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2:01 PM
well technically laws can be derived. But in doing so you are basically revisiting the whole cultural history that lead to the law (and why it is in that form), which I believe is a book longer than any existing proofs in mathematics
This is a list of unusually long mathematical proofs. As of 2011, the longest mathematical proof, measured by number of published journal pages, is the classification of finite simple groups with well over 10000 pages. There are several proofs that would be far longer than this if the details of the computer calculations they depend on were published in full. == Long proofs == The length of unusually long proofs has increased with time. As a rough rule of thumb, 100 pages in 1900, or 200 pages in 1950, or 500 pages in 2000 is unusually long for a proof. 1799 The Abel–Ruffini theorem was nearly...
A typical history of an average nation goes over 10000 pages, right...?
 
> 1799 The Abel–Ruffini theorem was nearly proved by Paolo Ruffini, but his proof, spanning 500 pages, was mostly ignored and later, in 1824, Niels Henrik Abel published a proof that required just six pages
Um.
So what they're saying is that there's still hope for the FLT
 
@AkivaWeinberger Depends on which part one considers "the proof"
 
@BalarkaSen applied topology?
 
heh
so how's your numerical analysis going
 
My exam was moved to Tuesday because there are too many people taking it
But I'm quite ready
 
2:22 PM
neat
 
@Secret depends on how long that nation has been around
@Secret speaking of which, can you prove that exp(r ln x) is the extension of x^q?
 
I would have preferred doing it tomorrow actually since I'm ready but a few more days won't hurt. I also aced the topology exam from Monday
 
Cool
 
How can we show that one vector space is the complement of an other vector space?
 
@DHMO I think I need hints for this one, as I felt like my current thoguth process is massively overthinking on the level of domains and codomains
 
2:34 PM
Are you talking about 2 subspaces of a bigger space?@MaryStar
 
Let $V$ be the real vector space $\mathbb{R}[X]$ and $M \subset \mathbb{R}$ a set with $d$ elements. Let $$U_1 := \{ f \in \mathbb{R}[X] | \forall m \in M : f(m) = 0\}, \ \ U_2 := \{ f \in \mathbb{R}[X] \mid \deg(f) \leq d − 1\}$$ be two vector spaces of $V$. I want to show that $U_2$ is a complement of $U_1$. @AlessandroCodenotti
 
@Secret well what are we trying to prove?
 
Do we have to show that the intersection is zero? @AlessandroCodenotti
 
@Alessandro Do you want to talk about differential forms now then?
I am more or less free for the next hour
 
I don't know anything about infinite dimensional vector spaces @Marystar but I'd guess you also need their direct sum to be the whole of $\Bbb R[x]$
Sure @Balarka, thanks! So we defined what an alternating multilinear function is last time
 
2:41 PM
@DHMO that $x^q$ is the restriction of $exp(r \ln x)$?
 
@Secret well... do we need to prove continuity as well?
 
@Alessandro Yeah, so it's just a multilinear map $T : V \times V \times \cdots \times V \to \Bbb R$ such that $T(\cdots, a_i, \cdots, a_j, \cdots) = -T(\cdots, a_j, \cdots, a_i, \cdots)$.
Examples include the determinant, as we mentioned - eating column vectors and spitting the det of the matrix.
 
Every alternating multilinear function is $0$ if supplied the same argument twice, just like the determinant
 
Yeah.
 
@DHMO we do need to if $q$ is rational, and I am not good at continuity stuffs
 
2:45 PM
alright, let's prove the weaker statement then
 
Does anyone know if this method for integrating has a name?
 
@AlessandroCodenotti So do we have to find a basis for each for them?
 
@Secret Shall we start with the naturals?
 
$$\int te^t\ dt=f'(1),\quad f(x)=\int e^{tx}dt$$
 
Hmm...
 
