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12:01 AM
:(
I assume "here" does not refer to Math SE
Violence is not the answer, it's the question and the answer is "yes"
@BenSteffan I don't work at SE. :)
no, but being a mod is like a job something something
Hmm... every open cover has an open refinement of size $\leq \kappa$ iff every open cover has a subcover of size $\leq \kappa$
never thought about this
This also shows how paracompactness is closer to compactness than one thinks
Oh, this isn't related to my position on the disciplinary committee... This is related to my role as chair of the Instructional Council. Darn I actually have to organize this shindig... :( :( :(
12:20 AM
And if every open cover has a locally finite subcover, then say $(U_i)$ is an open cover, pick some non-empty $U_j$ and let $V_i = U_i\cup U_j$ then if we take a locally finite subcover of $(V_i)$ then at some $x\in U_j$ the local finiteness shows that the subcover needs to actually be finite. So this is actually the same as compactness
> Given a bounded function $f:[a,b]\to\mathbb R$, let $$H(x)=\lim_{\delta\to0}\sup_{|y-x|\leq\delta}f(y),\quad h(x)=\lim_{\delta\to0}\inf_{|y-x|\leq\delta}f(y).$$Show that $H(x)=h(x)$ iff $f$ is continuous at $x$.
This is an exercise from Folland's book in proving the Lebesgue criterion. I think I know a solution, but I'm more concerned about elementary things. Are $h,H$ both functions from $[a,b]$? Are they well-defined, i.e. how can we know the limits always exist?
I can't visualize the deeper meaning behind $h$ and $H$, what they represent or whatever.
@psie If $x\notin [a, b]$ then you would have to take supremum/infimum of the empty set at some point
The limit superior and inferior always exist (though either could be infinite).
the limits are well-defined basically because monotone sequences, but they could be limits in the extended real line
oh sorry, $f$ is bounded
@psie they should represent lower and upper semicontinuity
And you can always assume that delta is small enough to live in your interval (as long as you aren't sitting at an end point).
12:29 AM
ok
Oh! f is bounded. Easy peasy.
So the limits both exist. They are monotone as delta goes to zero, and bounded by the difference between the to and bottom of f(x).
$H = f$ should be equivalent to $f$ being upper continuous, and $h = f$ should be equivalent to $f$ being lower continuous
or, pointwise if we fix a point. And both imply that $f$ is continuous
@XanderHenderson I see how $\sup_{|y-x|\leq\delta}f(y)$ is a monotone decreasing function, and so the limit exists because...$f$ is bounded?
12:35 AM
Cool beans. Fava beans!
For any particular choice of $\delta$, then $\sup\{ f(y) : |x-y| < \delta\} < \sup\{ f(x) : x \in [a,b]\}$, and $f$ is bounded, so...
(My mixed notation is GOOD! GOOD, I TELL YOU!)
Also, someone else took a shot at Trump?!
 
1 hour later…
2:06 AM
Is there anywhere on the site where I would be able to have someone check my work for answers?
*mistakes
2:17 AM
@VulpesInculta only in this chat
this is not allowed on the q&a system
unless you specify an exact step which needs to be explained, see wiki for the solution-verification tag
 
