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5:00 AM
@Kaumudi What is $n$?
 
@Josué an integer
 
@arctictern Right. I was just curious about exactly how his book is defining $n$. It's possibly arbitrary.
 
it's defining integers mod n
 
@arctictern Oh. Duh. You're right. Haha.
 
Is there anything flawed with my question?
1
Q: How do I solve this second-order homogeneous differential equation with piecewise constant coefficients?

TheGreatDuckI am trying to solve the following differential equation (for fun, mind you): $$\lfloor x \rfloor y'' + 2\lfloor x \rfloor y' + \lfloor x \rfloor y = 0$$ Because of the piece wise coefficients, my gut instinct is to first solve the associated implied differential equation. This means that I ca...

I want to make sure I didn't write anything confusing. This subject has a tendency to confuse people in my experience. Also, sorry for the large link.
 
5:10 AM
Wikipedia calls a topological space $X$ contractible if its identity map is null-homotopic. Consider the identity map $i$ on $\mathbb C^*=\mathbb C\setminus\{0\}$ and define $H:X\times[0,1]$ by $(x,t)\mapsto tx$. This looks continuous despite $\mathbb C^*$ not being contractible.
 
@Josué um what?
 
$H(x,0)\equiv0$ and $H(x,1)\equiv i$
 
@Josue Whwre does everything go at t=0?
 
user228700
@BalarkaSen I don't understand the definition is what I meant. (This is part of a question, so that is why I kept asking "What is it asking of me?", sorry.
 
@Kaumudi what part don't you understand? do you know what a relation is? do you know what <=> means? do you know what n|(a-b) means?
 
user228700
5:15 AM
No, I don't understand what $n|(a-b)$ means.
 
then say that
it means n divides a-b
i.e. n is a divisor of a-b, or a-b is a multiple of n
 
user228700
@arctictern OK, sorry. Thanks!
 
nvm
Oh, shoot, I forgot that the codomain must be $\mathbb C^*$. Ignore my naïveté, lol.
 
I will take that as a no then...
 
user228700
Does anybody know which set is represented by the letter $S$?
 
5:26 AM
I know s^2 is spherical plane
 
user228700
Um, no, I don't think that's what my textbook is going for...
 
context then?
cause it looks familiar
wait
 
user228700
Oh, nvm.
 
nevermind
It looks familiar cause that was the symbol I used for complex space when I was messing around. XD
I'd hope your textbook didn't somehow use the same symbol and meaning I made up on a whim. XD
 
I don't think there are universal letters for sets other than $\mathbb Z$, $\mathbb R$, etc., and those aren't even letters.
 
5:30 AM
well...
most people tend to think of them as Z and R
 
I've seen them written like that, but bolded.
 
I mean that most people call them "Z" and "R'
verbally not in writing
I know the symbols are different
 
I get you. I was defining a letter as being an element of the set $\{A,B,\dots,Z\}$, lol.
 
oh well that's silly.
the set of letters would be a set of geometric figures.
specifically, figures in the euclidean plane
built entirely from line segments
and circles
 
 
2 hours later…
7:19 AM
Interesting geometry question, a generalization of Pascal's theorem to three conics.
 
8:14 AM
We have seen many false "proofs" that 0=1... is anyone interested in a real proof?
 
I am not.
 
user147690
8:40 AM
@BalarkaSen And existence of these corresponds to having $w_2(M)=0$ right?
 
Yes.
 
user147690
@BalarkaSen I just gave a talk(on Wednesday) on SW classes for AT, and I was asked about these afterwards and didn't know them.
 
