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12:00 AM
That's a pretty standard problem. I recommend a more modern book these days — Friedberg, Insel, Spence.
 
Hmm, not familiar with that one
 
Here's a problem involving similar ideas: if $T$ is a normal operator on a Hermitian space $V$, then $T^*$ is a polynomial in $T$
 
It was disappointing when we put the simultaneous diagonalization of commuting diagonalizable operators on the algebra qual and NO ONE had a clue. I was livid. (It appears numerous times on previous quals, but students have a way of "praying" things they don't know won't show up.) Only one or two people even mumbled eigenvectors.
That was the last qual I co-wrote before becoming a bum.
 
Huh, strange
It's such a natural result
 
Basically, the grad students hate/avoid linear algebra. Guess none of them want to do representation theory or geometry or applied math.
 
12:05 AM
I don't understand that sentiment. Linear algebra is so deep and vast. I remember there being a popular saying that one can never know enough of it
 
I'm not condoning or explaining it.
 
It's everywhere
 
I remember a professor told me once that in math the only things you know how to do are linear algebra and kinda combinatorics, and that you try to reduce other problems to those problems
 
was that Babai
 
Sounds like it.
 
12:07 AM
Nope, I guess it wasn't quite a professor, more a postdoc working in algebraic topology
 
Those aren't the only things I know how to do, for sure. And I certainly don't do combinatorics very well.
 
I should learn combinatorics one of these days
 
It was basically setting up to, in order to do topology you usually either put a manifold structure and do linear algebra or some complex to do combinatorics
 
I'm not sure I consider the "linear algebra" of homology combinatorics at all.
 
simplicial sets :3
 
12:09 AM
I mean, there is a "combinatorial" structure to the simplicial structure, but ...
 
@Daminark what about model categories tho
:3
 
If you try hard enough that's also one of the two
 
does J P May agree
 
Nah jk idk, but yeah I will say I did not pick out any of the combinatorics Babai taught me in AT, maybe I'm just not there yet or maybe it's only kinda combinatorics, sorta like what Ted said
Never asked him about that specifically
 
The only spaces that exist are CW complexes
 
12:12 AM
Demonark: They refer to combinatorial structure if you can do things in terms of the simplicial structure. One of the big things when I was in grad school was a Russian paper on the combinatorial way to compute Pontryagin classes.
 
There are big function spaces which aren't CW complexes yet have good homotopical properties
 
Are vector spaces CW complexes?
 
eg Whitehead's theorem pushes through for Frechet manifolds
@Ted Dami-level joke
 
I wasn't meaning to be joking.
 
They aren't finite CW complexes but I guess if you fill in a lattice maybe?
 
12:16 AM
I'm not sure the topology works right, but I dunno.
 
What are we talking about? Vector spaces are cells
 
I've gotten this far in my life not thinking about infinite CW complexes, so I'll stay content.
 
Oh, infinite dimensional
 
OK, @Balarka, and in infinite dimensions?
 
Is anyone here familiar with the Riemann-Roch theorem for curves?
 
12:17 AM
Yes.
 
@TedShifrin Sure, you can realize it as a direct limit of finite-dimensional subspaces.
 
Hmmm, how does that work as a CW complex?
For example, the unit ball will often be non-compact ...
 
Give $\Bbb R^{n+1}$ a CW structure in which $\Bbb R^n$ is a subcomplex (this is easy, Daminark's lattice construction works).
Then it's $\bigcup_{n \geq 0} \Bbb R^n$
Still a CW-complex
 
Hmmm ... This seems to require CH or something.
 
@TedShifrin - Has anyone written a good "narrative" account of what it's saying? I understand sheaves from a logical point of view, but my broadly geometric experience stops at introductory differential equations and complex analysis; but I'm trying to understand Riemann-Roch against my better judgment....
 
