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1:17 AM
@Thorgott @Lelouch Yeah that's what I meant, the general case follows from Cartan's magic formula
Much better than doing coordinates
That circle of ideas is known as the Moser trick; you have an isotopy taking a closed form $\omega_0$ to another closed form $\omega_1$ and you want to say that means the forms differ by an exact form.
 
ah, makes sense
 
Technically speaking Moser trick goes backwards. Here's an application; say $M$ is a closed manifold, $\omega_0$ and $\omega_1$ are two volume forms on $M$ such that $\text{vol}(M, \omega_0) = \text{vol}(M, \omega_1)$.
Then there is a diffeomorphism $f : M \to M$ such that $f^* \omega_1 = \omega_0$
 
that's cool
 
re @Thor, hi, a @Balarka
 
Hi @Ted!
@Thorgott Want to try and prove this?
 
1:29 AM
rehi Ted
 
I have to work this out everytime but the main idea is, write the concordance of forms $\omega_t := t \omega_0 + (1 - t) \omega_1$, and then try to solve for an isotopy $f_t : M \to M$ such that $f_t^* \omega_t = \omega_0$.
 
it sounds like a good exercise
but I'll save it for later
 
Mmk
 
I think I'm currently getting close to finally figuring out the sphere bundle
 
What is so difficult for you?
 
1:34 AM
$f_t^* \omega_t = \omega_0$ implies $\mathcal{L}_{X_t} \omega_t = 0$ where $X_t$ is the time-dependent vector field that integrates to $f_t$... Cartan's magic formula implies $0 = \iota_{X_t} d\omega_t + d\iota_{X_t} \omega_t$...
i think thats how it goes anyway; you differentiate a differential equation to solve it lol
Oh I messed it up
$\partial_t(f_t^* \omega_t) = \mathcal{L}_{X_t} \omega_t + \partial_t \omega_t$
So I need to solve for $\partial_t \omega_t + \iota_{X_t} d\omega_t + d\iota_{X_t} \omega_t= 0$
If $\omega_t$ is already closed as in our case the middle term goes away
And $\partial_t \omega_t = \omega_0 - \omega_1$ which is actually some exact form because $\omega_0$-volume and $\omega_1$-volume of $M$ are the same.
If $\alpha$ is the potential we just need to solve for $\iota_{X_t} \omega_t = \alpha$ which is always possible since the volume forms are nowhere vanishing
 
 
1 hour later…
2:44 AM
Let $\langle x\rangle$ be the integer nearest $x$, defined for $x$ not a half integer. It equals $\lfloor x+\frac12\rfloor=\lceil x-\frac12\rceil$.
Then the $n$th nonsquare number is $n+\langle\sqrt n\rangle$.
The $n$th nontriangular number is $n+\langle2n\rangle$.
In particular, those are never square (resp. triangular).
 
Hey, can we divide a straight line into $m:n$ ratio, using ruler and compass only? You know, with the aid of Euclidean Geometry, and not with the Cartesian one?
 
$m$ and $n$ are integers? Yes.
 
Uh yes, $m$ and $n$ integers. So what do I look up for? I mean, what keywords should I use? (^^")
 
You can search "divide a line segment into equal parts using compass and straightedge" or something similar
Once you've divided into $m+n$ pieces you're golden
 
Yup :3 Thank you, this works!
 
2:53 AM
Here's another way, but it assumes you know how to draw parallel lines using compass and straightedge (not shown in the video):
@Swarup
 
Ah huh, yes! Tysm! I'll check it out too!
I actually had this one in high school... sigh, I forgot everything...
*the first one
 
It's interesting how you can divide a line in thirds but not an angle
(Theorem: You cannot construct a 20 degree angle with compass and straightedge, but you can construct a 60 degree angle.)
The proof involves linear algebra. It's to do with statements like this: the set of numbers of the form $a+b\sqrt 2$ where $a$ and $b$ are rational (written $\{a+b\sqrt2:a,b\in\mathbb Q\}$) is 2-dimensional vector space over $\Bbb Q$
Very rough proof sketch: Let $\alpha=\cos(20^\circ)$. It turns out that $8\alpha^3-6\alpha-1=0$; it's the root of a cubic equation.
 
