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00:17
Two fields $F=(\Bbb R, +,\times)$ and $G=(\Bbb R^*,\times, \exp).$ $G$ is not closed under the addition of $F$ but one can still add elements in $G.$
So you can use addition in $G$ but you can't have the closure of the operation I guess?
maybe easier to state with groups, $(\Bbb R,+)$ and $(\Bbb R^*,\times)$ which are isomorphic
$(\Bbb R^*,+)$
that is closed under addition
why is this person saying that the mapping does not commute with addition?
01:05
Where is leslie when you want his guessing abilities.
01:17
huh?
LESLIE
I no longer need you.
But I can ask you if you wanted, anyway.
i guess you don't
slaps their knee
is it interesting or funny? or both?
Neither, in fact.
01:21
what a downer
I don't have any consolation jokes or facts for you.
as my daughter would say, phbhtbhtth
when are you going to start her on operator theory so that it becomes p*hb*htbh*tth
@TedShifrin 10
But that was not required for my question.
But thanks a lot for catching that. I just miscalculated it at that time.
I discard n=4 as follows: if there were such a union then in that union there will be at most 16-3 =13 elements (distinct) and 3 here is being subtracted due to identities presence in every subgroup that's part of the union.
I did a similar thing to discard n=5.
10 because 4 cyclic and 6 Klein 4.
01:39
Hi everyone, I'm trying to use reduced row echelon form in Matlab and Mathematica for an augmented matrix A=[1 -2 x;2 1 y;-3 1 z] where x,y,z are symbolic variables. Both software treat the matrix as 3x3 generating three pivots whereas the system has a most 2 pivots. How can I let Matlab or Mathematica to detect it as augmented matrix?
RowReduce[{{1, -2, x}, {2, 1, y}, {-3, 1, z}}]
yields {{1, 0, 0}, {0, 1, 0}, {0, 0, 1}}
it doesn't sound like they're even treating them like symbolic variables. i dunno. this is a software thing i am unfamiliar with. you could apply the row operations manually and stop when you clear the first two columns.
So you want the third column to be 'augmented'?
wolfram recognizes the cases. wolframalpha.com/…
@leslietownes I've done the manual calculation which is pretty easy but I'm surprised why the software failed to reach to the same result.
@Koro correct
croco: there must be some special syntax for augmented matrices or partitioned matrices where you only want to rref the first x columns, but i don't know what it is.
i never did symbolic calculation in matlab, it wouldn't surprise me if it were bad at that. but i haven't used it seriously in many years.
01:44
@leslietownes I think the posted link yields incorrect results.
it sort of makes sense that in general it wouldn't know what to do with a symbolic matrix unless all of the 'variables' are in the last column only. that's really key here. if the matrix is just of data type "any entry is some function of x, y, and z" it's going to choke on that. too many cases in the rref.
not sure what's goin' on here.
Actually I've faced this problem a lot, but I was lazy to investigate the problem and tend to do it manually.
croco: it's not treating it like an augmented matrix, but it's recognizing the relevant cases. it suggests that you'd end up with 0, 0, 5x+5y+5z (or with minus signs) in the last row if you do what you want to do.
I get (7x-2y)/3, (2x-y)/3, (3z+19x-5y).
hopefully I didn't screw it up.
but nonetheless, it shouldn't generate three pivots.
now try adding multiples of the first and second rows to that one, to clear out the first two entries.
you should get 0, 0, something and it wouldn't surprise me if it's what WA suggests ought to be there. i'm certainly not doing this calculation myself. you would definitely expect there to be three pivots a lot of the time if it's treating it as a 3x3 matrix. 0, 0, nonzero in the final row would, if you treated it as a 3x3 matrix, turn into 0, 0, 1.
01:50
I need them as this because I need to check the spanning vectors.
@Koro I do not believe this.
@leslietownes but I didn't understand when it says assuming non-zero and zero determinant.
Hi, munchkin’s slave.
croco: if you can get the first two rows to look like 1, 0, [something] and 0, 1, [something], respectively, then you can make the last row look like 0, 0, [something] where something is a linear combination of x, y, and z.
if it's 0, then you have a consistent system. if it's nonzero, you have an inconsistent system. those are the cases.
this is exactly what I've done.
01:54
and those happen to be the same cases as the determinant being nonzero and zero
i see
this is somewhat unique to this square matrix setting. for general rectangular matrices you could do the same calculation and you'd just have potentially multiple combinations of variables that have to be 0 for the system to be consistent.
in that sense, it's sort of an accident that the determinant has to give you the one condition in this case. but it's interesting that wolfram notices it, where mathematica apparently just assumes whatever expression you get in that last entry is nonzero so it can divide by it.
Actually I have two vectors of 3 dim. I'm trying to find their span set which I believe it is a plane
v1=[1 2 -3]^T and v2=[-2 1 1]^T.
Mathematica does the generic case, unless you give it rules that dictate otherwise .
@leslietownes I return for guessing abilities: let $\mu$ be an $\mathbb R^m$-valued measure over $\mathbb R^n$. What should the notation $\int_{\mathbb R^n}f(x)\,d\|\mu\|(x)$ mean?
01:57
anak: perhaps the total variation?
or whatever it's called?
Take the norm of the vector and do a real-valued measure.
it'll be a measure in the usual sense if mu is.
anak: en.wikipedia.org/wiki/Vector_measure calls it the "variation". my guess is it's that.
@TedShifrin this is the actual augmented matrix
A=
[ 1 -2 | x]
[ 2 1 | y]
[-3 1 | z]
this is system has two pivots.
how to tell Mathematica this info
@leslietownes So since x is merely a vector here, it's like Ted suggests and is just the norm, $x\mapsto\|\mu(x)\|$?
You want the constraint equations for consistency. Forget row reduction and use theory.
Where $x$ is a set in your sigma algebra?
02:01
I guess yeah it would have to be to make sense
anak: you might need to use a sup formula as in wikipedia in general for countable additivity but yes.
@TedShifrin I can do it manually since this is not a big matrix but for matrix 4x4, I keep getting same issue.
this is the example from the book I'm following.
I'm not able to get 11x+5y+2z=0 using software but I've managed to get it manually using rref
Theory (see my book or lectures) tells you to find a basis for the nullspace of the transpose.
Unfortunately, I couldn't get your book in my university's library. I will try your videos.
Ted, when are you going to release your textbook pdf online for the masses.
02:11
@anakhro we had this discussion before and it seems the publishers are the issue here.
well let's just say it's out there if you know where to look
coughs something about russian libraries
this water is full of dragons
@TedShifrin why not?
There are 4 elements of order 4.
Nope, let me rethink.
@anakhro Learn undergrad diff geo :)
There are 12 elements of order 4.
(order from 1st Z4, order for second Z4): (1,4),(4,1),(2,4),(4,2),(4,4)
02:25
So 6 subgroups?
@TedShifrin is this a mad diss against me :(((
So 2+2+2+2+4=12
Cyclic subgroups of order 4 is: 12/2=6
I agree: 6 subgroups and 1 Klein subgroup. Your 4 was nuts.
Oh, right, 6. Even nuttier.
Order 2 elements are: 2+1=3 so number of K4 is 6.
Total number of subgroups is: 12
You’re crazy.
Give me the Klein subgroups explicitly.
02:28
{identity, 3 choices for order 2, 2 choices, 1 choice} and we have 3 elements of order 2.
Write them down.
{(0,0),(0,2),(2,0),(2,2)}
Oh 1 only!
Yup. You need to be careful!
Thanks a lot. :)
Sure :)
02:30
@TedShifrin *cyclic
So total number of subgroups of order 4 is 7.
Yes, right.
I believe so.
:)
there's 16 people in the chat
a few hours ago there were only 5
participation in the chat was very less yesterday @geocalc33
02:46
I can depart.
“Very less” is an odd construct.
In this video (youtube.com/watch?v=dNLmvhZWEq8), the professor solves a heat equation with two boundary conditions and one initial condition, $u(x, 0) = 0$ via the similarity solution method. The PDE is used to construct a second order ODE, and two boundary conditions determine the two arbitrary constants from the ODE. However, the initial condition is never used. How is it possible to solve the heat equation without using the initial condition?
Does the similarity solution method only work for that particular initial condition and use it implicitly?
03:11
I expect participation to be high tomorrow
03:29
I have come across two definitions of what is means for a set to be connected, and I am unsure why they are equivalent.
The first: $A\subset X$ is connected iff there do not exist open sets $U$ & $V$ in $X$ with $A\subset U\cup V$, $A\cap U\neq\emptyset$, $A\cap V\neq\emptyset$, & $A\cap U\cap V=\emptyset$.