6 hours later…
8:10 AM
Hello
8:33 AM
how do I prove the following identity: if $a,b>0$ and $0<p<1$, then $(a+b)^p \leq a^p +b^p$. My initial attempt was to use concavity of $x \mapsto x^p$, which gives us $tf(x)+(1-t)f(y) \leq f(tx+(1-t)y) \implies ta^p+(1-t)b^p \leq (ta+(1-t)b)^p$ but that seems dead end. Is there a substitution I can do in Holder or Minkowski inequality?
@nickbros123 divide both sides by $b$, consider $f(x) = x^p-(x+1)^p+1$
show that its increasing
8:49 AM
right, got it
9:10 AM
or writing $p=1-q$ for $q\in ]0,1[$ you have $(a+b)^p=a(a+b)^{-q}+b(a+b)^{-q}<aa^{-q}+bb^{-q}$
@SineoftheTime neat!
10:17 AM
Interesting that some people study black holes in 5 (or higher) dimensional space
@onepotatotwopotato 4-space is hard :(
well at least 4-manifolds are f'ed up
I'm not sure how high-dimensional study helps the understanding of black holes in dim 4
you could hope that the things you learn in higher dimensions somehow generalize down
if you can develop a solid theory of thing in high(er) dimensions you can then study the question of how the theory translates to lower dimensions (and how much of it)
something like that, maybe
I don't know any single example that kind of "generalization" actually worked
10:34 AM
it's not my area of study, so my knowledge is rather limited, but something like $h$-cobordism comes to mind
the topological versions of it that hold in low dimensions, as opposed to the smooth one that only holds in dimensions $\geq 6$ (was it $\geq 5$?)
that's mathematics of course, not physics
the $h$-cobordism theorem was first proved in the smooth setting, and because it's so powerful people thought about how to prove analogues in lower dimensions, and actually succeeded (asterisks apply)
proof techniques for showing that there exist manifolds without smooth structures, and manifolds with more than one smooth structure were also pioneered in dimension 7 and above by Milnor and then studied and transferred downwards
10:48 AM
Hmm. If that black hole paper I mentioned above actually is for the understanding of 4 dimensions, it sounds convincing but I don't know if that's the case.
That $h$-cobordism, as far as I know is for higher dimensional Poincare conjecture. But regardless of that, it feels to me that $h$-cobordism is for high dimensions and people try to generalize to lower dimensions after knowing the usefulness of that. The main target or purpose of that theory is not for the understanding of the lower dimensional manifold.
The $h$-cobordism is not just for the Poincare conjecture
It's very, very useful
people initially started out trying to prove it in all dimensions, but the proof that emerged only works in dimensions $\geq 6$
The point is the last sentence.
yes, but I'm not done
people then thought about how to generalize downwards, because it is so useful
this lead to some results in lower dimensions, even though the conjecture in the smooth category is not true below that dimension
but the point really is that it provides precedent for studying things in higher dimensions
studying thing in large dimensions with the hope of being able to later study how eventual results transfer down is a valid strategy
whether this was the goal or not of the people studying $h$-cobordism initially is irrelevant
all that's important is that this pattern worked, and one can try to emulate it
whether you can justify this approach or not sufficiently or not is ultimately something for the people reading your grant proposal to decide :)
 
1 hour later…
12:23 PM
Hi. I have a statement in mind that goes like "A matrix A (not necessarily square) has linearly independent columns iff A^T A is non-singular". This seems to be wrong, but does someone here recognize it and can tell me what the correct statement is?
12:54 PM
@Bubaya Why do you think this is wrong?
@SoumikMukherjee Because with A = (1 \\ i), we get det (A^T A) = 0
is your $A$ supposed to be diagonal? that seems like a wrong computation
@Thorgott No, A is the 2 x 1-matrix with the single column (1 \\ i).
ah, of course
This is a non-zero matrix, so (because it has only one column), it has lin. indep. columns.
1:01 PM
I suspect you're forgetting to conjugate when transposing here
Mad
Mad
Is there a short course introduction for Differential geometry for physicists?
like 100 pages or less
Ted's book?
@Thorgott Oh, sure. That was stupid. Which raises the question: how to see that the statement (with conjugation) is true?
Or, say, how do I know there's no other field for which I have to do some other operation?
Mad
Mad
@SineoftheTime is it suited for physicsts tho?
dunno, try to see the topics in the index
1:13 PM
@onepotatotwopotato Even in Newtonian physics, it can be instructive to analyze orbits in a higher dimensional space, and with a different parameterization of time. From John Baez's blog, johncarlosbaez.wordpress.com/2015/03/17/…
> You probably [know] that planets go around the sun in elliptical orbits. But do you know why?

In fact, they’re moving in circles in 4 dimensions. But when these circles are projected down to 3-dimensional space, they become ellipses!
@Bubaya The statement is not true for finite fields
@SoumikMukherjee Do you know where it holds? Only char = 0?
2
A: Why is $A^TA$ invertible if $A$ has independent columns?