12:22 AM
What if my vector space isn't $\aleph_0$-dimensional?
@Malice: Phillip Griffiths has beautiful explanations in terms of the geometry of the osculating spaces to the canonical embedding of the curve.
You can find this on pp. 12 ff. of Geometry of Algebraic Curves, Volume I, by Arbarello, Cornalba, Griffiths, and Harris. It's also in Griffiths & Harris.
 
Excellent, thank you. I'll give those a look.
 
You're welcome.
Also, look at Griffiths's Introduction to Algebraic Curves. Very classical. Nothing sheaf-y.
 
The classical stuff is actually my stumbling block :P
 
@TedShifrin Ok yeah the topology is a problem; I had standard $\Bbb R^{\Bbb N}$ in mind, no weird general sort of topological vector spaces. By what I said, a separable Hilbert space has a dense subspace which is a CW-complex. I don't know beyond that.
 
LOL, @Balarka. I will continue not to think about it.
 
12:27 AM
Me neither. Subtle point. Interesting.
 
I've done diffeq and complex, but my geometric intuition stopped at first year calculus. But I've done research in categorical logic, because that actually makes sense...
 
So Peter subbed for the first day of Shmuel's AT class and in office hours I remember seeing them have a somewhat similar exchange
 
Too bad you never learned multivariable calculus or differential geometry. Pretty hard to do higher dimensional geometric stuff without those.
 
Multivariable I've done.
But not differential geometry.
 
Geometric intuition has to come from multivariable.
Demonark: Similar to what Balarka and I were just mumbling about?
@Malice: You certainly don't need fancy differential geometry for this, but thinking about curves and surfaces in 3-space builds lots of intuition.
 
12:30 AM
Peter said on day 1 that every group arises as the fundamental group of some space, by just attaching disks along relations to a bouquet of circles. Shmuel was like well that gives you finitely generated (presented?). For a second Peter was like, wait why? Shmuel asked "What's the topology on an infinite bouquet of circles?" and Peter was like oh
 
Right.
 
Lol
 
Claim: If $Y$ is a proper linear subspace of a TVS $X$, then $Y$ has empty interior. Proof: By way of contradiction, suppose $y$ is some interior point of $Y$. Then there is some $U$ open such that $y \in U \in Y$ which implies $0 \in U-y = Y-y = Y$. Let $x \in X$ be arbitrary. Since $\{x\}$ is bounded, there is some $s > 0$ such that $\{x\} \subseteq s(U-y) \subseteq sY = Y$, so $x \in Y$, which is a contradiction.
How does that sound?
 
I made a comment here about the Hawaiian earring not being an infinite bouquet of circles.
Huh? @user193319?
 
What's the problem?
 
12:33 AM
What in the world is going on with $0\in U-y$, then $U-y = Y-y$, then $Y-y=Y$?
 
Looks fine to me modulo some notation
 
I'm working in a topological vector space.
 
And $U\in Y$ is of course wrong.
 
$Y-y = Y-\{y\}$
 
I know that.
Interior is in terms of $X$, first of all. So $U$ is open in $X$. What is going on?
 
12:34 AM
Oh, sure...$U \in Y$ is a mistake.
 
Wait aside from $U-y \subset Y-y$ and $U\subset Y$ what's wrong here?
He's using $A-B$ not as set difference but translating if that's the confusion?
 
Isn't it true that $y$ is an interior point of $Y$ if and only if there is some open set $U \subseteq X$ such that $y \in U \subseteq Y$?
 
So we're supposing $U\subset X$ is open and also $U\subset Y$. So those equals are $\subset$s?
 
@Daminark Well, I don't see why Shmuel's comment is a problem, though. I can still make a cell complex with number of 1-cells and 2-cells being likely some infinite cardinal.
 
@TedShifrin - I found multivariable strightforward so far as it went, but there must be some dot I never connected. Because complex was gibberish to me, even though I did reasonably well in it, and nothing's coming together for me with the algebraic geometry (I've been reading Vakil's notes and Hartshorne).
 