Yeah... I'm technically still in high school...
I have only done calc 1 & 2 by myself out of enthusiasm xD
 
Hi everyone
Can someone tell me what will be the general formula for tan(a+b+c+d......+n)
 
OK @Swarup
 
3:06 AM
@AkivaWeinberger But actually, I heard of this too! I heard it was a famous problem for a while. But isn't it actually a group theory problem?
 
It's to do with a field called Galois theory. A lot of Galois theory is about connecting things called fields to groups. But for this I don't think you need groups
Do you know what fields are?
They're sets of numbers that are closed under addition, subtraction, multiplication, and division (except division by zero)
For example: It turns out that, if $a$ and $b$ are rational, then $\dfrac1{a+b\sqrt2}$ equals $c+d\sqrt2$ for rational $c,d$
 
Yep, I know what fields are. But I don't know things beyond that (rings, and... and... well things like that).
 
So $\{a+b\sqrt2:a,b\in\Bbb Q\}$ is a field
 
I see
 
When I say it's a "vector space over $\Bbb Q$", I mean (roughly) I can specify its elements by lists of rationals (in this case, two rationals, $a$ and $b$)
It's a two-dimensional vector space over $\Bbb Q$
Similarly, $\{a+b\sqrt[3]2+c\sqrt[3]4:a,b,c\in\Bbb Q\}$ is also a field
(division isn't 100% obvious)
It's a three-dimensional vector space over $\Bbb Q$
Puzzle: write $1/(1+\sqrt[3]2)$ in that form
@Swarup Here's some notation. Write $\Bbb Q(\sqrt[3]2)$ to mean the smallest field containing the rationals and $\sqrt[3]2$
 
3:16 AM
@AkivaWeinberger Yep, (roughly) it sounds like a function...
 
It turns out that $\Bbb Q(\sqrt[3]2)=\{a+b\sqrt[3]2+c\sqrt[3]4:a,b,c\in\mathbb Q\}$
and so $\mathbb Q(\sqrt[3]2)$ has dimension $3$ over $\mathbb Q$.
So, back to geometry
 
That links a tuple of two numbers to another number... but I guess the interesting details really lie in the abstraction that comes from more advanced subjects like LA, Number Theory, Analysis...
 
I mentioned that $\alpha=\cos(20^\circ)$ satisfies $8\alpha^3-6\alpha-1=0$. It's the root of a cubic equation. (I'm skipping details, but it ultimately comes from the angle addition formula)
So it turns out that$$\mathbb Q(\cos(20^\circ))=\{a+b\cos(20^\circ)+c\cos^2(20^\circ):a,b,c\in\mathbb Q\}$$
It's dimension 3
(this comes from how it's a root of a cubic equation; again, skipping details)
(It turns out that it's important that the cubic equation is irreducible: it's not the product of two equations of smaller degree)
(I won't prove this)
So. About geometry
Theorem: Say you start with a line segment of length 1, and you have a straightedge and compass
and you manage to construct a line segment of length $x$.
Then the dimension of $\Bbb Q(x)$ is a power of 2.
Corollary: You cannot construct a line segment of length $\cos(20^\circ)$
 
Did someone look at my problem ?
 
Corollary: You cannot construct a 20 degree angle (if you could, you could use it to make a segment of length $\cos(20^\circ)$)
@ronakjain I don't know the answer
 
3:22 AM
Suppose $X_1, X_2, \cdots$ are independent random variables and $X_1', X_2', \cdots$ are independent copies such that $X_i'$ has the same distribution as $X_i$. Then variance of some function $Z = f(X_1, X_2, \cdots)$ is bounded by $\sum_{i = 1}^\infty \Bbb E[(Z_i - Z)_+]^2$ where $Z_i = f(\cdots, X_i', \cdots)$, replacing the $i$-th random variable by it's independent copy.
That is to say, variance of the function can be bounded by computing how much $f$ depends on each individual variable
 
Why can't I, solely because $\alpha$ is the solution of a cubic equation?
 
