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12:09 AM
if f(c,b)=y(c) is true for all c, then y(a)=y(c)
(not sure where you'd be getting y(b) from)
 
hmm
for what region of $\mathbb{C}$ does the following series converge $- \sum_{n=1}^{\infty} \dfrac{\sin(nz)}{2^n}$
im getting that the region is $|z| < 2$
 
absolute convergence?
 
oh and the question asks $-$ compute the the sum of the series to give an explicit expression for the analytic function
 
Regardless, that can't be right: When $z=\pi$, that collapses to being identically zero
 
schwizles
yes, absolute convergence
hm, how do i attack this problem
 
12:16 AM
Hint: Euler's formula.
 
but euler's formula takes a real number $x$
 
What?
 
Euler $-$
 
By Euler, I mean $e^{i \theta}=\cos\theta+i\sin \theta$
 
for a real number $x\in\mathbb{R}, e^{ix} = \cos(x) + i\sin(x)$
that's De Moivre's formula
 
12:20 AM
It's still valid if $x$ is complex.
 
but De Moivre's formula takes in the argument of a complex number $\arg(z) =: \theta$
 
Well, how are you defining $\sin z$ for complex z?
If you're doing so as a series, then the usual proof of Euler's formula via Taylor series is still valid.
 
$\sin z = \dfrac{e^{iz}-e^{-iz}}{2i}$
 
Ok. And similarly for cos(z), I presume
 
yeah
 
12:23 AM
in which case $\cos z+i \sin z=e^{iz}$ is true by that definition
 
sweet
lets verify
 
In any case, though, it's just as useful to use the definition you just stated in this problem
At least, for explicitly summing the series it is
 
ok. so i did that
it would stand to reason that the valid region is all of $\mathbb{C}$
since $|\sin z| \le 1$
 
That's only valid for real $z$.
 
ok
 
12:25 AM
For imaginary z, that passes over to the sinh function
 
what passes over?
the inequality?
so $|\sinh z| \le 1$?
 
sin(z)=-i sinh(iz)
 
in any event, i plug that identity in
 
so when z=iy is purely imaginary, you get -i sinh(-y)=sinh(y)
and sinh grows without bound as y->infty
so the inequality $|\sin z|\leq 1$ cannot be valid in the entire complex plane
What I'd consider is $|\sin z|^2=\sin(x+I y)\sin(x-I y)$ and use Euler's formula to express that entirely in terms of real functions
 
$\sum_{n=1}^{\infty} \dfrac{\sin nz}{s^n} = \sum_{n=1}^{\infty} \dfrac{e^{inz}-e^{-inz}}{i \cdot 2^{n+1}} = \sum_{n=1}^{\infty} \dfrac{1}{i \cdot 2^{n+1}}[e^{inz}-e^{-inz}]$
 
12:28 AM
yep. At that point it's useful to split the series in two
\cdot, maybe?
For instance, can you compute $\sum_{n=1}^\infty e^{i n z}/2^n$ ?
That's a good deal less painful to deal with
 
and and that point ^ im stuck
 
How about if you write that as $\sum_{n=1}^\infty (e^{iz}/2)^n$?
See if you can remember anything about series of that form.
(back in a bit)
 
geometric series
 
12:44 AM
hm, so perhaps the region is $-\ln2 < |iz| < \ln2$
and the sum evaluates to $\dfrac{1}{2i} \Bigg[\dfrac{1}{1-\dfrac{e^{iz}}{2}}-\dfrac{1}{1-\dfrac{e^{-iz}}{2}}\Bigg]$
 
Second looks right. But for the first, you’d have z=pi lying outside that region
 
hrmp
i get $|e^{iz}| < 2$
 
more generally, the series should vanish term-by-term for any multiple of pi
 
true. can i get more specific than $|e^{iz}| < 2$? take $\ln$ of both sides?
 
Sure. But that equals |e^x e^(iy)|
 
12:50 AM
yeah, more specific than that?
 
how?
taking $\ln$ of both sides doesn't work (?)
 
Well, x and y are real. So what can you say about e^(i y)
 
complex
 
What about it’s modulus?
 