2:48 PM
@Alessandro So now I want to construct a vector space $\Lambda^k(V)^*$ of alternating multilinear maps $V^k \to \Bbb R$ (here $V$ is a vector space of dimension $n > k$); that it's a vector space is easy to check.
Because adding two alternating multilinear maps is alternating multilinear, multiplying by a scalar is obviously so.
 
@MaryStar You just need to show that the spaces intersect trivially and that any polynomial can be written as a sum of an element from each
 
*$n \geq k$. Do you see why it's not interesting if $n < k$?
 
When $f\in U_2$ it holds that $\deg (f)\leq d-1$. Since $M$ is a set of $d$ elements, it can be that $f\in U_1$ only if $f=0$, since it must have $m$ roots. From that we get that the intersection is trivial, right?
@TobiasKildetoft
 
@MaryStar right
 
But how can we show that any polynomial can be written as a sum of an element from each?
Suppose that $f\in U_1$ and $g\in U_2$.
If $\deg h\leq d-1$ then $h=0+g$, or not? @TobiasKildetoft
 
2:54 PM
sure
 
@BalarkaSen in that case the only multilinear map is the 0 one I think?
Because I can write one of its arguments as a linear combination of the others
 
@TobiasKildetoft And if $\deg h>d-1$, what happens then?
 
@Alessandro Bingo. Right.
 
@MaryStar You want to subtract something of degree at most $d-1$ such that you end up with something that vanishes on all the given elements
 
So, ok, suppose $v_1, \cdots, v_n$ is a basis of $V$. Let's try to write down a basis for $\Lambda^k(V)^*$ too.
Later we'll do the wedge product construction, which is possible to do without fiddling with basis, but I find the basis-wise construction cleaner.
 
3:00 PM
Ok, let me think about it
 
Try for $k = n$ first.
 
So, if we have a polynomial of degree >d-1 then we write as f-g, so that the terms that don't exist vanished? @TobiasKildetoft
Or did I misunderstand it? @TobiasKildetoft
 
@DHMO Ok I am somewhat stuck. If both $x \in \mathbb{N}$ then there is no difference between the two functions as both their domain and images have the same set of points
 
@Secret both?
 
@MaryStar I am not sure what you mean
 
3:12 PM
@Secret I don't understand. Domain and image having the same set of points doesn't prove anything...
 
No I mean the images of exp(r ln x) and x^q will be the same if $x \in \mathbb{N}$
 
@Alessandro Here's the thing. If $T : V^n \to \Bbb R$ is an alternating $n$-multilinear form then for random vectors $w_1, \cdots, w_n$, $T(w_1, \cdots, w_n)$ is stuff times $T(v_1, \cdots, v_n)$, by expressing $w_i$'s in terms of the basis $\{v_1, \cdots, v_n\}$. What's that stuff?
 
@Secret ah, I meant when r in N.
I'm not sure how you'd prove it if x in N instead.
 
@TobiasKildetoft I haven't understood why a polynomial of degree >d-1 can be written as a sum of an element of $U_1$ und one of $U_2$. Could you explain it to me?
 
@MaryStar Try to do the case where $d=1$ first
 
3:20 PM
Also you should just set $V = \Bbb R^n$ and the basis to be the standard basis $\{e_1, \cdots, e_n\}$ (ie $e_i$ = vector with 1 at $i$-th slot and zero everywhere else)
 
So, we have a set of constant polynomials and a set of polynomials that have one root, right? Suppose we have a polynomial of degree n. Then we have to write it as an polynomial of the set $U_1$, since the other one are constants, or not? @TobiasKildetoft
 
@MaryStar no
 
But how can we write it as a sum? I haven't understood it yet. @TobiasKildetoft
 
So I have $T(w_1,\cdots,w_n)=T(\sum\alpha_iv_i,\cdots,\sum\gamma_iv_i)=\sum...\sum\alpha_i‌​...\gamma_jT(v_i,...,v_j)$ if I opened it correctly (that sure is uncomfortable to type on mobile)
 
@Alessandro There are a bunch of signs involved though. What's $T(a_1 e_1 + a_2 e_2, b_1 e_1 + b_2 e_2)$?
Note that $T(e_1, e_2) = -T(e_2, e_1)$, not $T(e_2, e_1)$.
 