Because 3 is not a power of 2
 
@AkivaWeinberger This is an (easy) exercise in my algebra book. :)
 
I didn't prove the theorem
 
Oh... I see
 
3:24 AM
To prove the theorem, it's helpful for me to bring up some more machinery
 
Thanks for giving me a rough outline though :)
 
Let's look at $\Bbb Q(\sqrt2,\sqrt3)$. This is the smallest field containing $\sqrt2$, $\sqrt3$, and the rationals
It's things of the form $a+b\sqrt2+c\sqrt3+d\sqrt6$
Every element can be represented by four rationals, so it has dimension 4… over $\Bbb Q$.
But! We can also write its elements in this form:
$(a+b\sqrt2)+(c+d\sqrt2)\sqrt3$
Every element can be represented by two things in $\Bbb Q(\sqrt2)$.
So what this means is, $\Bbb Q(\sqrt2,\sqrt3)$ has dimension 2 over $\Bbb Q(\sqrt2)$.
This is the first time I talked about dimension over something other than $\Bbb Q$.
Some notation: write $[\Bbb Q(\sqrt2,\sqrt3):\Bbb Q(\sqrt2)]$ to mean the dimension of $\Bbb Q(\sqrt2,\sqrt3)$ over $\Bbb Q(\sqrt2)$.
And in general, $[G:H]$ for the dimension of $G$ over $H$.
Then:$$[\Bbb Q(\sqrt2,\sqrt3)]=[\Bbb Q(\sqrt2,\sqrt3):\Bbb Q(\sqrt2)]\cdot[\Bbb Q(\sqrt2):\Bbb Q]$$
$$4=2\cdot2$$
In general, $[G:K]=[G:H][H:K]$, where $G,H,$ and $K$ are fields
Now we're getting pretty deep into Galois theory
But I want to tell you this to tell you where the "powers of 2" come from
Think of a ruler and compass construction. Think of the x- and y-coordinates of those points, and think of the field generated by all of those coordinates
Every time you draw a new line or circle, you construct new points (the intersections with the lines and circles you've previously drawn)
So you can consider $\Bbb Q($all the (coordinates of the) points you've constructed$)$
and we want to know its dimension over $\Bbb Q$
It's simpler to ask for its dimension over $\Bbb Q($all the points you constructed until a step ago$)$
(until you drew that last line or circle)
Let $S_n$ be all the (coordinates of the) points you created up to and including the $n$th step of the construction.
Then it turns out the field $\Bbb Q(S_n)$ either equals $\Bbb Q(S_{n-1})$, or it has dimension $2$ over $\Bbb Q(S_{n-1})$
$[\Bbb Q(S_n):\Bbb Q(S_{n-1})]=1\text{ or }2$
(The main reason is, when you intersect a circle with a line or a circle, to get the coordinates of the new points, you usually have to solve a quadratic equation)
So, assuming we accept that, then$$[\Bbb Q(S_n):\Bbb Q]=[\Bbb Q(S_n):\Bbb Q(S_{n-1}][\Bbb Q(S_{n-1}):\Bbb Q(S_{n-2})]\dotsb[\Bbb Q(S_1):\Bbb Q]$$is a product of a bunch of $1$s and $2$s, so it's a power of 2
If you could construct $\cos(20^\circ)$, then $\Bbb Q(S_n)$ would contain $\Bbb Q(\cos(20^\circ)$, so we could ask what $[\Bbb Q(S_n):\Bbb Q(\cos(20^\circ)]$ is.
But$$[\Bbb Q(S_n):\Bbb Q]=[\Bbb Q(S_n):\Bbb Q(\cos(20^\circ)][\Bbb Q(\cos(20^\circ):\Bbb Q]$$
$$\text{power of 2}=[\Bbb Q(S_n):\Bbb Q(\cos(20^\circ)]\cdot 3$$
$3$ isn't the factor of any power of 2
So contradiction. The conclusion is that $\Bbb Q(\cos(20^\circ))$ isn't a subfield of $\Bbb Q(S_n)$ (where $S_n$ is the numbers we constructed with a straightedge and compass), so $\cos(20^\circ)$ isn't in $S_n$, so we can't construct $\cos(20^\circ)$.
 