SW classes are good stuff. What did you learn?
 
user147690
I'd been looking at Milnor&S and I'd done essentially the first 4 chapters
 
Hi, btw. Tobias was looking for you a few days ago.
 
user147690
8:44 AM
So I haven't done Steenrod & Thom isomorphism yet
 
Me neither. Also working through Milnor-Stasheff here.
along w/ other stuff
 
user147690
Oh I see, thanks. @TobiasKildetoft I'll be online more frequently again, classes have ended and finals in 2 weeks.
 
user147690
@BalarkaSen I want to go through Serre's Linear representation theory over christmas and do most of the exercises from Dennis & Farb's noncommutative algebra
 
user147690
M&S is pretty nice
 
user147690
Still trying to work out what I will do for my honours thesis next year.
 
8:47 AM
@AlexClark It is. I am complementing it with Hatcher's notes, which is also good.
 
user147690
His K-theory and vector bundles?
 
Yah
I haven't made much progress on M&S the past few days because I was looking at some diffgeom. Maybe I should read a bit
 
user147690
A friend did his talk on Chern classes, using that as a main reference, but he had to blackbox some things. It was only a 20 min talk, so I just gave axioms, did some consequeces, showed whitney duality, and blackboxing cohomology of $\Bbb{RP}^n$ did all the whitney classes of $\Bbb{RP}^n$
 
user147690
(all in M&S as you'd know)
 
mhm
 
user147690
8:51 AM
I thought I'd need to speak very fast to cover all that, but I made 17 min :P
 
cool
 
user147690
@BalarkaSen What diffgeo?
 
9:24 AM
I wonder how do they get .2/1.9 = .08? I am getting something closer to .105.
 
 
1 hour later…
10:34 AM
> We often hear that mathematics consists mainly of "proving theorems." Is a writer's job mainly that of "writing sentences?" - Gian-Carlo Rota
4
 
that is a good quote
 
I like it and I hadn't heard it
overtly profound math quotes are what I live for
 
> If I have not seen as far as others, it is because there were giants standing on my shoulders.

--Hal Abelson
 
11:11 AM
what would be good way to motivate the tensor product for undergraduates?
something that scratches this very vague itch of "understanding what it is about"
I gave an exercise group on friday any they wanted to know, I felt the things I said in class were extremely unsatisfactory and told them I'd send them a write up today
 
11:40 AM
In.
 
@DHMO hi
After a long time
 
11:57 AM
Day 20+ on group theory:
The classical groups have very lengthy articles which highlight properties that are interesting in studying those groups, but not very helpful in creating a catalogue of group properties
 
@Ramanujan hi
 
12:48 PM
Hello.
 
@s.harp, is something near the universal property out of the question? Or, depending on what kind of tensor product you are teaching, extension of scalars?
 
@Mees the basic plan of what I'll do is like this:
1. given a basis of $V$, $W$ introduce $V\otimes W$ as a vector space having basis $e_i\otimes f_j$, show how terms $v\otimes w$ can be viewed as elements of this space. This way they have a feeling of how to manipulate vectors in the tensor product
2. Give a formal definition via a quotient of the free vectorspace on $V\times W$.
3. Explain how the tensor product lifts bilinear maps to linear maps, this being the primary reason we want to look at this thing, note that this uniquely determines the tensor product as VS
 
1:15 PM
explain the trace in terms of the tensor product
(real definition of the trace)
canonical isomorphism of M* tensor V with Hom(W,V) this is how you use tensors in differential geometry
where M=W lol
are they physics students?
 
yea they are 3rd semester physics undergrads
 
how about mention that if S,S' are quantum mechanical systemts with state spaces H, H' then the composite system has state space H tensor H'?
 
What is $F$? The dual space or something?
 
I'm sure you can explain that basically
but as far as i know it is an axiom
physically*
not basically
 
Actually, we knew in general $A\otimes B \neq B \otimes A$ but why in quantum people seemed to interchange the subsystems freely as if the tensor product is commutative?
 