12:36 AM
Oh, crap...I made a lot of notational errors...
 
No, @Malice. Those are orders of magnitude far more advanced and sophisticated. You need a year of undergraduate algebra and then some graduate algebra to do algebraic algebraic geometry.
 
I've done a year of abstract algebra.
 
Doing it with Griffiths's approach you need some complex analysis, topology, and a bit of differential geometry, but it's still very sophisticated.
Oh. Well, you didn't say that.
 
The fundamental group on the bouquet is still free, and the relators get killed anyhow. You just need some transfinite version of van Kampen which is annoying.
 
I don't think of it as being geometric :P
 
12:37 AM
Here's a correction: By way of contradiction, suppose $y$ is some interior point of $Y$. Then there is some $U$ open such that $y \in U \subseteq Y$ which implies $0 \in U-y \subseteq Y-y = Y$. Let $x \in X$ be arbitrary. Since $\{x\}$ is bounded, there is some $s > 0$ such that $\{x\} \subseteq s(U-y) \subseteq sY = Y$, so $x \in Y$, which is a contradiction.
Is that better?
 
Algebraic algebraic geometry is more algebra than geometry. That's not how I think of it, because I'm a follower of the Griffiths style.
$U$ open in $X$, not in $Y$, @user193319. That's the whole complaint.
 
I never claimed that $U$ was open in $Y$.
 
But you're supposing that an open subset of $X$ is contained in $Y$. Make things clear.
 
Oh I guess for what it's worth I don't know the technical definition of a topological vector space, in normed spaces I obviously see why $\{x\} \subset s(U-y)$ and I'm just taking it on faith here that this translates over to TVS
 
I just said it was open in the ambient space.
 
12:39 AM
Actually, you never said anything of the sort.
This is why I lose patience.
 
Or, rather it was implicit that $U$ is open in $X$.
 
"implicit" ... bah.
OK, I will quit for now.
 
Whoa let's keep it friendly
 
After I've spent hours and hours helping you, feel free to be a rude ass.
 
Likewise, I know a reasonable amount of sheaf theory, but I know it as a logician, so thinking of them as geometric is weird to me. I think my instructor for this course was hoping the sheaf theoretic approach would play to my strengths, but it hasn't turned out that way.
 
12:40 AM
You never had to help. I was asking help from anyone who was willing to help.
 
Anyway, I found a copy of Griffths's Introduction to Algebraic Curves, so I'll see if that's better...
 
math.stackexchange.com/questions/242450/… I know this function locally invertible at non zero elements of $\mathbb R^n$ using Jacobian. But proving function injective. I used the standard technique. $f(x)=f(y) \implies x||x||^2=y||y||^2 \implies ||x||^3=||y||^3\implies (||x||-||y||)(||x||^2+||x|| ||y||+||y||^2)=0$
 
I don't know the right answer for you, @Malice.
 
Algebraic curves seem fun, should probably learn about them soon
 
Form this How do I prove that $x=y$?
 
12:44 AM
Oh, that works, @N.Maneesh. Unless $x=y=0$ the second factor can't be $0$.
 
@MaliceVidrine My opinion is that it's probably a good idea to learn some manifolds first to have some sense of 'local properties' vs 'global properties'
 
@TedShifrin - It's okay, I don't expect that there is one, much less that anyone would know it.
Mostly I'm just trying to track down any resource that has a story about this stuff. Like calculus has the story of looking at infinitesimal slivers of stuff, group theory has the story of symmetries and permutations.
I don't know what the story is here, yet.
 
I stand by my original suggestion, @Malice, but still you need to know about the canonical embedding (and it fails for hyperelliptic curves).
 
@TedShifrin From that I got $||x||=||y||$, But If $x, y\in $ a same sphere. This happens to be true. Right?
 
Now put that into your first equality.
 