3:49 AM
fuck...
 
@Swarup It's OK if you didn't get all that
 
I'll try understanding it!
 
Also, it's not obvious how to define "dimension"
 
No, we actually had a load shedding :( so I couldn't get here for a while...
I'll go on and read it
 
The main idea for that section is, I kept on saying "dimension over $\Bbb Q$", can you have dimension over something other than $\Bbb Q$? (Yes)
$\Bbb Q(\sqrt2,\sqrt3)=\{x+y\sqrt3:x,y\in\Bbb Q(\sqrt2)\}$
(I did not prove that $[G:K]=[G:H][H:K]$. This is not obvious and requires proof.)
 
3:57 AM
Good Morning
How many of you all giving JEE this year?
 
Oh man... all of this sounds pretty tough :(
 
Also, I'm not totally mentally stable in lockdown
Pretty sure won't make it through JEE this year.
May need to take a year off for it :-(
 
If I manage to construct a line segment of length $x$, how does that imply that the dimension of $\mathbb{Q}(x)$ is a power of 2?
Ahh forget it, don't answer me :( a FAIR amount of grip in fields is prolly needed to grasp all that, which I don't think I have...
 
@Swarup By induction
 
@AkivaWeinberger Is that something related to topology or what?
 
4:02 AM
Well hold on
First we prove $\Bbb Q($_everything_ we've constructed so far$)$ is a power of 2, by induction. I called that $S_n$
Then, since $x\in S_n$, I know the field $\Bbb Q(x)$ is a subset of $\Bbb Q(S_n)$
so I can ask what the dimension of $\Bbb Q(S_n)$ over $\Bbb Q(x)$ is
By the multiplication formula I stated but didn't prove, $[\Bbb Q(S_n):\Bbb Q]=[\Bbb Q(S_n):\Bbb Q(x)][\Bbb Q(x):\Bbb Q]$
On the left side of that equation we have a power of two
so the two things on the right side of it have to multiply to that
so they're factors of a power of two
If you're a factor of a power of two, you're a power of two.
So $[\Bbb Q(x):\Bbb Q]$, the dimension of $\Bbb Q(x)$ over $\Bbb Q$, is a power of two.
@Swarup In any case, hopefully you at least have a rough idea of how it goes. Eventually you'll learn enough to fill in the gaps. With experience comes understanding
 
0
Q: Is a 2:1 Lissajous orbit possible in the Circular Restricted Three Body Problem?

uhohWas Queqiao in a halo or Lissajous orbit? Why do sources disagree? says Proper halo orbits have the same period for their in-plane oscillations and out of plane oscillations, so they are closed orbits with roughy circular motion in the rotating frame, whereas Lissajous orbits are those where the...

 
4:51 AM
Give a man a fish and he'll have food for a day. Give a fish a man and it'll have food for the rest of its life
 
@AkivaWeinberger <insert you had me in the first half ngl meme>
 
@BalarkaSen Idea for finitely many variables: Say $Z = f(X_1, \cdots, X_n)$. Look at the martingale differences $M_i = \Bbb E[Z|X_1, \cdots, X_i] - \Bbb E[Z|X_1, \cdots, X_{i-1}]$, so that $\sum_{i = 1}^n M_i = Z - \Bbb E[Z]$.
 
@BalarkaSen ooo ISI probability gawd
:P
 
probability is very good
Say $i < j$, then $\Bbb E[M_i M_j] = \Bbb E[\Bbb E[M_i M_j|X_1, \cdots, X_i]] = \Bbb E[M_i \Bbb E[M_j|X_1, \cdots, X_j]]$.
 