V. MikaelianI think it need be mentioned that we deal with the real field, as the mentioned both facts may not be true for arbitrary field $F$. Example 1. Let $F=\mathbb Z_5$ and $A=\left[\begin{smallmatrix} 1 & 3\\ 2 & 1\\ 0 & 1 \end{smallmatrix}\right]$. Then $A$ has two independent columns, but $A^T A=\l...

@Bubaya it's true for reals, and for complex I think you have to take the adjoint
@SoumikMukherjee Thank you very much for the link; that helps. Do you know of any "similar" statement that works over arbitrary fields?
Of course, with additional hypotheses then and/or weaker statements.
@Bubaya No, I don't know any
1:29 PM
OK, thank you.
@PM2Ring Oh, hey! That dude! He was on my PhD committee!
1:44 PM
@XanderHenderson Wow! He's currently in Edinburgh, living in Maxwell's house.
1:55 PM
There's two ingredients, best highlighted from a multi-linear perspective. If we do this in a coordinate-free manner, the question is when $m$ vectors $v_1,\dotsc,v_m$ in an $n$-dimensional vector space $V$ over a field $F$ are linearly independent. This is the case if and only if the element $v_1\land\dots\land v_m\neq0$ in the $m$-th exterior power of $V$.
Now, if $\langle-,-\rangle$ is a bilinear form on $V$, then $(v_1\land\dotsc\land v_k,w_1\land\dotsc\land w_k)\mapsto\det(\langle v_i,w_j\rangle)_{i,j}$ induces a bilinear form on $\Lambda^kV$. The result of pairing $v_1\land\dots\land
If you replace "bilinear" with "sesquilinear" and "symmetric" with "conjugate-symmetric", you obtain the complex-flavored version.
@PM2Ring Good for him.
oh, I forgot to mention that the Gramian determinant is the same thing as the determinant of $A^TA$ if you take orthonormal coordinates because transposing the matrix corresponds to taking the adjoint
I like to read his Mastodon feed from time to time. mathstodon.xyz/@johncarlosbaez
@XanderHenderson good to have such prominent mathematicians as That Guy on your PhD committee
That D. Guy
@PM2Ring John baez was what I used to dream of becoming- a physicist and a mathematician:)
2:12 PM
He was also one of the inventors of blogging. Back in the day of Usenet, he had a regular post named This Week's Finds in Mathematical Physics, which combined technical info with a little bit of personal info. math.ucr.edu/home/baez/TWF.html
He's a Stack Exchange member, but doesn't post very often.
3:03 PM
@PM2Ring Honestly, I applied to the PhD program at UCR in large part because of his earlier work in math/physics. Then I got there and found out that he was mostly working in category theory, which I don't find to be all that interesting. I attended his seminar for a couple of semester, and got a fair amount out of it (I think), but ultimately ended up working with Michel (the other person I applied to UCR to potentially work with).
John is an extremely charismatic lecturer---I really enjoyed his seminars---but... category theory. Ew. X(
:P
Mad
Mad
how would one go around calculating the sigma algebra of $ $ $ E_n \subset \mathcal{P}(\mathbb{N}) $ with
$ E_n :=({2},{4}...,{2n}) $
what do you think the algebra should be? :)
Mad
Mad
I managed to find the ring
$ R(E_n):= \mathcal{P}(E_n)$
And the Sigma Ring is equal to it.
When i start taking compliments, i get confused.
my guess is $A(E_n ):= \mathcal{P}(\mathbb{N})$
But i can not seem to replicate the set containing {1} so it can not be P(N)
3:21 PM
@XanderHenderson Fair enough. I get why some people are excited by category theory, but it definitely doesn't inspire me.
Mad
Mad
Def tho $ N, N\{2k}, N\{2,4,...} $ and so on are in the Algebra for sure.
@BenSteffan hmm... anything that deals with multiplication or generalization of such, and talking about things relating to it. So for example topological vector spaces wouldn't talk about operations or things relating to it so its not algebra, but linear algebra would