3:31 PM
Ah, right, what I wrotr above was for a multilinear map
@BalarkaSen $(a_1b_2-a_2b_1)T(e_1,e_2)$
 
yay determinant.
also, hi chat
 
@MaryStar so you have a polynomial $f$ and you want to write it as $h + g$ where $g(a) = 0$ and $h$ is constant.
 
That's right. So T(v_1, ..., v_n) = ??? T(e_1, ..., e_n)?
@Semiclassical yo
 
@Secret Yes, it is quantum computing related. This specific data (calculated from a model, so not measured, although I am an experimentalist) is about what the effect of a specific noisy environment is on the decay of phase information of a two level system
 
Numerical data is the closest I come to being an experimentalist :)
 
3:36 PM
Well I'm going to guess that's the determinant of a matrix with the coordinates of the $v_i$ in the basis $e_j$ on the rows (or columns)
 
and you'd be quite right to guess so!
So $\Lambda^n(V)^*$ is a one dimensional space, with basis the determinant.
 
@TobiasKildetoft But why can every polynomial be written in that form?
 
In general $\Lambda^k(V)^*$ is generated by multilinear $k$-forms I'd denote as "$dx_I$", defined by setting $dx_I(v_1, \cdots, v_k)$ = determinant of the $i$-th rows of $v_1, \cdots, v_k$ where $i \in I$. Here $I$ is an ordered $k$-subtuple of $\{1, 2, \cdots, n\}$
 
@MaryStar Think some more about how you would find those
 
@user129412 What kind of two-level system? I've been doing research in the realm of certain multi-level quantum systems lately, the simplest version of which is the Landau-Zener problem (i.e. two coupled levels whose energy separation varies linearly with time).
 
3:41 PM
If $I = \{1, 2, \cdots, n\}$ is the full tuple, then $dx_I$ is precisely the same as the determinant operator.
The generator of $\Lambda^n(V)^*$ that is.
 
That makes intuitively sense but I'll need a moment to convince myself
 
@Semiclassical Interesting! I'm doing research in superconducting circuits, so we basically cooper pair box type of systems as our qubits. I'm familiar with the Landau-Zener problem, which is actually interesting because the thing I am working on right now is intimately related to Landau-Zener-Stuckelberg interference. Its not the same thing, but a nice coincidence
 
Neat.
 
When we subtract from f the constant term, so h, we get a polyonmial that has the root $x=0$, since every term is $x^i, i\geq 1$. The rest from the subtraction would be g? But how do we know that 0 is the only root? @TobiasKildetoft
 
@Alessandro You can try to write down a proof. Given a multilinear $k$-form $T$, set $a_I = T(e_{i_1}, \cdots, e_{i_k})$ where $I = \{i_1, \cdots, i_k\}$ is an increasing $K$-tuple. Then check that $T = \sum_I a_I dx_I$ where $I$ runs through increasing $k$-tuples. Hint: Check basis-wise.
 
3:43 PM
I have to catch a bus to return home, I'll be back soon
 
See ya on the bus.
 
hi, i need to show somehow that $ a \ ^ 2 + b \ ^ 2 $ is not $3$ $ mod 4$ when $ a,b \in Z$ someone see a way to do it?
 
What is an endomorphism ring? I know what an endomorphism is, and what a ring is, but what are the two operators for an endomorphism ring (specifically of an elliptic curve)?
 
Specifically I'm interested in recent work on $n$-level Landau-Zener problems, i.e. $i\frac{d}{dt}\Psi=(A+B t)\Psi$ with $B$ diagonal and $A$ off-diagonal.
 
Hm. That sounds computationally challenging.. Many experimental efforts in that direction?
 