Hi everyone ! Can someone tell me that how can I proof that for two quadratic equations to have both roots same the only condition is that therecoefficient should be proportional ?
 
5:05 AM
@ronakjain use factor theorem
ie if $P(a) = 0$ with mulitiplicity $m$ then $(x-a)^m$ divides $P(x)$
 
@Lelouch Actually surprisingly the probability courses here are terribad
 
@Lelouch can you proof ? I am not able to understand that
 
@BalarkaSen huh, didn't expect that
 
yeah i mean its just basic stuff
 
@ronakjain Well, if $\alpha, \beta$ are roots of $Q(x)$, then $(x-\alpha)(x-\beta)$ divides $Q(x)$. Now expand what divisibility means and you're done
@BalarkaSen CLT/Martingales were done ?
 
5:09 AM
@Lelouch ok. I got that. Thanks
 
CLT is in the course, but since there's no measure theory you have to skip some details (i think the proof is optional, but thankfully was taught). there's nothing on martingales
there's a stochastic process elective that i'll take the next semester
 
But can you solve a one more problem. Can you tell me how to prrof the condition for one common root of two quadratic equations ?
 
can you recommend some books or something to read for probability, which is more into intuition than measure-theoretic stuff? I'm traumatized by the prob course done here
 
durrett
thats the holy bible
 
ooh, that looks cool. thanks
 
5:12 AM
cmi has probability? damn
i thought you guys just do algebra lol
 
@BalarkaSen it has in second sem, but I didn't like the way it was done. Basically 80% was what I felt unnecessarily formalism instead of actual probabilistic intuition. Some parts I liked though (eg: Delhi scandal, probabilistic proof of Weirstrass)
 
whats the delhi scandal lmfao
there should be more measure theory in our courses
 
ok, so Karandikar taught the course. He's a pretty pro probabilistic
*probabilist
 
ah ok
 
so there was once a scandal in Delhi engineering enrance
the test were rigged or something
 
5:14 AM
you mean he's pro-bability
 
he was on the team to detect if it was fraud or not
he told how he figured that out
I mean it was babied down but I liked it
 
ugh no stat in my town man
miss me with that crap
 
@BalarkaSen huh ?
 
i dont give a shit about stat lol
karandikar came here to give some stat talk, i fell asleep
 
yeah he dumbs down things too much for "intro" talks
 
5:16 AM
the stat courses here are so annoying
 
are they mandatory ?
 
its like a gigantic waste of time
yeah
 
can you take elective in third sem ?
 
yes
 
what did you take ?
 
5:17 AM
oh wait no, we can take elective in third year; so that'd be 5th and 6th sem
 
@BalarkaSen oh rip
@BalarkaSen not even in 4th sem lol ?
 
nah
 
enjoy stat then :P
 
but im in 5th sem now (or will be, whenever this thing starts)
 
@BalarkaSen they should make some exception for you ?
 
5:18 AM
no why should they
i mean i dont care much i can just read something
 
@BalarkaSen Well here normally people can take electives in fourth sem, but if you have ok-ish performance, you can take in third sem, and if you're really pro you can take in second sem (Mohan took diff geo)
 
Oh like that, yeah they asked me if I want to skip some courses, but I'd have to take the exam anyway
So I said screw it
Either let me skip the entire course or I'll just sit for it
Not going to prepare for the exam if I am skipping the course
 
I mean, isn't it a huge waste of time to sit through the course if you can test out with little prep ?
is attendance mandatory or smth
 
I am not going to read for shit courses if I don't sit for the course; like sitting for classes is half the preparation done anyway
and I didn't want to skip serious math courses because why not make a solid foundation
I learnt a lot from sitting in really simple courses like linear algebra even
 
How do you manage to properly learn through the courses you already know everything about?
I know like 70-90% of the stuff that's happening a priori, but the remaining 30-10% is important but I end up getting bored so I miss them.
 