The second: $A\subset X$ is connected iff the only subsets of $A$ that are both open and closed in the relative topology of $A$ are $\emptyset$ and $A$.
I like to think of the first as $A\subset U\cup V\rightarrow\left[A\cap U\cap V=\emptyset \rightarrow\left(A\cap U=\emptyset\lor A\cap V=\emptyset\right)\right]$, for every $U$ & $V$ in $X$. This reads as: When $A$ is a subset of the union of $U$ & $V$, if the intersection of $A$, $U$, & $V$ is empty, then either $A$ does not intersect with $U$, or $A$ does not intersect with $V$.
Normal rewriting things like this is sufficient to understand the link between two definitions, but in this case it has not been, because I was unable to write the second definition out in an equally expanded form. So I ask, how exactly are these two definitions equivalent?
03:41
@user400188 can you show that the definitions are equivalent if you consider $A=X$?
i don't think that thinking in symbolic sentences is a good way of unraveling one definition into the other. it sometimes is the simplest way (and maybe always is if you are a computer) but maybe not here.
That is, can you show "there do not exist non-empty open sets $U,V$ such that $X = U\sqcup V$" and "the only clopen subsets of X are X and the empty set" are equivalent.
From that, it's pretty natural to extend it to the relative topology case.
03:59
@anakhro I am not sure if I understand the first definition, and how it relates to the original. If there do not exist non-empty open sets $U$, $V$ such that $X=U\cup V$, then isn't that equivalent to saying that all non empty sets $U$,$V$ satisfy $X\neq U\cup V$? If so, that requirement of 'all' non-empty sets would include $X$ itself, which would have to satisfy $X\neq X\cup X$. Hence my confusion.
DISJOINT
@TedShifrin So it's meant to be "non-empty disjoint open sets..."?
Ok, thank you. I'll continue to try and show them equivalent.
Without that, of course you’re totally confused.
04:07
Exercise: show that topology is inconsistent.
Exercise: Do not trust sloppy crap on the internet.
That's where most of my learning in abstract mathematics takes place though. Although most of it isn't sloppy. (At least, I don't think it is.)
@TedShifrin đź’© . o O ( trust me )
04:22
I think I have shown that the first definition leads to the second, but not the other way around yet. I'll write out the first to second now just to make sure.
If there do not exist disjoint, non-empty open sets $U,V$ such that $X=U\cup V$.
- All disjoint, non-empty open sets $U,V$ satisfy $X\neq U\cup V$.
- Assume, for the sake of argument, that 'there exists a subset $A\subset X$ which is clopen, nonempty, and not equal to $X$.'
- - $A$ is open and non-empty.
- - $X\neq A\cup V$, for any $V$.
- - If $A$ had elements in common with $X$, but missed out on some, and had no more elements (i.e. $A=X-B$, for some $B$), then we could pick a $V$ to fill in the gaps. This is a contradiction, so it's not the case that for some $B$, $A=X-B$.
04:47
And I think I have the other direction now, if anyone actually understood what I wrote the first time.
If the only clopen subsets of $X$ are $X$ and the empty set:

- Then assume, for the sake of argument, that there exist disjoint non-empty open sets $U,V$, such that $X=U\cup V$.
- - $X-U=V$
- - $U$ and $V$ are open, so $U$ is clopen.
- - $U\neq\emptyset$, so $U=X$
- - But if $U=X$, then $V=\emptyset$. Although $V\neq\emptyset$.
- - Contraction
- So it must not be the case that there exist disjoint non-empty open sets $U,V$, such that $X=U\cup V$.
So if the only clopen subsets of $X$ are $X$ and the empty set, then there do not exist disjoint non-empty open sets $U,V$ such that $X=U\cup V$.
Did those two proofs(?) (if you can call them that) make sense @anakhro @TedShifrin?
05:20
I didn't read it all. But you need to say that $X-A$ is open (in $X$), which means ...
"then we could pick a $V$ to fill in the gaps" leaves something to be desired, even if it gets at the idea.
Leaves lots to be desired.
Even red leaves in the autumn won't do.
there are a few missing "open"s. it is often the case that U and V represent open sets, the same way that z often represents a complex number and x a real number. but if you're using it you should mention it.
might be possible to untangle some of those negations and contradictions, too, althoug that is more exposition than logic
Hi, suppose that I'm maximizing the perimeter $P(x,y,z)=x+y+z$ of a triangle in a ellipse $x^{2}/a^{2}+y^{2}/b^{2}=1$. Can I use Lagrange multipliers? Lagrange multipliers says I need to solve the equation $\nabla f=\lambda g$ where $f$ is the objective function and $g$ is the constraint. But here, we have $\nabla P=\lambda g$ with $g=x^{2}/a^{2}+y^{2}/b^{2}-1=0$ and then $(1,1,1)=\lambda(1x,1/2y,0)$ but then $1=\lambda 0$ but is not make sense. How can I use Lagrange multipliers here?
so in P(x,y,z), your symbols x, y, and z are lengths of sides in a triangle in the plane? do i read that right? but in the equation of the ellipse x and y are coordinates of a point in the plane?
05:32
Oh, well there is a real problem in my approach
Uhm
you might need more letters. certainly possible to parametrize this thing in some way to to get multivariable calculus to apply to it, but not if x and y are different things in different functions.
might help to try the case of a circle first.
Yeah, I am not sure how I should write it more precisely. $V=B$ does not work because $B$ might not be open, it has to be $V=(B+\text{some other things to make it open if it isn't already})$.