3:46 PM
Yeah. I haven't done a lot with the computational side yet because of that.
I think so? It's almost inevitable that you run into such things in practice, because you want to apply time-dependent fields to quantum systems in order to control them.
 
@MaryStar Obviously you need to subtract something that depends on which root it is you reqire
 
True. Bose einstein condensates come to mind
Ah, but many particle is of course not the same as n-level.
 
If you do it infinitely slowly, then the adiabatic theorem guarantees that you'll just stay in the same adiabatic state. But of course nothing is infinitely slow, so you have to worry about tunneling between those states. Hence why one cares about the scattering amplitudes in particular.
 
Right. I have to admit that I can't think of all that many applications that use n-level systems though; most of the stuff is geared towards quantum computing nowadays with their fancy qubits. But then again, in practice many of those are actually anharmonic n-level systems to begin with.
 
Right.
Anyways, in the usual Landau-Zener problem, one finds that the amplitude for scattering from one adiabatic level to the other is exponentially small. This can be shown exactly, but also can be found by semiclassical/adiabatic methods.
 
3:51 PM
Ok, I convinced myself of the determinant thing for $\Lambda_n(V)*$, now let's see for the general case
 
What's interesting is that there are cases of multi-state Landau-Zener where that's also true: The semiclassical computation of the scattering amplitudes appears to be exact.
So you end up with scenarios where the scattering matrix is a lot simpler than you'd expect.
That's what I"m trying to understand, more or less.
 
But isn't Landau Zener semiclassical itself?
The perturbation parameter in the Hamiltonian is a linear function of time, right
 
Right. In the two-level system, it's exact in that the boundary conditions are at +/- infinity.
 
Okay, yes
 
3:56 PM
In the multi-state case, though, there will be multiple level crossings and a finite time between them.
 
So you're investigating how (at first sight) approximate, semiclassical theories turn out to provide exact results for truly quantum systems
 
Exactly so.
 
Very interesting
 
For an instance of this for a model you might appreciate, check out this preprint: arxiv.org/abs/1602.03136
My adviser knows one of the authors; that's how I learned about it.
 
I'm quite convinced about the basis of $\Lambda_k(V)*$ @Balarka, I'll try to write it down properly on a piece of paper when I get home and see if it still makes sense :P
 
3:59 PM
Excellent.
 
I'll have a look at that, the abstract sounds promising. It is actually strangely close to what I am working on, which is how phononic modes could enhance excitation transport in disordered coupled two level systems (read, they have energy level splittings comparable to the phononic frequencies and the phonons help them cross the gap)
 
Ah, nice.
What's your Hamiltonian?
 
@Alessandro So the intuition you should have about all of this is that an alternating multilinear $k$-form on $V$ is something which eats a $k$-dimensional parallelpiped spanned by $k$ vectors in $V$, and spits out linear combination of (signed) area of it's projection to various coordinate planes.
 
And those phononic modes can essentially be seen as a structured bath. But the hamiltonian is just a tight binding hamiltonian of two level systems along with longitudonal coupling to harmonic oscillators
 
@TobiasKildetoft You mean the roots of the polynomial f?
 
4:02 PM
Because note that $dx_I(v_1, \cdots, v_k)$ is precisely area of the projection of the parallelpiped spanned by some random vectors $v_1, \cdots, v_k$, projected to the $i_1, i_2 \cdots i_k$-th coordinate plane.
 
A sort of longitudonal tavis cummings model with coupling between the spins
 
Heh, which is exactly what this is about. Nice.
In the case they discuss, there's only one optical mode.
But the two-level systems are otherwise unconstrained.
 
It's close, but that cavity has sigma_x coupling, which is a bit more invasive than sigma_z
 
For a top dimensional form, i.e., an alternating multilinear $n$-form on $V$ you don't have to worry about projecting - it's literally, upto scalar multiplication, volume of the parallelpiped spanned by the vectors.
 