haha
since I said "the" algebra clearly we're talking about universal algebra :^)
Mad
Mad
@BenSteffan i do not know that term, i know tho the Generated algebra, which is what i am searching for
universal algebra is a field of study
but yeah, as you essentially note, you can isolate even numbers, i.e. $\{2n\} \in E_n$ for all $n > 0$. Can you get a set that doesn't contain all odd numbers?
Mad
Mad
3:30 PM
n is finite. so it is not all even numbers.
wdym
oh, I might have misunderstood the problem, nvm
Mad
Mad
the set $ E_n$ extends to some n, lets say $n=2$ so $E_2:=\{\{2\}\{4\}\}$
so you have in the generated algebra $ N\setminus 2, N\setminus 4, N\setminus {2,4}$
Also you have $ N, \emptyset $. But for example you do not (seem to atleast)
get $\{1\}$
uhh
I don't think you get $N \setminus \{2\}$ or $N \setminus \{4\}$
Mad
Mad
But the ring as i mentioned (maybe i got it wrong) contains $\{2\}$ the compliment would be that?
about the ring thing I have no idea, but you start out with $\emptyset, \mathbb{N}, \{2, 4\}$
(also please be a bit more careful with notation)
what else can you get? $\mathbb{N} \setminus \{2, 4\}$
That's all.
Mad
Mad
3:36 PM
Sorry i might have wrote it badly
$E_n$ contains singletons...
Ah, okay
So you start out with $\emptyset, \mathbb{N}, \{2\}, \{4\}$, gotcha
Mad
Mad
No you start with only the set containing 2 and four.
when you build the generated ring of those, you eventually get the empty set. i am not sure where you get N from?
Mad
Mad
Your inital set is :
$E_n := \{\{2\}, \cdots \{2n\} \}$
You're trying to a calculate a sigma algebra on $\mathbb{N}$. This is given as a family of subsets of $\mathbb{N}$
$\emptyset$ and $\mathbb{N}$ you always get for free
2 mins ago, by Ben Steffan
So you start out with $\emptyset, \mathbb{N}, \{2\}, \{4\}$, gotcha
so this is correct
Mad
Mad
3:39 PM
I understand what you are saying, i was trying to be more methodical and calculate the ring, sigma ring, the algebra, then the sigma algebra.
You jumped to the sigma algebra. which is ok!
oh, is that the distinction?
Mad
Mad
No i am just trying to be more methodical. But let us continue! Yes you start with those in the sigma Algebra.
so you start out as above, and take all possible unions; this gives you $\{2, 4\}$ as an additional set
what about complements? well, that's easy
you get $\mathbb{N}$ sans $\{2\}$, $\{4\}$, and $\{2, 4\}$, respectively
Mad
Mad
Yes and the whole set minus these elements or sets respectively.
@Mad that doesn't give a set we don't have already
Mad
Mad
3:45 PM
The compliments of $\{2\} \cdots$ and so on...
that is in fact what I wrote
when I wrote $\mathbb{N}$ sans ...
at least what I meant :)
Mad
Mad
i am not sure what SANS means lol
"without"
Mad
Mad
Oh ok.
anyways, that's all
there's no more sets we can form
Mad
Mad
3:46 PM
Interesting. so you do not get the power set.
Thanks!
you're welcome :)
4:02 PM
If $(X,A)$ is space , $A$ closed in $X$, such that for some $U$ open in $X$, with $A\subseteq U$, $(U,A)$ is an NDR pair, does it follow that $(X,A)$ is an NDR pair?
@monoidaltransform If $X$ is normal, then I think so
How to show this?
4:17 PM
I didn't say that is true, but that it might be true if $X$ is normal
my intuition tells me that normality and tube lemma might be important
yeah, this should be false in general
Im wondering if $X$ is metric
if this holds
what, as a consequence?
Mad
Mad
@BenSteffan
in this post, they have a similiar problem
https://math.stackexchange.com/questions/1248973/of-which-sets-does-the-sigma-algebra-generated-by-the-first-n-singletons-of?rq=1