1:19 PM
yes that is basically a consequence of $F(A)\otimes F(B) = F(A\times B)$ when $F$ is a suitable function space
 
Have they had any QM? If so, they might appreciate that e.g. $|00\rangle \otimes |01\rangle = |0001\rangle$.
 
tensor product IS symmetric
@Secret
 
@Secret because $A\otimes B \cong B\otimes A$
 
ah i see
 
perhaps you can also explain braiding
in the end the following constructions are the fundamental ones in linear algebra
direct sum; quotient space; Hom; tensor
 
1:21 PM
Maybe it's easier to start with general monoidal categories :-)
 
nothing more, nothing less
:D
tensor hom adjunction is also very useful to know
but seriously i think to explain it for modules would be more useful
because in differential geometry you readily encounter modules over C^infty(M), M some base manifold
 
this is a third semester analysis course for physicists, they do not like abstraction and need to have something they can immediately calculate with. Introducing it via basis is I think the best thing.
 
I definitely agree.
 
me too. in the end most we mentioned above is only useful in higher mathematics
 
Back.
 
1:26 PM
I like the definition of the trace, I need to show them that $\mathrm{Lin}(V,W)=V\otimes W^*$ for finite dimensional spaces to do that though. This is also nice, but I promised to send them my write up today, and at $8$ I have a date with alcohol
 
Maybe I underestimate physics students, but I don't think many would appreciate $\mathrm{Hom}(V,W) \cong V^* \otimes W$.
 
Ah, I messed up where the star goes
and if I look at their next exercise sheet they will need that statement, so looks like I gotta do it :S
 
Currently, I lost track of things whenever I saw the words "homology", "homotopy", "morphisms" in a body of text I am reading in maths
I still yet to make them more tangible to stay in memory
 
have you done complex analysis?
 
@Secret do you know Green's theorem?
 
1:36 PM
Never had the chance formally (due to undergrad class crowding), but I do end up reading a couple of lecture notes myself from other unis, thus I knew a couple of things from cauchy integrals to residuals

Green's theorm is taught in multivariable calculus courses
 
@Secret Cauchy's integral theorem?
 
yup
 
Another way of stating it is that "line integral is homotopy-independent"
would that help you develop some intuition on what "homotopy" means?
 
Wikipedia gave a nice pictorial intuition on homotopy It's when they start going into homotopy groups the whole thing become quite abstract as they are buried in those $\pi_i$ maps
 
alright
 
1:39 PM
When reading classical groups like GL, U, SO etc., this keep popping up
but they are relatively tame compared to the bazillon types of morphisms
Everytime I saw a group $G$ doing something like $\textrm{Aut}(G)$ my brain starting drawing arrow from a featureless sphere and it end up going nowhere
While I knew what Aut means, it is sometimes hard to follow all the morphisms of a group, let alone "visualise mentally" or folow by pen and paper its structure
Basically, I am bad at visualising something that is "in progress". Unlike things like groups, rings etc., which kinda "sits there" and then you investigate it, maps and morphisms act between two things thus kinda "something in progress". This is the exact same reason I am bad at real analysis
Because most things in analysis don't "sit there" Take limits of a sequence for example
 
Meanwhile I am reading this
Harmonic analysis is a branch of mathematics concerned with the representation of functions or signals as the superposition of basic waves, and the study of and generalization of the notions of Fourier series and Fourier transforms (i.e. an extended form of Fourier analysis). In the past two centuries, it has become a vast subject with applications in areas as diverse as signal processing, quantum mechanics, tidal analysis and neuroscience. The term "harmonics" originated as the ancient Greek word, "harmonikos," meaning "skilled in music." In physical eigenvalue problems it began to mean waves...
which is a nice folow up after potrygian duality
 
2:07 PM
I am trying to explain something to someone in the comments of a question, and it is getting a little long, so I want to use the "move this discussion to chat" option
But it just gives me an error message, "Moving discussion to chat failed".
 
2:26 PM
@MeesdeVries link?
 