5:24 AM
@Lelouch can you tell me proof for a common root of two quadratic equations ?
 
i dunno, there's always new things to learn
 
@ronakjain The resultant would be zero
compute the resultant
 
@Lelouch I did not get this. Can you please give a explanation
 
In mathematics, the resultant of two polynomials is a polynomial expression of their coefficients, which is equal to zero if and only if the polynomials have a common root (possibly in a field extension), or, equivalently, a common factor (over their field of coefficients). In some older texts, the resultant is also called the eliminant.The resultant is widely used in number theory, either directly or through the discriminant, which is essentially the resultant of a polynomial and its derivative. The resultant of two polynomials with rational or polynomial coefficients may be computed efficiently...
speaking of linear algebra, how will you motivate the proof of spectral theorem ?
 
just do it for normal operators
 
5:27 AM
@Lelouch I am just preparing for JEE. And all that you posted seem to be non understandable to me. Can you explain thst in your language ? I just want the condition for two quadratic equations
 
@Lelouch Quickest proof of spectral theorem for normal operators is to show that generalized eigenvectors of normal operators are eigenvectors, so the Jordan canonical form is actually diagonal, and checking by hand that eigenvectors are all orthogonal
Normal operators is the optimal condition, so everything becomes clear if you use just that much hypothesis
 
@ronakjain The main idea is that if $f(x)$ and $g(x)$ have a common root, then you can find linear $p(x), q(x)$ with $f(x)p(x) + q(x)g(x) = 0$ (why ?). This can be stated in terms of solving linear equatoins (how/why ?). Now rest is using a system of linear equation has a nontrivial zero iff the determinant is zero (you can blackbox this fact ig)
 
Round $n+\sqrt n$ to the nearest integer. It is never square
 
OK man @Akiva
 
In fact, $n+\langle\sqrt n\rangle$ is the nth nonsquare number
 
5:34 AM
Nobody cares
 
I'm surprised
 
@BalarkaSen um, yeah but how do you a priori get that all eigenvalues do lie in $\mathbb{R}$ without mimicking the proof of real spectral theorem ?
 
What? Having eigenvalues in $\Bbb R$ is obvious
 
wait why ?
nevemrind, ofc
 
If $T$ is normal, $T^* T$ is symmetric, which has real spectrum
 
5:38 AM
yeah, sorry I realized it was obvious immidiately after asking it
 
I need help formatting plain text with spaces in an exponential. Can anyone help?
 
There are also deformation proofs; normal operators which have multiplicity in the spectrum can always be wiggled a little so they have a simple spectrum
for which spectral theorem is obvious
and these kind of proofs work for arbitrary fields if you use Zariski topology
 
@BalarkaSen Wiggled as in, the set of the such operators are dense ? (like an way to prove CH is to show diagonalizable operators are dense in Zariski topology)
 
yeah
 
@Manan $a^{\text{blah blah $b$ blah}}$
Like that?
a^{\text{blah blah $b$ blah}}
 
5:42 AM
I would say the most important thing I have learnt in my linear algebra course is how to think about Hermitian inner products
that shit is nonobvious (TM)
 
@BalarkaSen How are you going to generalize the notion of a bilinear form to arbitary fields ? Matrices like $\begin{bmatrix} 1 & 1 \\ 1 & 1 \end{bmatrix}$ are nilpoitent in $\mathbb{F}_2$
 
yeah nonzero characteristic is a problem; but sometimes you can pass to the algebraic closure
the details depend on what you want to do
 
@AkivaWeinberger take a look at $\left \lfloor{n + \sqrt n + \dfrac{1}{2}} \right \rfloor$
 
@BalarkaSen btw, this is a nice problem, you can try if you don't know about it: Determine all possible values of $[\overline{K}:K]$
the answer is $1, 2, \infty$
 
i don't have a clue on how artin proved that
if it's proper and finite, then we have the complex numbers from bizarro world o_o
 
5:47 AM
@Lelouch yeah believable
 
@BalarkaSen How do you think about it? The way I think of it is having a matrix $M$ with $\langle v, w \rangle = v^T M w$
@BalarkaSen it's not very easy to proof though, atleast the (only) proof I know is quite involved
 
yeah i guess this has to do with formal reality and so on
i can believe this is hard
 
formal reality ?
 