12:52 AM
drawing blanks
 
So you don’t know the absolute value of e^(i pi/3)? (Picking an arbitrary example)
 
oh
its $1$
by Euler, and then Pythagoras
 
Right. That applies to any $e^{iy}$ with $y$ real.
Alternatively, you've got $|e^{iz}|^2=e^{iz}e^{-i \overline{z}}=e^{-2y}$
 
right
 
Oh. I wrote |e^x e^(i y)|=|e^z| earlier when it should have been |e^(ix)e^(-y)|=|e^(iz)|
same idea, but slightly different algebra
So what does that inequality become?
 
12:59 AM
yes yes
 
is it unwise to concentrate in abstract algebra for a math PhD?
 
ok good. that bothered me acutally
 
seems so many people pick applied topics for their PhD these days
 
drumroll
The region is $-2 < \ln\Im{z} < 2$
 
still not right :(
that'd be e^(-2) < Im(z)<e^2
but both of those are positive, i.e. you'd be talking about a region of positive imaginary part
which again would exclude real z
 
1:04 AM
$|e^{-y}| < 2$ for ${y\in \mathbb{R}}$
specifies the region right?
 
Right. But $e^{-y}$ is positive for all real y
so you can drop the absolute value sign
 
yes
and we get $y > -\ln 2$
 
Yep. So the imaginary part must be larger than -ln(2)
That definitely includes all real z, so it passes that check
 
:)
thanks
 
Hmm, though
The region we get this way isn't symmetric across the real line
 
1:07 AM
what do you mean
 
Suppose $\sum_{n=1}^\infty \frac{\sin n z}{2^n}$ converges. What can we say about $\sum_{n=1}^\infty \frac{\sin n\overline{z}}{2^n}$?
 
ought to converge as well
 
Right. So the region in which the series converges out to be symmetric across the real line
since otherwise you'd have z for which the series would converge but not z-bar
 
im not following what you mean by symmetric across the real line?
for real z, z = z-bar
 
Draw the region in the complex plane. Is the real line a line of symmetry?
 
1:11 AM
no
ohh
 
Yeah
I think the resolution is simple, though. the requirement that |e^(iz)/2|<1 is the condition for $\sum_{n=1}^\infty (e^{iz}/2)^n$ to converge
 
right
 
But you actually had two series. The second was $\sum_{n=1}^\infty (e^{-i z}/2)^n$. What's the condition for that to converge?
(It's not quite the same!)
 
$y < \ln 2$
 
Yep. So between the two you get $-\ln 2 <y <\ln 2$
 
1:15 AM
yes
which is why i had $-2 < \ln\Im{z} < 2$ except my $\ln$'s were misplaced
 
Ah.
In any case, I think that's the final correct domain of convergence
 
looks good. thanks again!
 
Hi
For solving proofs, in general, (started proofs now), is getting to a solution more on based on doing many different proofs and luck, or...?
 
1:51 AM
@Strikers both luck and practice -- maybe practice on how to use the given assumptions
 
2:03 AM
there are two solutions to $e^{1/lnx}=x$ the solutions are: $x=e$ and $x=1/e$
 
those are the two positive real solutions, at any rate
 
what is pythagoras's constant?
ohh
it's $\sqrt{2}$
 
2:26 AM
what kind of number is $e^{-\sqrt{2}}$
 
 
2 hours later…
4:05 AM
One of those that are less than < 1/2
 
 
1 hour later…
5:11 AM
4
Q: Uncountable orderings

Jacopo BelboLet $P$ be an uncountable linear ordering. Is it true that either $P$ contains an order-copy of $\omega_1$ or there is $x_0\in P$ such that there exist uncountably many distinct $y\in P$ with $y< x_0$? If so, where can I find a reference for this? Thank you.

This link provide an example of constructing a singular $\omega_1$ in ZF
 
6:05 AM
[Random]
a is 0, a is positive, a is negative, a is fractional, a is decimal, a is continuous, a is undefined, a is unknown, a is ill defined
 
6:31 AM
@Semiclassical thank you. I mistyped and wrote y(b) instead of y(a).
 
7:03 AM
Is anyone familiar with abstract algebra / groups here
If I take product of two normal groups is the result group abelian?
 
7:14 AM
@PiyushDivyanakar Well, a group can't be normal by itself, it's only normal as a subgroup of another group.
But if you take the product of two abelian groups, the result will indeed be abelian. You should check this yourself; i.e. compute $(g_1, h_1) \cdot (g_2, h_2)$ and compare it with $(g_2, h_2) \cdot (g_1,h_1)$, keeping in mind that each group is abelian by itself.
 
hi @Gargle
 
ouch
 
digaonal is normal iff group is abelian right
 
7:31 AM
Yeah. In particular, for any $g,h \in G$, $(g,1)(h,h)(g^{-1}, 1) = (k,k)$ for some $k \in G$, so that $ghg^{-1} = k = h$.
 