12:46 AM
@loch - You're probably correct. What I'm in now is a directed study course described as "applied abstract algebra" for maths seniors, and I have not been pleased that it has turned out to be algebraic geometry.
@TedShifrin - I will definitely check it out. I do appreciate the suggestion.
 
It gives a concrete intuition, at the very least, @Malice.
 
Okay $x||x||^2=y||x||^2\implies x=y$
 
Right, @N.Maneesh.
 
Thank you@ Tedshifrin :)
 
(Assuming $\|x\|\ne 0$, but we already have no problem with $0$.)
 
12:48 AM
mmm
 
What does everyone think of the new proof by Maryna Viazovska and co.?
 
Perhaps here is some part of the story:
- Algebraic curves = 1-dimensional algebraic varieties (shapes cut out by polynomial equations) - in some sense they're the simplest (but non-trivial!) shapes you can study. (1-dimensional objects is easier than higher dimensional objects! )


- In studying geometry, one common thing to look at is the collection of functions (satisfying some properties) that you can define on your object. For algebraic varieties, the functions you care about are functions given by polynomials. If you're working over \C, you can think of holomorphic functions instead.
 
@Ultradark haven't heard of it, what was proven?
 
+1 @loch
 
Ah apparently a few years ago she seemed to solve sphere packing in dimensions 8 and 24 and has now generalized that result a fair bit
 
12:53 AM
@Daminark They proved that the configurations that solve the sphere packing problem in dimensions $8$ and $24$ also solve an infinite number of other problems about the best arrangement for points that are trying to avoid each other. The points could be an infinite collection of electrons repelling each other and
 
I don't know how many electrons are in dimension 8 or 24 ...
 
I'm not terribly familiar with sphere packing and related problems to be giving much of my sought after commentary but this sounds cool for sure
 
Sphere-packing certainly is a classic hard question. I haven't kept up with the progress. Some false results were obtained in the 70s-80s, if I remember correctly.
 
It seems like this is the paper in question: arxiv.org/pdf/1902.05438.pdf
 
@loch - Are you able to elaborate more on "look[ing at] the collection of functions ... that you can define on your object"? I think part of this is I don't really know what kinds of questions one would even ask about curves or functions on them.
(And I definitely appreciate that outline above. Even that last point about what Riemann-Roch is relating is more than was clear to me before)
 
1:06 AM
Well I think I passed
L
I got the questions that were obviously based on material we covered
 
Hmm maybe an application would help: if you're ever heard of elliptic curves - they tend to be introduced as curves defined by the Weierstrass equation y^2=x^3+ax+b, (in fact its homogenized version Y^2Z = X^3 + aXZ^2 + bZ^3) satisfying some conditions (to ensure that the curve is smooth).

But that's now how geometers think of elliptic curves - because having this dependence on the presenting equation can be awkward. For instance, if you take the chart Y=1, your equation now looks like z = x^3 + axz^2 + bz^3 - it's not clear now why this should be an elliptic curve using that definition!
 
@GFauxPas congrats!
 
@loch - Interesting. And, strangely, I understood most of that.
 
It helps to have examples
 
We'll see
I didn't know how to find the normal vector to a surface of a curvy line y=f(x) rotated around the x axis. And that ruined a hugely weighted question
 
1:24 AM
I hope I can end this course without being entirely scared away from the subject; it seems like it might have high points. But I'm pretty sure I'm going to fail unless we're only graded for effort... :P
 
2:13 AM
hi @loch
attending first conference ever today
very exciting
 
hi @Adeek
exciting indeed - what's the topic?
 
2:28 AM
@loch algebraic cycles
 
2:38 AM
i see
i hope you get to learn a bunch of cool math !
 
me 2. Just have to learn how to socialize properly haha
 
3:12 AM
Let $f:\mathbb R^n \to \mathbb R$ be a function defined by $L(x)=\langle x,y \rangle$ for $x\in \mathbb R^n$. I know that $DL(x)=L,\forall x\in \mathbb R^n$. right?
 