@Lelouch the real part is an actual inner product, the imaginary part is a symplectic form
Formally real fields are where -1 is not a sum of squares; it should be possible to prove that formal real closures have infinite degree over the base
whereas formally real closed fields have degree 2 algebraic closure
formal reality is also the same thing has having an order structure, but maybe this is not relevant
 
These are all relevant. It's not hard to finish from here assuming A-S.
 
5:54 AM
whats A-S
 
I'm bit surprised how did you think of formally real fields so quickly, I thought that was the hard part
@BalarkaSen Artin-Schreier
 
this is some relevant exercise in dummit foote
 
oh
 
@Lelouch oh ok i dunno this, x^p - x - a shit?
i thought that was char p garbage
 
@BalarkaSen no, Artin-Schreier is literally what I asked to prove
if you assume some other characterization of formal real field
 
5:57 AM
Um, huh?
See Artin–Schreier theorem for theory about real-closed fields.In mathematics, Artin–Schreier theory is a branch of Galois theory, specifically a positive characteristic analogue of Kummer theory, for Galois extensions of degree equal to the characteristic p. Artin and Schreier (1927) introduced Artin–Schreier theory for extensions of prime degree p, and Witt (1936) generalized it to extensions of prime power degree pn. If K is a field of characteristic p, a prime number, any polynomial of the form X p −...
Oh there are two Artin-Schreiers
lol
 
Ok I didnt know these nutcases did formally real fields
 
Thanks @AkivaWeinberger - I found on TeX SE $\textsuperscript{text goes here}$
 
E[E[Z|F]|G] = E[Z|G] if G is a sub sigma-algebra of F, right? lol
Of course
Too hard to keep track of garbage
 
6:15 AM
@Manan doenst look too right
 
6:58 AM
if $K/L$ is Galois and $L/F$ is Galois, then $K/F$ is Galois, right?
separability is ok, and I'm too sleepy to write down normality
 
7:16 AM
Take $F = \Bbb Q$, $L = \Bbb Q(\sqrt{2})$ and $K = \Bbb Q(\sqrt[4]{2})$
 
that's a good one. thanks.
 
7:32 AM
@LucasHenrique It's as good as $^{\text{}}$
 
$\pi=2.34129...$
 
9:08 AM
By going through the Artin-Schreier stuff you should also get a almost completely algebraic proof of the fundamental theorem of algebra
 
9:52 AM
@Alessandro Here's what I was confused about earlier. If you throw away a $1/n$-ball around $1/n \cdot \Bbb Z^2$ in $\Bbb R^2$, and take the pointed GH limit, it converges to $\Bbb R^2$ because the metric on $\Bbb R^2 - \Bbb Q^2$ and $\Bbb R^2$ are comparable; the infimum distance between two points on $\Bbb R^2 - \Bbb Q^2$ is the same as that of $\Bbb R^2$
But take some other measure 0 set, let's say even a straightline segment $L$ in $\Bbb R^2$. $\Bbb R^2 - N_{1/n}(L)$ does not pointed GH converge to $\Bbb R^2$
Because the metric on $\Bbb R^2$ and $\Bbb R^2 - L$ are not comparable. The GH limit introduces a bulge near $L$
This is an interesting example to me
I think the GH limit is what you get if you cut $\Bbb R^2$ along the the segment $L$ and "separate" the two flaps
 
10:25 AM
@BalarkaSen wait why?
Which metric are you using on $\Bbb R^2\setminus N_{1/n}(L)$?
 