The space of sequence is extremely elusive a concept to me. The sequence ($x_{n}$) are elements in a field of scalar. If, say, $x_{1}$=1. What exactly is $x_{n=1}^{k}$ for all natural number k? How does one even have a sequence for a point? — Mathematicing 11 mins ago
Oh, huh. It changes it to a quote automatically. That's new to me.
 
@Semiclassical New QM problem set ;_;
First problem is linear algebra because everyone got the linear algebra question wrong on the midterm. Ah! The midterm
@Semiclassical I won't scan it because he's collecting it again.
But I can tell you what was on it
@Semiclassical We were given an operator on a 2D Hilbert space. We had to show that a certain construction with it is a projection operator. We had to write down the matrix rep for the operator and its adjoint. We have to compute the eigenvalues and eigenvectors of a Hamiltonian constructed with it
We had to compute a probability at time $t$ using this Hamiltonian, and had to explain why some other construction with the operator is an observable
That was problem 1
Problem 2 was an SHO problem, construct a maximum $\langle x\rangle$ state using only $|0\rangle$ and $|1\rangle$
Compute the time evolution of this state, then compute $\langle x\rangle_t$ in the S and H pictures
Now compute $\Delta x^2(t)$ using both pictures
Problem 3: box potential, what is the condition for bound states
Problem 4: solve the double delta potential S eq for a bound state
 
2:45 PM
at what speed would you have to listen to a audiobook i.e. 1x is normal 2x is twice as fast, to remove all the redundancy from English so its as if your listening to an efficient book at 1x speed?
 
2:56 PM
100000000x
 
3:13 PM
@0celo7 Sounds tedious but straightforward
in fact, that pretty well describes all of those problems
 
I think everyone got it wrong. Too much algebra
 
perhaps, yeah
i imagine it has something to do with the fact that any diagnolizable operator can be written as a sum of projectors
 
@Semiclassical Have you ever seen the matrix $U=(a_0+i\vec\sigma\cdot\vec a)(a_0-i\vec\sigma\cdot\vec a)^{-1}$?
 
I feel like I ought to have
 
I recall it from QFT, perhaps. Maybe I should check Weinberg
But it's on my QM homework. I'm thinking one needs $a_0^2+\vec a^2=1$ for it to be unitary
but that restriction is not stated
 
3:16 PM
The stuff in brackets reminds of quternions
 
It should. That's basically just a quaternion written in terms of pauli matrices.
 
is there any connection between polynomial convolution and convolution?
 
I expect that you can reduce that down to the case of $(a_0+i \sigma_3 |a|)(a_0-i \sigma_3 |a|)^{-1}$ by an appropriate rotation
 
polynomial convolution is basically a discrete version of convolution. In fact multiplying two polynomials is a discrete convolution between the two
 
@Secret thanks
 
3:18 PM
Expanding terms is also a thing I don't like as I always make mistakes and miss terms
writing the multiplication as a cayley table format does help somewhat in keeping track of the terms
 
apparently one doesn't need that condition
back to the drawing board
 
Meanwhile: PHYSICS!
In mathematics, the special unitary group of degree n, denoted SU(n), is the Lie group of n×n unitary matrices with determinant 1. The group operation is that of matrix multiplication. The special unitary group is a subgroup of the unitary group U(n), consisting of all n×n unitary matrices. As a compact classical group, U(n) is the group that preserves the standard inner product on Cn. It is itself a subgroup of the general linear group, SU(n) ⊂ U(n) ⊂ GL(n, C). The SU(n) groups find wide application in the Standard Model of particle physics, especially SU(2) in the electroweak interaction and...
this is where I am now in this more than 2 weeks of group theory self study
 
3:33 PM
Good god. @Semiclassical was your grad QM class this computation intensive?
 
eh, is that really so bad? You've just got $R=e^{i \vec{\sigma}\cdot \frac{\vec{\phi}}{2}}\oplus 1$ or something like that
 
No it's not so bad if you write out the exponential using the usual identity
 
Plus, the left-hand side is pretty much begging to have the BCH identity used
 
Does somebody know of an example of a function space where $\mathcal F(A)\otimes\mathcal F(B)$ has a canonical inclusion into $\mathcal F(A\times B)$ that is not also an isomorphism?
 