if we apply his argument to our case, we would have
$A_\sigma (E_2 )= P(\{2\}) \cup P^c(\{2\}$
But $P^c(\{2\}= P(N\setminus \{2\})$
And that would contain elements like $\{1\}$
Which we shown to not be part of it.
If $(X,A)$ pair, $X$ metric, $A$ closed, $A\subseteq U$, $U$ open, if $(U,A)$ NDR is $(X,A)$ NDR?
4:25 PM
@Mad no, read the definition of $P^c$ again.
it's not the powerset of the complement
Mad
Mad
@BenSteffan Ahh i see! i missed that!
the calculation in the post agrees with what I did above :)
Anyone willing to help me with some trigonometry I am working on? One question I am having some trouble with & a few others I am not overly confident in my answers.
Mad
Mad
@BenSteffan can you also help me understand this short proof, while we are still on the subject?
https://math.stackexchange.com/questions/1978907/about-the-sigma-algebra-generated-by-n-first-integers?rq=1

in this question, they look at the sigma algebra generated by the first n elements.

i understand the authors idea, but the Answer is confusing me. i am not sure how it follows from that, that the union is not a sigma algebra
It took me a while to parse what's going on, too :)
What the answer is showing is that the infinite sets $\mathcal{A}_k$ are of the form stated in the question
so complements of finite sets
4:39 PM
@monoidaltransform If $U$ is a 'halo' around $A$, i.e. there is a continuous function $\tau\colon X\rightarrow[0,1]$ s.t. $\tau\vert_A=0$ and $\tau\vert_{X-U}=0$, then $(U,A)$ is an NDR-pair iff $(X,A)$ is an NDR-pair. This neither requires you to assume that $A$ is closed or $U$ is open, but if you do assume those, then $U$ being a halo around $A$ is automatic as soon as $X$ is a normal space, as Jakobian intuited.
you can do this by observing that you know sigma algebras $\mathcal{B}_k$ containing the $\mathcal{A}_k$ for which this observation is true
@Thorgott doesn't $\tau \equiv 0$ work?
should one of those restrictions be $1$?
ah, typo, it should be $\tau\vert_A=1$
thanks @Thorgott !
ill try to prove this
and then the idea from the question goes through. $2\mathbb{N}$ is an infinite set that is not the complement of a finite subset of $\mathbb{N}$, and if $\bigcup_k \mathcal{A}_k$ was a sigma algebra then it would need to contain $2\mathbb{N}$ (in fact, the smallest sigma algebra containing all the $\mathcal{A}_k$ is $\mathcal{P}(\mathbb{N})$ since it contains all singletons), contradiction.
4:55 PM
@Thorgott how do you extend the homotopy to all of $X$?
I have a 2 part question where I need to find the number of solutions of an SSA triangle. Then in the next step determine the measure(s) of angle B. i am given side a, side b, & angle A. Would the measure(s) of angle B not have to be determined to find the number of solutions?
Mad
Mad
@BenSteffan and why would this be a contradiction?
@Thorgott $H'(x,t)=H(x,t\tau(x))$?
see what I wrote a few messages below that
Mad
Mad
5:13 PM
@BenSteffan i see!
@monoidaltransform Its not so clear to me if you can give an explicit argument
Mad
Mad
@BenSteffan do you have a hint on why it needs to contain the 2N?
@BenSteffan oh because it is an infinite union.
ah wait, you can
recall that a closed subspace $A$ of a space $X$ is cofibered in $X$ iff there is a continuous function $\varphi\colon X\rightarrow I$ s.t. $A=\varphi^{-1}(0)$ and $A$ is an ambient deformation retract of $\varphi^{-1}([0,1))$
so in the previous scenario, let $\tau\colon X\rightarrow I$ witness $U$ as a halo of $A$ and $\varphi\colon U\rightarrow I$ witness $A$ as cofibered in $U$, then $\psi\colon=\max(1-\tau,\varphi)\colon X\rightarrow I$ is continuous and witnesses $A$ as cofibered in $X$
5:37 PM
In terms of the homotopy $H:U\times I\rightarrow U$ rel $A$, where $A=\phi^{-1}(0)$, how is the extended $H$ related to $\psi$?
@Thorgott
@Mad yeah, if you have all singletons then you have all sets since $\mathbb{N}$ is countable, and sigma algebras are closed under countable unions
Mad
Mad
@BenSteffan Yea! i can make the same argument for my case.
My brain has a hard time accepting this proof, because the process of going to infinty messes me up.>
So in the countable union, you do have N or 2N in this case.
but then it needs to spesifically be part of one those sets, which is not.