3:39 AM
What's $DL$ and what's $y$?
 
@GFauxPas $y$ is some fixed vector.
 
Presumably $y$ is a fixed vector, $f = L$, and $D$ is the derivative
 
ah
 
So, $DL(u)=DL(v),\forall u,v \in \mathbb R^n.$ Right?
 
I forgot the definition of a derivative of a functional. Is it supposed to produce a functional?
 
3:48 AM
Here, $L$ is a linear transformation. If $T$ is linear transformation. Then $DT=T$
 
oh its the best linear approximation operator
$f(x + h) = f(x) + Df(x)h + o(\Vert h \Vert)$ ?
 
Just to make sure it's conceptually clear
 
@Semiclassical @TedShifrin I got this question wrong on the final and I'd like to know how to do it
 
So if you have a function $f:\mathbb{R}^n\to \mathbb{R}$, then given $x_0 \in \mathbb{R}^n$, the derivative of $f$ at $x_0$, called $Df_{x_0}$, is going to be a linear map $Df_{x_0}:\mathbb{R}^n\to \mathbb{R}$ such that $f(x_0 + h) = f(x_0) + Df_{x_0}(h) + o(\|h\|)$
 
let $f: \mathbb R \supseteq [a..b] \to \mathbb R$ be a positive smooth function
let $E$ be the set obtained by rotating the curve $f([a..b])$ around the $x$-axis in $\mathbb R^3$.
What's the normal vector to $E$ at a point $(x,y,z) \in E$?
Your help is appreciated tia
 
4:00 AM
When you're thinking of the derivative as an operator, the idea is that you have a map $Df:\mathbb{R}^n \to L(\mathbb{R}^n,\mathbb{R}) = (\mathbb{R}^n)^*$ given by $Df(x) = Df_x$
 
well sure, the best linear approximation to a linear functional is the linear functional
I'm given an embedding
for $t \in [a..b], \theta \in [0..2\pi]$,
$\begin{pmatrix} t \\ \theta \end{pmatrix} \mapsto \begin{pmatrix} x = t \\ y = f(t) \cos \theta \\ z = f(t) \sin \theta \end{pmatrix}$
but not sure if the embedding is meant to help for this part or a later part of the problem
 
Isa
4:19 AM
What is $f^-$ in R? I know in $\overline{R}$ is the maximum of {0,-f(x)}
 
is the context integration?
 
Isa
yes, Lebesgue integral
 
then it's the negative part of $f$
In mathematics, the positive part of a real or extended real-valued function is defined by the formula f + ( x ) = max ( f ( x ) , 0 ) = { f ( x ) if...
oh you have the definition right there
it's the same thing
 
Isa
oh thank you. I was confused because for R, $f^+=\frac{f+|f|}{2}$
so I thought something similar would be for $f^-$
 
The WP page I posted has some identities
$f^- = \dfrac {f-|f|}{2}$
 
 
3 hours later…
7:50 AM
@EarthCracks 1 is true, I don't know what 2 means and 3 is true
More generally in 3 if you have $X=\mathrm{Spec} R$ and an $R$-module $M$ you can define a (quasicoherent) sheaf $\widetilde{M}$ as $\widetilde{M}(D(f))=M_f$ for all $f\in R$ ($D(f)$ is the usual basic open set $\{f\neq 0\}$, you get restriction maps from the universal property of the localization and a sheaf defined on a basis can be extended to a full sheaf
This is actually an equivalence of categories between quasicoherent $\mathcal O_{\mathrm{Spec R}}$-modules and $R$-modules (the inverse functor is the global sections functor $\Gamma(\mathrm{Spec} R,-)$), and you can check it sends free modules to free sheaves
 
8:19 AM
$\omega_1$ first ordinal that has a fundamental sequence longer than countable
 
Are you guys able to post pictures on the website?
 
use the upload button
 
it keeps failing "Failed to upload image; couldn't reach imgur"
 
Then try go to imgur and post the link from the picture there instead, it might be just some system hiccup
 
it doesn't allow, it needs to be on i.stack.imgur.com
just wondering if it's just me having the issue or if there is a problem with the website
 
8:27 AM
ok it does not work for me also, probably a website problem
 
ok, thanks for checking
 
8:55 AM
any pros of audio amp in here?
 