4:04 PM
Still, many similar ingredients.
 
Right, that makes a lot of sense
 
The model here also assumes that the coupling to the optical mode is the same for all spins (though it doesn't assume anything about the local splitting of the two-level systems.)
 
Yes, so it is a strongly correlated system in the end
 
Yeah.
 
@Alessandro I can say more if you want to hear more. There's still the wedge product construction before we go to the manifold-level.
 
4:07 PM
My adviser does a lot of disorder stuff, though I don't.
 
(Essentially a differential form is a smoothly varying alternating multilinear form on the tangent spaces of the manifold)
 
@MaryStar If $f(a)$ is not $0$, what do you need to subtract from it to get $0$?
 
Hm, wait, I need some time to digest the construction so far and a moving bus is not the best place to do so
 
I mostly work on analog quantum simulation these days, so it varies quite a bit depending on which field the system we want to simulate originates from. Currently working on photosynthesis, of all things
 
Heh, nice.
I can well believe that anything organic would have a lot of disorder to deal with.
 
4:10 PM
Oh, for sure. But we're actually looking in the opposite direction. At which quantum features can still survive even in the presence of large disorder
 
Sure, there's no hurry about it.
 
Ahh.
Where are you working?
I'm at the University of Minnesota. (physics grad student)
 
So basically this paper nature.com/nature/journal/v446/n7137/abs/nature05678.html launched an entire field of people looking at possible quantum effects in biological systems, which is also the direction we are working in
I'm at ETH Zurich, Switzerland. Also a physics grad
 
When we compute the function at $x=a$, we get a constant, so we have to substract it by the constant f(a), right? @TobiasKildetoft
 
4:12 PM
Neat.
 
The question is how those messy biological systems can still show coherent features, and right now the (theoretical) consensus is that it is due to their structured environment. We're working on experiments testing this.
 
Hmm, interesting.
 
This is when h is constant. What happends when deg(h)<=d-1? @TobiasKildetoft
 
@MaryStar try $d=2$ to see the pattern
 
Did someone have a question about quantum noise?
 
4:16 PM
nah
 
Then they're spinning lies over in the physics room.
 
that's what physics is so...
 
@DanielSank Aren't they always :)
 
@TobiasKildetoft :-/
 
@DanielSank I was, but not on an interesting level. Trying to guess a functional dependence of some curve, like a proper scientist.
 
4:20 PM
Heh.
Exactly the kind of thing I hate when my students do it in intro physics lab reports :)
(Though I hate it mostly because they don't have the experience to actually guess well.)
(They've got enough physics to derive equations for the simple experiments they're doing. Do that instead.)
 
Oh for sure. I was just looking for something it interpolate some data with as actual interpolations were misbehaving, wouldn't be a proper model. I have a proper model but its terrible to fit with.
 
Heh, I understand.
I wouldn't be surprised if our advisers know of each other somehow.
So this is indeed rather serendipitous.
 
It's very possible, as big as the field of physics is. The topics are close enough to have some overlap
 
Yeah.
 
Well, i'm gonna try again :)
I want to prove that for all $a,b \in Z $ $a \ ^ 2 + b \ ^ 2 \ne 3mod 4$ . someone see a way to prove it?
 
4:32 PM
@Liad what are the possible remainders mod $4$ of a square?
 
@TobiasKildetoft hmm, 0,1 ?
 
@Liad Right
 
@TobiasKildetoft but why?
 
well, how did you find them?
 
well if something happens for every number you are trying, then it is a good guess to think it happens for all of the numbers :)
 
4:36 PM
Maybe focus on which integers square to zero mod 4.
 
2^k
 
all even numbers
 
@KasmirKhaan's got it.
It's not just 2^k. 6 is the easy counterexample.
 
right.
 
The simple proof is that an even integer 2n squares to 4n^2=0 mod 4.
On the other hand, if you want to get m^2=1 mod 4, you need m^2-1=(m-1)(m+1)=0 mod 4.
So what does m need to be?
 