Take two points on the opposite sides of $L$, the distance between them in the interor metric of $\Bbb R^2 - L$ is not the same as the one on $\Bbb R^2$
@Alessandro The length metric, not the subspace metric. Should have made that clear.
I only care about geodesic metric spaces
 
Ah ok, makes sense then
 
You agree with my picture of the GH limit, yeah?
slit the plane along the segment $L$ and separate the flaps
like you do in branch cuts to construct riemann surfaces
 
So the point is that the first set is made of isolated points, you don't waste any time walking around them
 
yeah
it doesn't locally disconnect the ambient
 
 
1 hour later…
11:32 AM
I don't think A-S helps with the FTA
or am I missing an obvious a priori reason why $\overline{\mathbb{R}}/\mathbb{R}$ should be finite?
 
(removed)
 
12:01 PM
Hello there
 
(removed)
after u say hello u post question
 
Hi I have kind of a dumb question, that I don't think is meaningful to make a post for. In this question math.stackexchange.com/questions/2837202/… I am having a lot of trouble understanding what $\partial f(x) = \{\nabla f(x) \}$ means. The squiggly parenthesis are especially confusing me because it makes it look like $\partial f(x)$ is now a set with a single element?
 
looks like nonsense to me
 
littleO's answer is also confusing me because it says if f is differentiable, but I don't see how you get meaning out of \nabla without the function being differentiable in the first place?
 
please how I read latex (ಥ_ಥ)
 
12:11 PM
ah, I see, it does make sense
$\partial f(x)$ is the subderivative and, as such, a set
@Specter see top right corner
 
Ah I've never heard of a subderivative before. I will have to figure that out then
I think I see what is going on now. So a subderivative always lies under the graph of f which isn't necessarily unique. But if the function is differentiable and convex, then it is unique and equal to the gradient?
 
yeah
 
Thank you so much for the help
 
12:26 PM
it works it works! it fails to work
why don't sem create chat like this
 
12:39 PM
@Thorgott because it is real closed
The algebraic closure of a real closed field is always a degree 2 extension, that's part of what A-S gives you
 
I don't know the real closed stuff, but from which property of $\mathbb{R}$ does this follow?
 
@Alessandro @Thorgott The analysis lies in showing R is real-closed
 
The proof I know needs that odd degree polynomials with different sign values on a and b have a root in [a,b], which is why I said almost algebraic
@BalarkaSen or in showing an equivalent characterization of real closed, depending on your definition R could be real closed by definition :P
 
being real-closed is equivalent to every odd deg poly having a root in the field, and every element to be either a square or - a square
@Alessandro give me one definition of real closed where its obvious that R is real closed without any analysis
 
I mean, I know the standard Galois-theoretic proof of the FTA, but I don't see how to do it with A-S
 
12:50 PM
the point is real closed is equivalent to not being algebraically closed by immediately being algebraically closed once you adjoint square root of -1
 
@BalarkaSen a field is called real closed if it is elementary equivalent to the real numbers
 
FTA is baked in there
@Alessandro oh not a logic definition man
come on
you'll do some model theory trick on me
 
yeah, but why is $\overline{\mathbb{R}}/\mathbb{R}$ finite
once we have that, A-S does give us the FTA
 
F real closed implies F(sqrt(-1)) is algbebraically closed man
 
12:53 PM
That's equivalent to being real closed actually
 
overline F = F(sqrt(-1))
 
so why is $\mathbb{R}$ real-closed then, whatever that means
substituting tautologies isn't gonna give us a proof
 
because every odd degree polynomial has a root in R
that implies real closed
just read the real closed stuff man its in dummit foote as an exercise
 
that sounds like it's basically the standard Galois proof of the FTA
 
yeah it is
 
12:55 PM
ok, so A-S doesn't really give us a different proof of the FTA
 
thats right
there is no interesting algebra proof of FTA
 
the standard one is nice tho
 
meh
just do loopy loop
 
ok, can't argue with that
 
lmao
 
12:57 PM
but still better than the elementary proof
 
the loopy loop proof actually gives proof for quaternions as well
so its very superior
 
does it work on real closed fields?
 
Isn't there a proof for quaternions using that they are basically a union of slices that look like C?
 
yeah
by Cullen-regularity of polynomial functions
lmao
 
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