9:11 AM
How to see that $4x^2+6x+3$ not zero divisor in $\Bbb Z_8[x]$?
 
 
3 hours later…
12:28 PM
So, given the set of equivalence classes of finite groups (related by being isomorphic to each other), define a binary operation on this set to be where, given two groups, combining them gives you some type of product of the two groups (direct product, semidirect product, wreathe product). In the direct product case, this resultant structure is a monoid, if I'm not mistaken. Though, is there a type of product which would make the resultant structure a group in it's own right?
 
12:39 PM
Jun 27 '18 at 2:58, by Alex
You should really go about fixing a set of groups, and giving the set magma,semigroup, monoid structure etc. What do you want as an inverse?
Your biggest challenge is to define some kind of product such that you can produce an identity when you multiply two groups together. It is not clear how this can be done
 
 
2 hours later…
2:24 PM
I know that 1,2 are false.
I know that $(\nabla f)(x)=2(a_1x_1,a_2x_2,...,a_n x_n)=\vec 0\implies either a_ix_i=0\implies a_i=0 $or $x_i=0$. Hence $f=0$
(4) is false. right?
consider $f(x_1,x_2)=x_1^2-x_2^2$. $f(1,-1)=\vec 0$
but $(\nabla f)(1,-1)\neq 0$
Am I correct?
 
3:06 PM
Looks correct to me
 
okay. Thanks
 
3:25 PM
Does there exist a function $f:(0,1)\to\Bbb R$ that is twice differentiable such that $f$ bounded, $f'$ bounded but $f''$ unbounded?
 
$f'$ is bounded means uniformly continuos
 
omg! i did not know that!
So, can f'' be unbounded in my question, @N.Maneesh?
 
I am thinking
This was the firt thing I got .
 
alright
 
3:55 PM
I think $f(x)=\int_0^x\sin\left(\frac{1}{t}\right)\mathrm{d}t$ should work, though I also think there should be a less contrived example
 
4:08 PM
If $\{f_n\}$ is bounded in $L^1[0,1]$, is $\{f_n\}$ uniformly integrable over $[0,1]$? If it isn't, please don't give a counterexample.
 
4:46 PM
These are neat:
In recreational number theory, a narcissistic number (also known as a pluperfect digital invariant (PPDI), an Armstrong number (after Michael F. Armstrong) or a plus perfect number) is a number that is the sum of its own digits each raised to the power of the number of digits. This definition depends on the base b of the number system used, e.g., b = 10 for the decimal system or b = 2 for the binary system. == Definition == The definition of a narcissistic number relies on the decimal representation n = dkdk-1...d1 of a natural number n, i.e., n = dk·10k-1 + dk-1·10k-2 + ... + d2·10 + d1,with...
 
 
1 hour later…
user280247
6:04 PM
Hi, im with a naive question:
 
user280247
suppose have no knowledge of maths and for practical purposes measure with a stick three values
 
user280247
a,b,c
 
user280247
a is the angle of a right angled triangle, b and c the sides
 
user280247
suppose we measure it for a particular case $a_1$, $b_1$, $c_1$, is there any way to predict mathematically that for the same relation $b_i$,$c_i$ $a_1$ is the same?
 
6:40 PM
is $\lim_{n \to 0} \frac{1}{n}\sin \left( \frac{x}{n} \right)$ a function?
also is it a space filling curve?
 