somehow my brain rejects this proof. But whatever.
give it a good night's rest and come back to it tomorrow
that sometimes helps
Mad
Mad
Thats true, but honestly, the concept of going to infintity never computed in my brain.
But yet again, my brain has no obligation to be able to understand such concepts at all.
5:53 PM
@monoidaltransform there is no extension necessary, that is the point of my characterization
6:03 PM
when I say "ambient deformation retract" in my message, I mean a homotopy $\varphi^{-1}([0,1))\times I\rightarrow X$ rel $A$ from the inclusion to a retraction onto $A$
the way you construct from that in turn a homotopy as in the definition of an NDR-pair is by piecewise-linearly reparametrizing the second coordinate so that the homotopy is unchanged for points with small $\phi$-value and constant the identity for points with large $\phi$-value
 
3 hours later…
8:41 PM
I have a problem: "Prove rigorously that $\bigcap\limits_{n=1}^{\infty}(0,1/n)=\varnothing.$ Hint: Use the Archimedean property." But I don't see why I'd need the archimedean property for this proof
oh nvm, I think I'm interpreting this wrong. I thought this was the nested interval property which is the same thing but with closed intervals (and this intersection is nonempty)
we just used axiom of completeness to prove that
8:59 PM
this is essentially the definition of the Archimedean property
Yeah. But if you write it in an equivalent form
for fields that is
there exists rings which obey Archimedean property but this intersection is non-empty
wait.. I accidentally proved it's nonempty
I'm sure it's logically flawed somehow though
it better be
:-)
Recall: The Archimedean property states that for all $\epsilon\in K$, $\exists n \in \mathbb{N}$ such that $n>\epsilon$ ($\mathbb{N}$ is unbounded). It also states that $\forall \epsilon\in K,\exists n \in \mathbb{N}$, $\epsilon>0 \implies \epsilon>\frac{1}{n}$ (rational numbers are dense in $\mathbb{R}$).
Begin proof: Let $K = \bigcap\limits_{n=1}^{\infty}(0,\frac{1}{n})$. We will use induction to prove $K$ is nonempty for all $n \in \mathbb{N}$.
stop stop stop
9:10 PM
ok
there's nothing to induct over!
$K$ does not depend on $n$
so "$K$ is nonempty for all $n \in \mathbb{N}$" does not parse
I suppose you could interpret it as $\mathbb{N}$ being unbounded, but you can also interpret it as $\mathbb{N}$ being cofinal
oh
I don't know why $K$ suddenly became the intersection. I thought $K$ was the field?
if this were $K = \bigcap\limits_{n=1}^N(0,\frac{1}{n})$ then I could use induction?
9:12 PM
yes, you could use induction on $N$
and this $K_N$ would in fact be non-empty for all $N$
@Jakobian yes, I should use a different letter for that intersection.
@BenSteffan that's...strange to me but oh well.
is it?
in fact, $K_N = (0, 1/N)$
The negation of "there exists $n$ with $x > 1/n$" is that "for all $n$ we have $x\leq 1/n$"
think about it: an element of an intersection is an element that is in each of the sets you're taking the intersection over
oh I see, I think you should write $K_n$ instead of $K_N$ because in my mind $N \subseteq \mathbb{N}$ which could be $\mathbb{N}$ itself
9:16 PM
An element in $K$ would have to be $\leq 1/n$ for every natural $n$, but we know there exists a natural with $x > 1/n$
I think this notation is good exercise for your mental flexibility :-)
also you were the one to suggest $N$, I just put it in the subscript
In any case, you can't have $n$ as it's written right now, because that's already the index variable in the intersection
you could have $K_k = \bigcap_{n = 1}^k (0, 1/n)$, say, or $K_n = \bigcap_{k = 1}^n (0, 1/k)$
but it's all tomato tomato
@Jakobian This is not true for some $x \in \mathbb{R}$ though. For example, $x = 2$, then $2\leq 1/1$ is not true.
oh nvm
"for every"
you have to swap the quantifiers on $x$ too so we get $\neg\forall x \to \exists x$
@jakobian is this right: $$\neg\left(\forall \epsilon\in\mathbb{R},\exists n\in\mathbb{N}\left(\epsilon>0\implies\frac{1}{n}<\epsilon\right)\right)=\exists\epsilon\in\mathbb{R},\forall n\in\mathbb{N}\left(\epsilon<0\implies\frac{1}{n}\geq \epsilon\right)$$
for negation of archimedean property
I should probably keep inequalities pointing in the same direction oh well
gotta run now, bbl
 