4:40 PM
dont you need the "-1" before the square?
 
if m^2 =1 mod 4 doesnt it means that (m-1) ^ 2 = 0 mod 4
 
Um, why?
I'm just subtracting over the 1 and using a^2-b^2=(a-b)(a+b).
 
but you claim now it is equals 0 mod 4
huh
i thought it is m^(2-1)
sorry, yes im with you
 
Oh, no.
(m^2)-1.
 
4:43 PM
yea
it means that m must be odd.
 
Right.
So m odd -> m^2 = 1 mod 4, m even -> m^2=0 mod 4.
And since m is either even or odd, those are the only possibilities.
 
wait, you showed that if m^2 =1 mod 4 , then m is odd
 
So you know that, regardless of what a,b actually are, that they each square to 0 or 1 mod 4.
 
alright
 
4:45 PM
since if it is even it equals 0 mod 4 then if it is odd it must be 1 mod 4
 
Right.
 
ok , so a ^ 2 = 0 or 1 mod 4
 
Right. Same for b^2.
So what can a^2+b^2 be mod 4?
 
is it correct that a^2 + b^2 mod 4 = a^2 mod 4 +b^2mod 4?
yea i think it is
 
Yeah.
 
4:46 PM
nice. thank you!
 
simple proof: If x=aq+r and y=bq+s, then x+y = (a+b)q+(r+s).
So if x=r mod q and y=s mod q, then x+y = r+s mod q.
 
yep :-)
 
Here's a number-theory question of my own, actually, motivated by my desire for this matrix I'm writing out to have simple parameters.
Are there positive integers $a<b<c$ such that $\dfrac{c+b}{c-a}$ and $\dfrac{c+a}{c-b}$ are both squares of rational numbers?
I don't know, actually.
 
$a=4$, $b=4$, $c=5$ @Semiclassical
Both fractions become $9$
 
@AkivaWeinberger a<b
 
4:58 PM
a<b
 
16,56,65?
@Semiclassical
 
That'd do it.
How'd you come up with that?
 
@AkivaWeinberger wow, impressive
 
$65\pm56$ and $65\pm16$ are all squares
 
5:06 PM
Hmm.
 
I thought it would be impossible lol
 
I Google'd for a number that could be written as the sum of two squares in two different ways
and got $65=1^2+8^2=4^2+7^2$.
 
Well, no need for a post on main :)
 
And then I messed with that a bit.
 
I'm still a bit amazed by that, to be honest.
 
5:08 PM
now, let's search for smaller solutions
you gave 65 as the upper bound
 
Note that $56=2(4)(7)$ and $16=2(1)(8)$ @Semiclassical
 
whistle
 
So the idea was that $(4^2+7^2)\pm2(4)(7)$ and $(1^2+8^2)\pm2(1)(8)$ are all squares.
Which is easily seen by the fact that those are just $(4\pm7)^2$ and $(1\pm8)^2$.
 
Could still make a main site question, I guess. "How does one generate triplets a>b>c>0 such that (c-a)/(c+b) and (c+a)/(c-b) are both squares of rational numbers?"
 
Either I ran into a comment you wrote earlier or there is another Akiva Weinberger commenting math pages on facebook :P @Akiva
 
5:12 PM
Mathematical Theorems You Had No Idea Existed, Because They're False?
 
precisely
 
4,23,27 with the help of program
 
@DHMO I don't think either of those give squares…
$50/23$ and $31/4$?
 
sorry, I meant 9,23,27.
 
Cool. 50/18 and 36/4.
 
5:18 PM
2,13,14
i'm not programming it to find the minimum
i'm just using it to partially help me
but at this stage it is bash-able
 
I see. Here (14+2)/(14-13) is the ratio of two squares, and (14-2)/(14+13) is the ratio of two triple-squares.
16/1 and 12/27=4/9.
 