$\exp(-i\sigma\cdot n\phi/2)=\cos(\phi/2)-i\sigma\cdot n\sin(\phi/2)$
@Semiclassical No, that's overkill
You can write down the exponentials in one shot
 
3:39 PM
true enough
 
Then just matrix multiply
 
Seems pretty straightforward.
 
Straightforward but tedious
I want more conceptual homework
 
I find the font in that image to be ugly
really ugly
but its probably just computer modern at 11pt blown up to 30pt or something
 
I am guessing for the 2nd question, rewrite it in index and use $[\sigma_i,\sigma_j]=i\epsilon_{ijk}\sigma_k$
 
3:47 PM
Hello
.
Hey @Semiclassical :D
 
@DHMO What you suggested is also a good gateway to understand cohomology too. Fix a subspace $U$ of $\Bbb R^2$; Let $C_0$ be the vector space of smooth functions on $U$, $C_1$ vector space of "1-dimensional integrands", $f dx + g dy$ (think of it as a vector field $X = (f, g)$), $C_2$ be the vector space of "2-dimensional integrands", $f dx dy$. Then define $d : C_0 \to C_1$ as $df = f_x dx + f_y dy$, and $d : C_1 \to C_2$ as $d(f dx + g dy) = df dx + dg dy = (g_x - f_y) dx dy$.
Using the identification with vector fields earlier, the former is gradient, the latter is curl. Check that $d^2 = 0$ (curl of grad is 0!). Green's theorem becomes $\int_D d\omega = \int_{\partial D} \omega$, where $\omega = f dx + g dy$ is in $C_1$. If $\omega \in C_1$, $\ker \omega = 0$ means the corresponding vector field is irrotational. $\omega \in \text{im} d$ means it's conservative.
A natural question to ask is, "which irrotational fields are conservative", which is precisely what $\ker d/\text{im} d$ (two different d's) measure. That is the 1st cohomology group $H^1(U)$ of $U$.
 
hi @mahmoud
 
Hey everyone, it's been a while...
 
@BalarkaSen sorry i know you used a lot of effort to type that but i must say that i do not understand...
 
speaking of cohomology, here's something neat I've been playing with (though not very elegant)
 
3:49 PM
Sure, I just wrote it down, didn't expect you'd understand.
 
good
 
suppose I've got a Riemann surface $y^2=x(x-1)(x-\lambda)$. That's an elliptic curve, and since it's got genus 1 the first homology group is 2D. hence, so is the first cohomology group.
as i understand it, a basis for that is $dx/y$ and $x dx/y$
What I've been grappling with is how one practically uses that fact, e.g. how to express $x^2 dx/y$ in that basis (up to an exact form)
 
shrug
 
currently the only way I know how to do that is to observe that $dx/y=d(x/y)-x d(1/y)=d(x/y)-x dy/y^2$
 
pick a diffeomorphism with R^2/Z^2, and then integrate it along the two obvious loops. if the result is (a,b), it's equivalent to adx + bdy
 
3:53 PM
he has weird basis though
 
better yet, just pick any basis for homology, and integrate those two forms on it, dx/y and xdx/y
then integrate x^2dx/y along them, and figure out what linear combo you have to be
 
Easier said than done, I think. If I do those integrals, I get elliptic integrals and it's not obvious how to break them apart
Hence why I wanted a way purely at the level of algebra
but, I wasn't quite done
 
i see no particular reason that there's an algebraic way of finding a decomposition of a form given by rational polynomials
just have matlab do them? :)
 
in what I wrote above, i've got $dx/y=x dy/y^2$ up to an exact form (minus sign error earlier)
but I know that $2ydy=d[x(x-1)(x-\lambda)]=p(x)\,dx$ for some quadatic polynomial $p(x)$
hence $\frac{dx}{y}=x\frac{dy}{y^2}=\frac{x p(x)}{2y^3}dx$
 
you've convinced me mainly that i don't wanna do this
:)
 