Also, you are right that I forgot to mention a few times that $U,V$ are open. I say so at the start, but I also should have said it whenever I wrote "for 'any' $U,V$.
I was reading a similar approach here in MSE with a rectangle, but I don't have the link because seems MSE is in maintenance. By the way, "$(1,1,1)=\lambda(1x,1/2y,0)$ should be "$(1,1,1)=\lambda(2/a^{2} x,2/b^2 y,0)$". I'm sorry.
@TedShifrin Did you happen to mean my $A$ from the proofs I attempted to write, or the $A$ in the original definition?
@leslietownes Yes, for all the question. I think the problem is that the function $P(x,y,z)$ depends of three variable but $g(x,y)$ the constraint depends of two variables.
05:44
alex: it's a little more than that. the x, y in g(x,y) are coordinates of a single point, and the x, y in P(x,y,z) are lengths of sides between points (not coordinates that satisfy the constraint). you're not maximizing P(x,y,z) subject to g(x,y) but to some more complicated constraint that is not easy to express as a constraint on the lengths of sides.
Well, I understand that :-(
mse main site seems to be having a lot of issues lately
i think it might help to try the circle case first. you could well assume one of the points is (1,0) and if you parametrize right you can represent the other two points in two variables instead of four and they are not constrained.
@copper.hat There is a post on meta.se about cyber attacks.
if you want to think of the points in the triangle as pairs subject to the constraint then the perimeter would be a function of six real variables (subject to constraints), or four if you fix one of them at (1,0).
05:47
damn cylons
@user400188 thanks :-)
lots of flexibility in setting these kinds of things up but the choices do matter and the setup that makes the most 'sense' from a 'just write it down' point of view might involve complicated calculations.
pays to be clever.
i am sorry i did not take up a life of crime (apart from driveways).
the opportunities are endless with the interweb
thank you leslie, I'm going to think about this some more.
I like how Axler shows that for every operator T in L(V), there is a one dimensional or two dimensional T- invariant subspace of V.
Using complexification :)
 
