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01:07
ilikemathematics if you choose any basis for a vector space (such as V^*) and any function from that basis to another vector space (such as V^double star) then there is a unique linear map that extends that function to all of the vector space
so if you just want some random map it's not interesting
Ah, you're right
Thanks
there's probably questions on main or MO about what it means to define a 'natural' map from one thing into another, there is always something from V to V star star but not into V star
although formalizing and proving that kind of stuff is not something that a healthy person should care anything about
 
1 hour later…
02:41
How are the munchkins getting along? @leslietownes
02:56
every day a little bit better!
03:13
cool
04:00
@leslietownes I love the double dual
04:24
@nickbros123 It doesn't love you, and it asked me to tell you to stop sending love notes and flowers.
It's creepy, dude.
Bob
Bob
04:49
good evening
I would like to know why I cannot reopen this question:
3
Q: Solving a system of two differential equations with no initial conditions given

BobProblem: Use the operator method described in this section to find the general solution of the following system of differential equations. \begin{align*} x' + y' - 2x - 4y &= e^t \\ x' + y' - y &= e^{4t} \end{align*} Answer: \begin{align*} Dx + Dy - 2x - 4y &= e^t \\ (D-2)x + (D-4)y &= e^t \\...

05:26
@XanderHenderson I thought we had something special, you mean to say when it gave me the canonical basis to V from V*, it was just being nice? come on Xander
 
2 hours later…
08:03
a boo
08:46
I've just realized that the real line admits multiple different complete uniform structures.
In particular, the fine uniformity on $\mathbb{R}$ effectively identifies the hyperbolic cosine function as uniformly continuous.
09:40
> Let $\mu$ be a finite measure on $(\mathbb R,\mathcal{B}(\mathbb R))$. For every $x\in\mathbb R$, let $$F_\mu(x)=\mu((-\infty,x]).$$ The function $F_\mu$ is increasing, bounded, right-continuous and such that $F_\mu(-\infty)=0$.
I struggle with a small detail of the right continuous part. Suppose now that $x\in\mathbb R$ and that $(x_n)$ is a decreasing sequence with limit $x$ (e.g. $x_n=x+1/n$). Then $(-\infty,x]=\bigcap_{n=1}^\infty (-\infty, x_n]$, and so by continuity from above we have $F_\mu(x)=\lim_{n\to\infty} F_\mu(x_n)$. Thus $F$ is right continuous, since for any $x<y<x_n$, we have $|F(y)-F(x)|\leq|F(x_n)-F(x)|$.
Question The inequality $|F(y)-F(x)|\leq|F(x_n)-F(x)|$ shows that $|F(y)-F(x)|<\epsilon$ for $n>N$, right? But what definition of continuity is this satisfying? I'm confused about the $n>N$ part, since there's nothing in $|F(y)-F(x)|$ that depends on $n$.
The argument "Thus $F$ is right continuous, since for any $x<y<x_n$, we have $|F(y)-F(x)|\leq|F(x_n)-F(x)|$." appears in Cohn's book, and I'm paraphrasing from there.
Actually, the act of choosing $y$ is dependent to $n$, for $x_n$ acts as an upper bound.
true :)
hmm, the whole argument, by writing $|F(y)-F(x)|\leq|F(x_n)-F(x)|$ for $x<y<x_n$ seems unnecessary
This utilizes the sandwich theorem.
If one just left it at $|F(x_n)-F(x)|<\epsilon$ for $n>N$, then at least this would be the sequential definition of continuity, but I'm puzzled at what introducing $y$ and writing $|F(y)-F(x)|\leq|F(x_n)-F(x)|$ brings to the table.
The $y$ must be involved because the sequence $x_n$ doesn't cover a right-open interval $[x, x + \delta)$.
Though, yeah, the sequential continuity coincides with the (usual) continuity when the space involved is metrizable.
Yet still, this fact cannot be used for one-sided continuity.
09:56
@DannyuNDos what do you mean by $x_n$ doesn't cover a right open interval $[x,x+\delta)$? How does introducing $y$ help us cover $[x,x+\delta)$?
By "doesn't cover", I mean there does not exist a $\delta > 0$ such that $[x, x+\delta) \subset \{x_n\}_{n=1}^\infty$.
So we need $y$ to, intuitively speaking, "fill the gaps" of the sequence $x_n$.
By introducing $y$, we're basically turning the sequence $x_n$ of points into the sequence $[x, x_n)$ of intervals.
ok 👍
 