3:59 PM
since $xp(x)$ is cubic, I can write $xp(x)=Q(x)y^2+R(x)$ where $Q(x)$ is linear and $R(x)$ is quadratic
 
Does anyone remember me? I gave up on mathematics for around a year, but now I'm in between jobs with nothing else to do
 
so therefore $\frac{dx}{y}=Q(x)\frac{dx}{2y}+R(x)\frac{dx}{2y^3}$
 
@teadawg1337 I don't, but welcome back to the Mathematics Community. :)
 
I can do that similarly for any $x^k (dx/y)$ and so obtain linear relations between forms $x^k dx/y$ and forms $x^k dx/y^3$
and if I get enough of those, I can express everything in terms of just $dx/y$ and $x(dx/y)$ purely from algebra
 
I haven't been on here in over a year, so I wouldn't expect many people to remember me :P
 
4:02 PM
name sounds vaguely familiar but I don't really remember :/
for instance, I get $$x^2 \frac{dx}{y}=\frac{2}{3}(1+\lambda)x\frac{dx}{y}-\frac{\lambda}{3} \frac{dx}{y}$$
Which is simpler than one might've expected
 
Is my virtual existence on this server annoying to anyone ? I mean all what I do is ask questions and post paradoxical math subjects.
 
@Mahmoud "virtual existence" is an oxymoron
 
sorry, @Semiclassical, it seems like you just answered your own question?
 
Exactly ! Is this annoying ?
 
@Mahmoud not at all
 
4:07 PM
I did. I was more wondering if there was an obvious way to make it simpler
 
So it's annoying ...
 
i'm guessing the answer there is "i dunno"
 
@Mahmoud it means it is not annoying at all
english
 
No it means it's not at all annoying, but a little.
 
@Semiclassical yup
 
4:08 PM
@Mahmoud don't twist my words
 
fiine
 
You should have written No, at all. :P
Anyway, it's just chat.
 
@Mahmoud what he said was perfectly good english to mean that you're not annoying
 
@Mahmoud it's just a translation of "pas du tout"
@MikeMiller thanks
 
O.O
French ?
 
4:09 PM
@Semiclassical this does give you some nice solutions to elliptic integrals
 
Français ?
 
it does
 
@DHMO
 
that's the motivation, in fact
though I'm trying to move towards a case that'd be periods of a non-hyperelliptic curve rather than an elliptic one
whiiiich is pretty terrifying
 
@Mahmoud I know some French
 
4:11 PM
C'est une surprise pour moi !
 
i realized a problem in a proof i was explaining to my advisor yesterday, and was terrified for a bit
 
@Mahmoud pour
 
and this morning i realized there's a more subtle and harder problem
(but the previous problem probably doesn't matter)
 
@DHMO :D
 
@Mahmoud alors tu parles trois langues?
 
4:18 PM
Français, Anglais et Arabe, oui mais je n'aime pas parler en français beaucoup.
 
alright then
 
English is much more elegant and it is a whole lot easier.
Even french people have to learn English :P
 
elegance and easiness are subjective
 
Well at least in my point of view, I meant
I don't have to include that in my speech, it is automatically determined once you realize that it is ME who wrote that down.
 
@Mahmoud alright
 
4:22 PM
@DHMO Any ideas about INVENTING usernames ?
For YouTube channels ?
 
@Mahmoud no idea
 
I driving myself crazy about finding the perfect unique username.
 
perfectness is subjective
 
Well almost everything is subjective,
Science is not.
 
precisely
 
4:25 PM
You'll never come up with a single username if you're searching for "the perfect one"
 
@teadawg1337 I just want it to be unique and has a ambiguity in it.
But that requires days and days of thinking and searching for inspiration.
 