4 hours later…
10:09
@robjohn cheers, so the joint distribution would be $\Pi_{i=1}^n f_{X_i}(x)$, this is only normally distributed when $p = 0$ or $1$, or when the two distributions are the same?
10:27
Hello, I have this sequence defined by $u_{n+1}=u_n+\frac{(-1)^n}{n+1}, n\in \mathbb{N}^*$
$u_1=1$
I proved that $(u_{2k})$ and $(u_{2k+1})$ are adjacent
Son they have the same limit
Then $(u_n)$ converge also to the same limit
I want to find an interval for the limit
I say $u_2\leq u_{2k}\leq u_{2k+1}\leq u_3$
Because u_{2k} is increasing and u_{2k+1} is decreasing
My question is : is u_{2k+1} start for k=1 or k=0 ?
That is I must say $u_{2k+1}\leq u_1$ or $u_{2k+1}\leq u_3$ ?
10:52
Oh sorry it is less then u_1 I don't know why I don't see this
@Govind75 I thought you were interested in the mean of two distributions. The probability of $N(\mu_1,\sigma_1)$ is used is $p$, and the probability of $N(\mu_2,\sigma_2)$ is used is $1-p$.
hi, can anyone help me out with this ? imgur.com/a/0HnnnAu, in the highlighted part of the second page, im not sure why $\nabla_{e_i}(e_j)$ can make sense if $\nabla$ is a map from vector fields on the entire manifold squared, but the $e_i$ are only defined on some open subset $U$, im guessing this is because $\nabla$ really only depends on local info but this hasn't been shown yet so
Does it make sense to add a quaternion to a location in 3d space?
I'm programming some physics stuff for games and found some code that does this and I don't quite understand what the purpose is. Code reads :

`const FVector lTargetPositionInWorld = lOwnerTranslation + lOwnerRotation *(
(mInitialRelativeTranslation + mInitialRelativeRotation.Quaternion() * lBoneTranslation));`

Where rotations are quats and translations Vec4
11:26
@robjohn ah, I was tryna describe the joint distribution of $X_1,...,X_n$, I thought the joint pdf would be what I said above where each $f_{X_i}(x) = pf_1(x) + (1-p)f_2(x)$
Where $f_1(x)$ is the normal pdf for distribution 1 and likewise for $f_2(x)$
11:50
disregard my question, didn't read the operation well, it's rotating a vector then adding the result -_-
 
2 hours later…
14:06
@user400188 Sorry, the point of using \sqcup over \cup is to indicate that the union is disjoint.
14:36
hi
can anyone walk me through what it means for an integral transform to have a symmetry under $f(x) \to f(1/x)$?
@geocalc33 do you have a reference for where you have seen this mentioned?
I can try to find the comment
found it
"Indeed, the Mellin transform is a multiplicative-coordinate analogue of Fourier transform, and like the symmetry of Fourier under $f(x) \to f(-x)$ there is a symmetry of Mellin under $f(x) \to f(1/x)$"
15:24
Does anyone know how to solve this: Let $X=A_1\cup\cdots\cup A_k$ where $k\geq 2$, sets $A_j$ are Jordan curves and $|A_j\cap A_{j+1}|=1$ (a set that has exactly one element) for every $1\leq j\leq k-1$ and $A_j\cap A_k=\emptyset$ for every $|j-k|\geq 2$. How one can show that $\pi(X)$ is not an Abelian group?
@geocalc33 can you link to the comment?
The symmetry for Fourier I thought had have a conjugate, $\hat f(x) = \overline{f(-x)}$.
Sorry, the second f should also have the hat.
15:47
3
A: Mellin transform of $f(1-x)$