1 hour later…
10:45 PM
I'm quoting Folland:
> For example, if $f$ is Riemann integrable on $[0,b]$ for all $b>0$ and Lebesgue integrable on $[0,\infty)$, then $\int_{[0,\infty)}f\,dm=\lim_{b\to\infty}\int_0^b f(x)\,dx$ (by the dominated convergence theorem), but the limit on the right can exist even when $f$ is not integrable (Example: $f=\sum_1^\infty n^{-1}(-1)^n\chi_{(n,n+1]}$.)
Here $m$ is Lebesgue measure and $dx$ denotes Riemann integral. I don't see how $\int_{[0,\infty)}f\,dm=\lim_{b\to\infty}\int_0^b f(x)\,dx$ follows from DCT. Moreover, why is the infinite sum not integrable?
In DCT, we have a sequence, but I don't see any sequence in $\lim_{b\to\infty}\int_0^b f(x)\,dx$.
Ah, ok, I think I understand my first trouble.
$$\int_{[0, \infty)} f \,dm= \lim_{c \to \infty} \int_{[0,\infty)} f \chi_{[0,c]}\,dm = \lim_{c \to \infty}\int_{[0,c]} f \,dm= \lim_{c \to \infty}\int_0^cf(x) \, dx = \int_0^\infty f(x) \, dx.$$
As for $f=\sum_1^\infty n^{-1}(-1)^n\chi_{(n,n+1]}$, my brain's a bit slow today, but is the integral of this function simply $0$?
I don't understand what he means by "...the limit on the right can exist even when $f$ is not integrable."
$\int_{[0, \infty)} f^+ dm$ essentially computes the harmonic series I think?
same for $f^-$
because $\int_{(n, n + 1]} n^{-1} (-1)^n d m = (-1)^n/n$
so $\int_{[0, \infty)} f^+ dm = \infty = \int_{[0, \infty)} f^- dm$ and the lebesgue integral fails to materialize
but the limit on the r.h.s computes $\sum_{i = 0}^\infty (-1)/n = \ln(2)$
11:04 PM
@BenSteffan ok, makes sense, thanks. I still do not quite see what $\int_0^b f(x)\,dx$ evaluates to under the $f$ specified. Is it simply $\sum_1^b (-1)^n/n$?
if $b$ is an integer, yeah
you can split the integral up into $\int_0^1 f(x) dx + \int_1^2 f(x) dx + \ldots + \int_{b - 1}^b f(x) dx$
which gives $\int_1^2 (-1) dx + \int_2^3 1/2 dx + \ldots + \int_{b - 1}^b (-1)^{b - 1} / (b - 1) dx$
and you're integrating constants over intervals of length 1 so you get exactly the sum you wrote, save for the fact it should end at $b - 1$
ah ok 👍
11:29 PM
@BenSteffan did you know that the harmonic series converges if you remove every number with a digit $9$ in it? :) Here we are not really getting the harmonic series, but a subseries. I still think it diverges, but I'm always cautious due to this fact.
oh that's fun, I didn't know that
yeah here you're essentially looking at $\sum_{n = 1}^\infty 1 / (2n)$ for $f^+$, and this diverges since you can just pull the $1 / 2$ out and get the harmonic series, and similar for the negative part
yeah 👍
11:59 PM
@psie You want to check for $\int |f|$. Then its clear this is just $\sum n^{-1}$

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