Everyone has a unique personality, so try to find something that expresses yours
 
They get bulky.
Because I don't know many English words
 
Who says it needs to be written in English?
 
@Mahmoud then produce them in Arabic (and translate to English)
 
4:29 PM
You could produce a random string of characters and call it a username
 
@DHMO Genius ! I can even write it down without translating !
 
@s.harp it's not compute modern
@Semiclassical If I write down an $\mathrm{SU}(2)$ matrix and try to identify it with a rotation $(\hat n,\phi)$, I get a sign ambiguity from some square roots. That's just because it double covers $\mathrm{SO}(3)$, right?
 
probably? i haven't done the stuff lately
but overall signs don't matter when it comes to wavefunctions anyways
 
that's correct
 
hi
 
4:45 PM
hi
 
hi
 
@Semiclassical I should pin a table of trig identities to my desk
 
not a bad thought
 
4:56 PM
Hi.
 
If $f:X\to\mathbb C$ is holomorphic, is it always the case that $f|_Y$ is holomorphic for every $Y\subseteq X$?
I think yes since $f$ being holomorphic implies that for every $z\in X$, the Cauchy-Riemann equations $u_x=v_y$ and $u_y=-v_x$ are satisfied, where $f(z)=f(x,y)=u(x,y)+iv(x,y)$, which also holds for every $z\in Y$.
 
@Josué If $Y$ is open, I would expect so. Complex differentiability is a local condition.
If $Y$ is not open you'll have problems defining derivatives on it.
 
5:11 PM
You can define complex differentiability on any subset of $\mathbb C$, namely $f$ is complex differentiable at $z$ if $\lim_{z'\to z} \frac{f(z')-f(z)}{z'-z}$ and the limit is taken so that only points the set you are working with are considered
and in this case it is obvious that $Y\subset X$ implies $f\lvert_Y$ is holomoprhic
but you now also have a little pathology: if $\bigcup_i A_i = X$ and $f$ is holomorphic on all of the $A_i$, then $f$ is not necessarily holomorphic on $X$
if the $A_i$ are open, then this pathology goes away
 
So it's like a necessary but not sufficient condition.
 
You should be aware that one almost never calls functions defined on a non-open set holomorphic, regardless of whether or not they are complex differentiable in the above sense.
But yeah, in the above sense knowing that $f$ is complex differentiable on subsets that cover the space is not enough to know that $f$ is complex differentiable on the space. But $f$ cannot be complex differentiable if it is not so on all subsets.
 
I see. Thank you.
 
@AlexClark Neat. Do you still have access to some computers that can run GAP? I have some code I would like to run for a while, and I will soon lose access to my office computer as my employment ends (and I only now finally got around to setting it up on that). This will require an old version of GAP though (however, I think Peter McNamara could be interested in the results of these).
 
5:46 PM
I don't visit here often, but thought that some of you might be interested that one of the most popular recent questions on CodeReview is arguably more about number theory than programming.
55
Q: Disproving Euler proposition by brute force in C

AidenhjjI wrote a little bit of code to brute force disprove the Euler proposition that states: $$a^4 + b^4 + c^4 = d^4$$ has no solution when \$a\$, \$b\$, \$c\$, \$d\$ are positive integers. I'm no mathematician, but reading around this, at least one solution was found by Noam Elkies in 1987...

@NoamD.Elkies: You might be interested in reading through some of the answers and comments to that question since it addresses your 1988 paper.
 
@Edward That won't ping him.
 
I didn't know that. Anyway, it's more for his amusement than anything else. Not critical.
I read the associated paper (or attempted to!) and learned a couple of new terms, but haven't yet fully understood them.
A "pencil of conics" was new to me.
 