11,13,14
and 2,13,14
are the minimum
 
huh.
interesting that they're so similar.
 
indeed, 11,13,14 generates 25/1 and 27/3
which is completely different
(2, 13, 14)
(11, 13, 14)
(4, 11, 16)
(9, 12, 16)
(11, 19, 21)
(1, 23, 26)
(22, 23, 26)
(18, 22, 27)
(9, 23, 27)
(4, 26, 28)
(22, 26, 28)
(14, 19, 30)
(8, 22, 32)
(18, 24, 32)
(17, 28, 32)
(4, 31, 32)
(17, 31, 33)
(19, 29, 35)
(11, 37, 38)
(26, 37, 38)
(22, 38, 42)
(6, 39, 42)
(33, 39, 42)
(19, 37, 44)
(12, 33, 48)
(27, 36, 48)
(47, 49, 51)
(2, 46, 52)
(44, 46, 52)
(9, 26, 54)
(36, 44, 54)
(10, 45, 54)
(18, 46, 54)
(1, 41, 55)
(43, 53, 55)
(8, 52, 56)
(44, 52, 56)
(7, 41, 57)
(28, 38, 60)
(13, 59, 62)
 
This seems like it might be related to Pell's equation
 
5:27 PM
I don't plan on optimizing it
 
That is… quite a few solutions.
 
is that sarcasm?
 
@DHMO There's a bunch of them that have a common factor and so can be reduced
@DHMO No, just awe. ("Quite a few" would mean "a lot")
 
good point
i don't plan on reducing them either
 
0
Q: Triples of positive integers $a,b,c$ with rational $\sqrt{\frac{c\pm a}{c\mp b}}$

SemiclassicalWhile working on a physics problem, I came up with a certain question in number theory: For positive integers $c>b>a$, can $\dfrac{c-a}{c+b}$ and $\dfrac{c+a}{c-b}$ both be rational squares? I asked this question on MSE chat (link) and a number of small solutions were quickly found, e.g. $...

I decided to make a question :)
Trying to decide if the title would read better with "$\sqrt{\frac{c+a}{c-b}},\sqrt{\frac{c+b}{c-a}}$" in place of the \pm / \mp construction.
I think it would. Changing.
 
5:40 PM
I just finished my analysis exam
 
how was it
ali
 
6:27 PM
[URGENT] I need a funny sentence about axioms
It's important
 
6:40 PM
Uhhh
There's the "Zorn's Lemon" joke I guess
 
is there a word which describes a single end point of the range of a function?
 
Boundary point, maybe?
Oh, wait, range
Extreme value, I think @greedIsGoodAha
A maximum or a minimum is an extremum.
 
can there be sets with 3(or more) distinct extreme values?
 
thanks akiva, that sounds good to me
 
what do you mean? @socrates
 
6:49 PM
Pretty sure you can't. Just a maximum and a minimum @Socrates
You can have lots of local maxima and minima
If the range is $[0,1]\cup[2,3]$ (possible if the function is discontinuous or has a disconnected domain or both), then only $0$ and $3$ count as extreme values. I don't know what you'd call $1$ and $2$.
 
so an ordered set is a two dimensional thing, in that sense
 
I'd say an ordered set is one dimensional
 
oh
 
Like $\Bbb R$
 
ups i misthought that^^
yeah
a line
 
6:51 PM
that's what a linearly (or totally) ordered set looks like
in a partially ordered set you can have a lot of maximal elements
 
Fun fact: any countable ordered set is order isomorphic to a subset of the rationals.
 
totally ordered*
 
Yeah
So, you're right, a "set with 3 or more extreme values" could exist if you allow partially ordered sets
(aka posets)
My phone just tried to autocorrect "poset" into "losers".
 
i don't use t9
or any autocorrecture
 
a maximum is always unique, as well as a minimum, if they exist but you can have a lot of maximal or minimal elements @socrates
 

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