2 hours later…
11:47
I don't get how do they claim that, "Each $P_i$ is isomorphic to $P^1$ ..." (highlighted part in the last image). Can someone please help me with it?
12:07
The conjugation map $x \mapsto \sigma^{-i} x \sigma^i$ is an isomorphism from $P_1$ to $P_i$
12:31
libgen is not working?
12:42
Looks like it
13:08
has anyone read the book "Introduction to probability models" by Sheldon Ross?
would you recommend?
13:28
@nickbros123 yes.
@nickbros123 for what?
I have a course on probability and stochastic processes
course outline seems rather application based rather than measure theoretic based
14:14
@VladimirLysikov Fine... I get it. But can you explain the line that follows after the highlighted text? I think there might be confusion with the phrasing tho.
to say that a permutation f of integers "influences" an integer k is presumably to say that f(k) is not k
there is an implicit claim that if f and g are permutations and they "influence" disjoint sets of integers, then they commute
the compositions fg and gf will both be "do f on the set that f influences, and do g on the set that g influences." you can find versions of this on main and on the web
@nickbros123 Is that the book assigned?
15:02
Consider an increasing, right continuous and bounded function $F:\mathbb R\to\mathbb R_+$ such that $F(-\infty)=0$. Then this function gives rise to a unique finite measure $\mu$ on $(\mathbb R,\mathcal B(\mathbb R))$ such that $F(x)=\mu((-\infty,x])$. Now, my book then goes on to define the Lebesgue-Stieltjes integral for every bounded Borel measurable function $f:\mathbb R\to\mathbb R$ $$\int f(x)\,\mathrm{d}F(x):=\int f(x)\,\mu(\mathrm{d}x).$$
I wonder, why only for bounded Borel measurable functions?
Or put differently, why do we require boundedness?
perhaps to avoid any issues around "convergence"
yeah
i wouldn't assume that any hypotheses in a treatment like this are necessary in any strict sense, it's just, there's a whole world of math around potentially divergent integrals and if that's not the subject of today's lecture then you maybe add hypotheses to avoid it
right 👍
I just thought the word "bounded Borel measurable function" popped up quite suddenly in the sequences of definitions and theorems in the book, but as you say, it's probably just to reserve the integral for finite things (for the moment being), which we've discussed before :)
this is something that very roughly separates introductory algebra from introductory analysis, if there is a hypothesis in an intro algebra book it is more likely to be there for some "real" reason other than convenience
whereas almost everything in analysis is convenience oriented and the vast majority of people who somehow care about what hypotheses are both necessary and sufficient for the FTC to hold aren't analysts
as one randomly chosen example
PDE people are more than happy to prove some inequality with like 10,000 more hypotheses than necessary to deal with one equation and you won't learn anything useful by asking why they didn't assume some weaker thing
15:14
:D
15:43
@leslietownes Thanks for the clarification!
@XanderHenderson it's in the list of recommendations in the course catalogue, yes
How do you justify that $\begin{pmatrix} 1 \\ 1 \end{pmatrix} \otimes \begin{pmatrix} 1 \\ 0 \end{pmatrix} = \begin{pmatrix}1 \\ 0 \end{pmatrix} \otimes \begin{pmatrix}1 \\ 0 \end{pmatrix} + \begin{pmatrix}0 \\ 1 \end{pmatrix} \otimes \begin{pmatrix}1 \\ 0\end{pmatrix}$ can't be given by $x \otimes y$ in $\mathbb R^2 \otimes \mathbb R^2$? We know that a basis of it is equal to
$$B = \left\{\begin{pmatrix}1 \\ 0\end{pmatrix} \otimes \begin{pmatrix}1 \\ 0\end{pmatrix}, \begin{pmatrix}1 \\ 0\end{pmatrix} \otimes \begin{pmatrix}0 \\ 1\end{pmatrix}, \begin{pmatrix}0 \\ 1\end{pmatrix} \otimes \begin{pmatrix}1 \\ 0\end{pmatrix}, \begin{pmatrix}0 \\ 1\end{pmatrix} \otimes \begin{pmatrix}0 \\ 1\end{pmatrix}\right\}$$
I mean, we probably can't say "you just see it from the basis"
I guess you can say it's because of the distributivity, we have $e_1$ as first vector once and $e_2$ afterwards. You can't obtain that with $x \otimes y$. Is there a different argument too?
Nevermind, I should've picked something like $e_1 \otimes e_2 + e_2 \otimes e_1$; like this, it's obviously expressible by $x \otimes y$.
16:38
Reading on Wikipedia about support of a function. I always forget what is what here, but if $f:X\to\mathbb R$ (where $X$ is some topological space) is continuous, then everything simplifies it seems. The set-theoretic support of a function is then simply the open set $f^{-1}(\{0\}^c)$ and the support is the closure (in $X$) of this open set. (Correct me if I'm wrong.)
I'm trying to figure out, if $f:X\to\mathbb R$ is continuous and $X$ is a locally compact metric space, and $f$ is compactly supported, if then it vanishes outside a compact set? But I find this difficult, since the support of the function doesn't seem to be strictly speaking the set on which it is nonzero.
16:59
@psie I don't know what "set-theoretic support" is, but yes, support of a function is defined as the closure of the set of points $x$ for which $f(x)\neq 0$
@psie that $f$ is compactly supported means that $\text{supp}(f)$ is compact
By definition, $f$ vanishes outside of $\text{supp}(f)$, and so if its compactly supported, then it vanishes outside of a compact set
and conversely, if $f$ vanishes outside of a compact set $K$, then the set of the points for which $f$ is non-zero is contained in $K$, so support of $f$ is contained in $K$, so support is compact
@Jakobian ok, makes sense, but it is possible for $f(x)=0$ for $x\in \text{supp}(f)$, or?
yes
it's possible
If the set of points for which $f$ is non-zero is not closed, and it most often isn't, then there will exist some $x\in \text{supp}(f)$ with $f(x) = 0$
ok 👍
 