There's quite a lot of number theory that effectively proceeds by starting by working in algebraic geometry and reducing to a computationally simpler problem. See also "Twists of X(7)" by Poonen-Schaefer-Stoll for a variation on a theme: there they calculate all the integer solutions to $x^2+y^3=z^7$.
 
6:03 PM
Can anyone please tell me how to use programs on GitHub, sorry it's out of the subject.
 
It's usually not straightforward. Most of what you'll find at GitHub is source code, which means that you'll have to download and compile it yourself before you can run it.
 
@Mahmoud depends on what has been uploaded. Mostly you would need to compile and run them yourself
 
@TobiasKildetoft It's written in python.
 
I don't have much of a clue on what kind of tools in algebraic geometry helps figuring out rational solutions. At a glance and without reading anything, Elkies 1988 seems to be setting a birational equivalence between $X^4 + Y^4 + Z^2 = 1$ and some elliptic curve, where the story is known, I guess.
 
I don't even know where to start. :(
 
6:06 PM
@Mahmoud Generally git clone xxx where xxx is the URL for the project. Then navigate into the project. There is often a README file.
 
@Mahmoud well, then you need to figure out how to run python code
 
Python is interpreted. In the best case scenario, you can copy the code and paste it into an interpreter.
 
I'm so not familiar with this.
I think there is a way to run it into GitHub's desktop program.
 
@Edward that seems to be precisely what he is not looking for :)
 
6:11 PM
:)
 
@Edward :) I want to use an existing program :)
 
@Mahmoud If you are not familiar with how to run source code then for the most part, GitHub will be the wrong place to find stuff
 
@Mahmoud Everything I know about git, I learned from this book: git-scm.com/book/en/v2
Read chapters 1 and 2 and you'll probably know everything you need to know to fetch the program you want.
 
Thank you guys that was helpful, just replying to my stupid question was already amazing :D
 
@Edward These are not really Git questions at all. They are essentially unrelated to Git
 
6:15 PM
@TobiasKildetoft You may be right.
 
@Balarka There is a complicated general story that I would know if I was a number theorist.
 
At least how to use this one github.com/3b1b/manim
 
@Mahmoud If you've already read and tried the instructions there, asking more specific questions in a more suitable venue about whatever particular problems you've encountered is likely to be more fruitful.
 
@Edward How do I run the commands ?
 
yo
Can somebody give me a hint on how to find a inverse function if the original function $f$ maps from $A\times A\to A$? (It's assumable that $f$ is inversible)
It's pretty easy for functions where the "from-dimension" and "to-dimension" is equal, however, how to proceed here?
 
6:39 PM
Do you have a specific function in mind?
@NaCl [citation needed]
 
Take a look at this: szudzik.com/ElegantPairing.pdf (page 8)
 
@NaCl That last is not true unless the functions are of some "nice" form
 
How did Szudzik find the inverse here?
 
try to invert something horrible like $\Gamma(x)+x^2$
 
@NaCl I might have been interested in reading more than a few lines of that, except he very quickly refers to that stupid book by Wolfram
 
6:42 PM
Stupid book?
 
@0celo7 A new kind of science
 
Yeah I figured out what book, but what's wrong with it?
 
@0celo7 More or less everything from the point of view of mathematics. There are some rather scathing reviews of it by mathematicians
 
Ouch
uh
Those links are all broken
> In this note, we disprove 44 claims in [4] on minimal Boolean
formula size of one-dimensional two-state nearest neighbor cellular
automata as well as set a new upper bound.
lol
 
6:46 PM
I am only now realizing that his manner of writing is very similar to the way in which Trump speaks.
 
What's wrong with having the best words?
 
Having the best words is obviously the best thing.
 
Maybe we should build a wall around your country
 
we should build a wall around trump
Anyways, as I just need a way on how to start this, how'd you, for example, find the inverse of Cantor's pairing function?
 
@0celo7 oops
 

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