ChappersNo. For one thing, most of the values of $f(x)$ in the integral for $F(s)$ are completely different from the values of $f(1-x)$ in $M(f(1-x))$: the former takes values from $f([0,\infty))$, while the latter uses $f((-\infty,1])$.

it's the comment under this answer
@anakhro
Wait can a 1D autonomous equation have infinitely many orbits?
I was thinking yes but my mate keeps saying it’s impossible, $\dot{x} = 1$ surely I can get infinitely many orbits as I can have different paths $t+C$
@Govind75 Yes, that's an easy example.
@geocalc33 I don't know the Mellin transform, but I figure it's something like the conjugate symmetry of the Fourier transform.
@anakhro is $\hat f(x)$ the transformed function?
for Fourier
Yes.
 
1 hour later…
17:13
@JaakkoSeppälä Have you drawn pictures? How do you show the fundamental group of a figure 8 is not abelian?
@Govind75 You’re misunderstanding. In dim 1 there is precisely one orbit. Look at $\dot x = Ax$ in $\Bbb R^2$.
 
1 hour later…
18:20
Why is there only one orbit?
Because one flow line fills up all of $\Bbb R$.
Oh, you said 1D.
Your mate wins.
Not a maths question, but can anyone British, say what's cool/cute about Paddington bear. I got an English assignment on Wojtek the polish and I got no clue what Paddington bear even go to do with it.
Is the orbit a range of values?
Orbits are the flow lines — the curves that are the solutions to different IVPs. You need to learn definitions.
Yeah, so surely the example I gave gives infinite different orbits?
In 1D
18:35
Surely? There is precisely one orbit.
What is it?
Every point is hit by any one of your solutions. It's just at different times. Who cares.
All of $\Bbb R$ is one orbit. The only way you can get more than one orbit is to have singular points (so that each of them will be an orbit by itself).
For example, $\dot x = x(x-1)$. Figure that one out.
Well, maybe start with $\dot x = x$. Then do the other one.
$\frac{1}{1-Ae^t}$?
The latter one is $e^t + C$
Nope on both, I believe.
But you're giving $x(t)$, not answering the orbit question.
$Ae^t$?
18:40
Yes, that one is correct. So what are the orbits?
It's the set of values taken by $Ae^t$ when $A$ is varied
So how many orbits?
Infinite?
yeah
18:44
I gave you a clue when I mentioned singular points. What are the singular points here? (or equilibrium points?)
You get equilibrium when $x = 0$ right?
Yes. So that is one orbit. Now what?
So $O(0)$ is a singular point
Then I get one more orbit for the other values of $x$
Can $x$ ever be $0$ though?
No, you can't get just one more orbit. Think about it. Orbits have to be connected, so one can't jump over $0$.
Lemme get the definition of an orbit straight, for any general solution $\lambda(t,t_0,x_0)$, we define the flow to be $\phi(t,x) = \lambda(t,0,x)$ - which is basically the general solution but around the initial condition $(0,x)$. Then the orbit is $O(x_0) = \{\phi(t,x_0) | t \in J_{\textrm{max}}\}$
where $J_{max}$ is our maximal time interval about $t=0$
18:57
OK, fine :) Note that $e^t>0$ for all $t$, so the sign of $Ae^t$ is completely dependent on the sign of $A$. Thus ...
So for $A > 0 $, our orbit is $(0,\infty)$, for $A = 0$, our orbit is $0$, for $A < 0$ our orbit is $(0,-\infty)$?
Bingo. I would write $(-\infty,0)$, but yes.
So three orbits. Now what happens with my more complicated example?
I get $log|x-1| - log|x| = t+C$, but I feel like I need to be careful from here
OK ...
I wanna just combine the logs and then exponentiate giving $\frac{x-1}{x} = Ae^t$
19:06
Provided $x\ne 0,1$ you're OK.
Yeah and then $1 - \frac{1}{x} = Ae^t$
So you work on it and tell me how many orbits.
But my general solution was wrong
You have the same issue with your first one. There you get $\log |x|=t+c$ and you have a problem with $x=0$.
You need to observe that if $x_0$ is a singular point (i.e., $\dot x=f(x)$ and $f(x_0)=0$), then $x_0$ is automatically an orbit.
That makes sense
Ohhhh
I guess up to this point I've only ever been looking at the solution
So $x = 0 $ or $ 1$ gives a singular point
19:15
Yup.
And then the rest will be governed by $\frac{1}{1+Ae^t}$
So, in summary, how many orbits?
Yup.
Go back and talk to your mate now :)
Cheers
So it is impossible in $1D$ to have infinitely many different orbits
 