2 hours later…
19:00
Hello, I was trying to solve the following exercise :

Let M be a compact manifold of *positive dimension*, and let p \in M . Show
that M is homeomorphic to the one-point compactification of M\{p}

I think I have solved the exercise but at not point I had to use the hypothesis that M has *positive dimension*. So I tried to study the 0-dimensional case in particular and unless I am mistaken in that case, since M is compact and discrete, it is a finite set with the discrete topology, and in that case, I think the one point compactification of M\{p} is also just a finite space with the discret
19:15
anthony all of that seems right, i would expect that the hypothesis is simply to exclude a category of spaces that don't resemble what normal people think of as manifolds
i'm not 100% sure of whether people would use 'compactification' to describe what is happening in the case where you have a finite set of points (i.e. a space that is already compact) and add another one
maybe they are also avoiding the case for that reason
"manifold of positive dimension" is just a bizarre way of saying "manifold" to me, i wouldn't think of the 0 dimensional case as having anything to do with what i think of manifolds as being
but there's no shortage of bizarre people in mathematics
@leslietownes the concept of "manifold of positive dimension" was introduced by Ted
19:41
@leslietownes Thank you for your help, you are probably right when it comes to the reason why the additional hypothesis was included in the exercise. Your confirmation is enough for me to consider the exercise solved and to move on to another one.
Just for the sake of completeness, the definition of the one-point compactification of a space X (assumed to be locally compact and Hausdorff) that the author uses is to add a new point called \infty to X, and then define the open subsets of this new space X* = X \cup \infty to be the open subsets of X, and the subsets U such that X*\U are compact subsets of X.
yeah, that seems fine to me, i just don't know why anybody would consider a compactification of a space that is already compact, and maybe that is where the exercise writer is coming from. this may be a situation where definitions and intuition just depart from one another (another way of rephrasing my remark above, is that the assumption that M has positive dimension, is exactly what ensures that M \ {p} is not compact and hence could be thought of as in want of a compactification)
from a pedagogical point of view, it was maybe a mistake for this writer to introduce 0-dimensional manifolds in the first place. offhand, i can't think of how you improve life by doing this, but there must be some reason for it
@leslietownes To be fair, it seems like a lot of definitions in the field of manifolds/topology can vary slightly depending on which author is writing them, so it might explain why people tend to be extra careful and present exercises/propositions in such a way that they are true in one definition and wrong in another. But I agree that sometimes some choices of definition are quite high on the bizarre scale
@leslietownes I get your point and I agree
is there a way to instantly get emails when you get a notification on the main site?
@leslietownes Thank you again for your help
@ModularMindset the speed of light is an obstacle to 'instantly' :)
19:50
I guess an alternative option is to get desktop notifications
i have generally found SE notifications (i only use it on desktop) to be pretty sporadic and, if i were planning on relying on them, unreliable (i use the network only for recreation so it basically doesn't matter). e.g. sometimes i'll get a notification of something that happened like a week ago, and anybody who assumed i was getting notifications in real time would have their expectation frustrated
20:20
@nickbros123 At every institution I have ever interacted with, books come in two categories: required texts, and recommended texts. Instructors generally teach along the outline of the required text(s), but may recommend exercises or exposition from the recommended texts from time to time.
If it is a required text, I don't see as it matters if it is any good or not. You will need it for the class. If it is a recommended text, I would generally wait to see how the instructor is using it.
In any event, I think that Ross' book is perfectly fine. It has been 20ish years since I've opened it, however, so my memory could be wrong.
