i really can't do chat on my phone.
 
I think our engineering calc classes have ~8*50 = 400 students
 
I wonder how Mike does it. (yeah, yeah, I know. with gusto.)
 
The derivative of a scalar function at a point is a covector.
 
so upwards of that many student problems to grade per long problem per quiz, with one of the TAs handling each pile over a weekend
 
6:56 PM
@Balarka: There is more than one way to define a tangent space, and these sometimes give distinct generalizations to algebraic geometry.
 
@MikeMiller examples?
 
interesting
 
it's not brutally hard, especially if the problem is straightforward to grade (and with this prof, as i said, i suspect it will)
 
it seems like it should be pretty nontrivial to define tangent spaces
 
Hey @TedShifrin
 
6:57 PM
@KajHansen harro
 
It's trivial to define the tangent space once you learn the correct notion for manifolds, ie one that doesn't depend on an embedding.
 
but lab report grading is pretty awful. you've still got a weekend to do it, usually, but you've got something like 35 student papers to grade, each of which are a few pages long
 
I am no longer as confident about my previous statement that the generalizations can be distinct.
 
heya, Kaj
 
lab report grading is what i'm dreading the most
 
6:58 PM
with singularities @Mike
 
@MikeMiller you mean of smooth manifolds? because I already know a coordinate free definition in the topological category : topological space which is locally homeomorphic to $\Bbb R^n$.
 
@Semiclassical I feel for you.
Stay strong brother.
 
thanks
 
I'm having a pretty good semester so far @TedShifrin
 
There is no tangent space in TOP.
 
6:59 PM
@Balarka: We're talking about tangent spaces, so if I'm talking about knowing the correct definition, I'm probably talking about tangent spaces.
 
things are also goofy this year because the campus physics building is being thoroughly renovated
 
Nakano's course is awesome. I'm really glad I waited to have it with him too.
 
00:00 - 19:0019:00 - 22:00

« first day (1857 days earlier)      last day (3162 days later) »