1 hour later…
20:31
Can you write a continuous function that has infinitely many zeroes?
Oh! Oh!
I can!
Pick me!
21:05
$sin(x)$
Im confused, so are there infinite orbits or not, dies $\dot{x} = sin(x)$ product infinite singletons?
 
1 hour later…
22:10
I've spent 3 years on this question. If I have two subpopulations $A_1,...$ and $B_1,..$, where $A \sim N(\mu_1,\sigma_1^2)$ and $B \sim N(\mu_2, \sigma_2^2)$ and the
What do you mean by producing singletons?
Now if I take a random sample $X_1,...,X_n$ where there is $\alpha$ probability $X_i$ is from $A$ and $1-\alpha$ probability $X_i$ is from $B$, what would the joint distribution of $X_1,...,X_n$
Points $x$ that give $\dot{x} = 0$?
infinite robots?
oh, orbits. nvm
Any idea for the stats one, my first though was $f_{X_i}(x_i) = \alpha f_1(x_i) + (1-\alpha)f_2(x_i)$ where $f_1, f_2$ are the pdfs of the respective normal distributions above
somehow infinite singletons seems contradictory
22:16
Is it because the maximal time interval would be finite?
A singleton means one of something.
makes sense
there's a lot of this around 'finite'/'infinite' as adjectives.
every open cover has a finite subcover. here 'open' refers to elements of the subcover, and 'finite' refers to the subcover (and not its elements).
elements of the cover, i should have said in the first part.
it's sometimes helpful to insert words between finite/infinite and what they modify. e.g. instead of 'infinite singletons,' 'infinite collection of singletons' clarifying that 'infinite' refers to the family itself, not to a property of individual members of the family.
Or is the distribution of $X_i = \alpha A + (1-\alpha)B$, then it's a lot simpler :)
But idk which one to choose agh
22:55
@leslietownes You missed the earlier discussion of how many orbits $\dot x = f(x)$ has. The word singleton is inappropriate. We're talking about singular points, equilibrium points, or zeroes of $f$.
And then @Koro was thinking about group actions and orbits. Orbits must be in the air.
@leslie Here is one for you to answer quickly.
23:15
looks like others are on it. my answer would have been that there's no reason for an operator to have eigenvalues no matter what the field is although i hesitated to answer because i was afraid the response would be "well what if they do??? where are they?" getting back to his fundamental discomfort with the field-dependence of the definition.
once you stop distinguishing between vector spaces, or allow yourself to embed the thing you care about in a larger space where the operator might have some natural extension, you can create all kinds of things, including eigenvalues where there were none in the smaller space. but probably not what this guy was asking.
my complex analysis book wants me to prove that if the coefficients of two polynomials differ by less than $\epsilon$ and the first doesn't have any roots on the unit circle, then they have the same number of roots in the unit disk
I know how to prove that, but not using any complex analysis.
seems like some quantifiers are missing. e.g. what does it mean for coefficients (lists of numbers) to 'differ by epsilon' and maybe even what epsilon is. 1 and z aren't that far apart as lists of coefficients but have different numbers of roots in the unit disk.
look in the index for rouche's theorem.
ooooh right Rouché's theorem
thanks. I hope I manage to learn this type of problem solving skill
23:46
@Derivative Oh really?

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