 
4 hours later…
10:36 PM
Hi @Ted, @PaulPlummer
 
Hi @BalarkaSen
 
How's it going
 
Things are going okay, not being very productive though. You? how is college life?
 
meh @ college
The semester's over, I'm back home for some time.
 
I guess I had a small paper(and even smaller result) show up on the arxiv a few weeks ago
 
10:45 PM
Oh nice congrats
 
11:04 PM
What's repulsive but also attractive
 
11:18 PM
An electric charge.
 
Let $M$ is a field, $\alpha$ an element in some larger field, and $E = M[\alpha]$. If $f(X) \in M[X]$ is a minimal polynomial for $\alpha$, does it follow that $|E: M| = \text{deg } f$?
 
Yes; $E = M[X]/(f)$, which is an $\deg f$-dimensional $M$-vector space
 
Ah, that's good to know. I thought it was true. Thanks!
 
@user193319 Note that the usual notation is $E = M(\alpha)$. The notations $M[\alpha]$ and $M(\alpha)$ are equivalent when $\alpha$ is algebraic over $M$, while if $\alpha$ is transcendental over $M$ you have $M[\alpha] \cong M[X]$ and $M(\alpha) \cong M(X)$, which is a cool fact I guess
 
Oh, yes. You are right. I should be more careful.
 
11:40 PM
@ÍgjøgnumMeg I advocate thinking about $|E : M|$ as the number of $\overline{M}$-valued points in the scheme $\text{Spec} E$ lying over a fixed $\overline{M}$-valued basepoints in $\text{Spec} M$ instead of the dimension of the $M$-vector space $E$ :3
Also what a horrible notation for field, $M$
Use $F$ or $K$ or $k$ for Christ's sake
 
Obviously it should be $k$
$F/k$ is a finite extension, $K/k$ is infinite
 
Very natural
F for Finite
K for ... Knot finite
 
Gottem
 
woppah
 
11:43 PM
u r reading Schneps right
i want to read it too
 
Nooo I am reading Tamás Szamuely's book
 
Hey guys
 
Oh I forgot the author
"Galois Groups and Fundamental Groups"?
 
Hey @Daminark
Yeah that one
 
K that's the one I had in mind
 
11:45 PM
Ah yeah I remember I was gonna read that at some point, but as with many other things I intended to read, I sadly didn't
 
One of my old lecturers recommended it to me for some direction over the summer
 
Alas those reading lists that keeps getting exponentially bigger
I might read it next year second semester during my field and Galois theory course
 
Okay so funny thing actually, I was talking to a friend and have thought of an evil idea
If I'm teaching a class I'll try to assign a problem which for a nearly unreasonable task but the condition is subtly vacuous
For example, in differential topology I'd say something like "Let $M$ be a hypersurface in $\mathbb{R}^4$ with $\chi(M) = 2$. Show that $\pi_3(M) = \mathbb{Z}\times \mathbb{Z}/2$"
And just watch to see how many people freak before they get it
 
I hope you mean closed hypersurface!
 
Oh yeah closed lmao
 
11:51 PM
@Daminark hi
 
The Greeks used two tools to make different geometric constructions. Name the tools.
 
@Daminark I was wondering if you could help me with something ?
I need your second opinion
 
I'm always glad to give my sought after commentary on things but I'll probably need to know what it is before promising that my opinion has value :P
 
can I send you email ?
 
Go for it
 
11:53 PM
Does anyone here like operator algebras or, more specifically, von Neumann Algebras?
 
Compass and straight edge
 
Do you have mine?
 
can you send me your email and delete it after 1 min
no @Daminark
got it
 
You saw nothing!
:ghost:
 
sent it to you @Daminark
did you get it ?
 
11:56 PM
Yup
 
can you check if do you think there is anything to add I am gonna use it to apply for scholarships
 
@Daminark I see your email id is n.wildberger@unsw.edu.a
 
D:
u got me
 

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