sometimes the choice of book matters less than the fact of making a choice of book
@leslietownes Indeed.
TLDR; questions from the required textbook show up on tests :P
@handan_toddler If you want to be cynical, sure.
Though I've had instructors who pulled exam problems primarily from the recommended texts, rather than the required one.
Ouch 😳
Without any mention of it in the class notes?
20:42
Let $\varphi: V \to W$. Then there exists a unique $$\hat \varphi: U \otimes V \to U \otimes W \quad \text{with} \quad \hat \varphi(u \otimes v) = u \otimes \varphi(v).$$ Show that if $\varphi$ is injective, so is $\hat \varphi$.
Does my solution look fine? We will instead show $\ker(\hat \varphi) = \{0_{U \otimes V}\}$. So let $f \in \mathcal L(U, W; K)$ be arbitrary. Then $$(u \otimes \varphi(v))(f) = f(u, \varphi(v)) \overset != 0_K.$$ Since $f$ is arbitrary, we can assume $\ker(f) = \{0_{U \times W}\}$. So we get $u = 0_U$ and $\varphi(v) = 0_W$. Since $\varphi$ is injective, we get $v = 0_V$.
@handan_toddler I mean, generally the understanding is "These are recommended texts. They cover the same material as the required text(s), but may take a slightly different approach, or give different exercises. You might want to read them."
If a book is "recommended", it is nigh certain that the instructor will be using it for something, including exercises which might show up on an exam.
Seems perfectly fair and reasonable to me...
Sure if that statement is made upfront in the notes.
@ILikeMathematics First, you need to consider $\hat{\varphi}$ on arbitrary tensors, not only on tensors of the form $u \otimes v$. Second, what is $\ker(f)$ for a bilinear map?
If a simple function $f$ is in $L^p$ for $1<p<\infty$, is it in $L^1$?
I know the converse holds, but I'm not sure how to argue about this direction.
@handan_toddler I don't understand. A book is recommended. That, all by itself, is a statement that the material in that book might be fair game.
20:54
@VladimirLysikov $\hat \varphi$ and $\varphi$ are both linear
Ah
You mean $f$ is bilinear
Ok, I should've written "Since $f$ is arbitrary, we can assume it only maps to $0$ for $u, v$ equal to $0_U$, $0_V$ respectively where $f(u, v) = 0_K$.
@XanderHenderson ok
@ILikeMathematics There are no such maps. We always have $f(u,v) = 0$ when $u = 0$, $v \neq 0$
The first thing you addressed makes the proof unusable
@VladimirLysikov Ah
Yeah
You need to consider arbitrary tensors and choose the bilinear map $f$ accurately depending on the tensors
21:17
@leslietownes as far as I know, the concept of "one-point compactification" as extension by one isolated point in the case of the space is compact is useful in algebraic topology etc.
while not compactification, it's still okay to name it this way, I guess
@Anthony for most people, a space is supposed to be dense in its compactification. While this will give you some new space if $X$ is compact, it's a bit sketchy to call that one-point compactification, because $X$ won't be dense in it
@VladimirLysikov Ok, let $u \otimes \varphi(v) = z \otimes \varphi(w)$. We need to show $u \otimes v = z \otimes w$. Let $B_U = \{u_i \mid i \in I\}$ be a basis of $U$, $B_V = \{v_i \mid i \in I'\}$ a basis of $V$, then $B_W = \{\varphi(v_i) \mid i \in I'\}$ is a basis of $W$ since $\varphi$ is injective and so maps a basis to another basis.
Now, $$u \otimes \varphi(v) = \dots = \sum_{i \in I, j \in I'}s_i \ell_j (v_i \otimes \varphi(v_j)) = z \otimes \varphi(w) = \dots = \sum_{i \in I, j \in I'}s_i' \ell_j'(v_i \otimes \varphi(v_j)).$$ Now, comparing coefficients, we get $s_i\ell_j = s_i'\ell_j'$ and thus $u \otimes v = z \otimes w$.
> The one-point compactification is usually applied to a non-compact locally compact Hausdorff space. In the more general situation, it may not really be a compactification and hence is called the one-point extension or Alexandroff extension.
this is from nlab, whetver for reasons of density of non-Hausdorffness
Does this look fine to you, @VladimirLysikov ?
21:38
math math math math math
i love math
If there wasn't math then what would there be
Existence only makes sense with math
 
2 hours later…
23:18
Might there be reason for my finding learning math from online and books as resources incredibly taxing?
23:32
learning math is always incredibly taxing

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