7:42 AM
@Fargle let me rephrase that. If we have H,K as normal subgroups of G then is the product set HK which is pairwise product of all elements in H and K. Then is HK abelian.
 
Oh, that's my bad, I misread you.
I think that's false: if you let $H$ be the subgroup of the quaternion group generated by i, and $K$ the subgroup generated by j, then $HK = G$, but the group is nonabelian.
 
@Fargle no that's not your bad
he clearly said "normal group" instead of "normal subgroup"
 
1
Q: Why is the group G a normal subgroup of itself?

usainlightningApparently $g^{-1}Gg=G$ for all $g$ in $G$. I understand that by closure if you multiply on the right by $g$ and the left by $g^{-1}$ you will get an element of the group $G$. However, how do i know that some of the elements of $g^{-1}Gg$ will not be duplicate and hence I will not be able to gene...

"self normal subgroup"
 
8:12 AM
@Fargle thanks I am getting it now.
 
 
1 hour later…
9:20 AM
[Random]
How big is the leap between 0 and 1
Given any definable function $f$, $f(\varnothing)=\varnothing$ always
 
@Secret 1-0=1
 
so that means 1 is effectively inaccessible from 0 (because to even get to 1 we need 1 itself)
yet $\mathcal{P}(\varnothing) = \{\varnothing\} = 1$
so somehow powersets (in the absence of inaccessibles) can reach a higher hierarchy of numbers from below
Is it even possible to have $1$ if we don't have:
Axiom of infinity
Axiom of pairing
Axiom of power set
?
In fact, one can argue the gap between $0$ and $1$ is much much bigger than the gap between any two infinite cardinals (however big they are). This is because for any cardinal $\kappa$, $0\kappa = 0$ and since cardinals are initial ordinals, it follows this is actually a well ordered sum of zeros which gets nowhere other than zero itself.
 
 
1 hour later…
11:12 AM
Therefore, one important observation that the zero ordinal is the lowest level of the hierarchy of "unreachable" quantities is the following:
> Any sequence formed by the arithmetic combination of zeros will always be the zero sequence, hence converging to zero for any topology $\tau$
So the zero ordinal is special. It is not an unreachable thing like anything else higher up, but it is "very hard to escape from"
The zero ordinal, in fact, is the opposite of any limit ordinal: It is something that everything will eventually converge to, give enough time for things to wander around in the class of ordinals
 
12:00 PM
0
Q: Doubt on Theorem 4.4.4 (Tutte [181]; Nash-Williams [145])

Math geek I understood that $T$ is one of the spanning trees which has disjoint edges compared to other $k-1$ edges. then, $T$ has $|V(G)|-1$ edges. What does the author say in the underlined statement? Isn't it a trivial thing?we know that $|\mathscr P-1|\leq|V(G)|-1$. Is it follow from this inequality...

please help me to find the converse
 
 
2 hours later…
1:33 PM
Problem: If $b \neq 0$ and $b_n \to b$, then $b_n \neq 0$ except for possibly a finite number of integers $n$. I discovered a simpler solution but I just want to verify that my original one is correct. If am not mistaken, the contrapositive states "If for every finite set $F$ in $\Bbb{N}$ there is some $n \notin F$ s.t. $b_n = 0$, then $b=0$."
With that in mind, assuming the hypothesis, there exists some $n_1 > 1$ such that $b_{n_1} = 0$. And given the finite $\{1,...,n_1\}$, there is some $n_2 > n_1$ such that $b_{n_2}=0$. From this we can inductively construct a subsequence $\{b_{n_k}\}$ such that $b_{n_k}=0$ for all $k \in \Bbb{N}$. Clearly $b_{n_k} \to 0$, so $b =0$, since the limit of the parent sequence must agree with the limit of any one of its subsequence.
Does this sound right? Did I get the contrapositive of the original statement right?
 
"The 3 groups of ppl most in conflict in israel are the Jews, the Arabs, and the Bus Drivers" - my sister
2
@user193319 Seems good
Yeah, you can't have infinitely many 'cause then you'd get an infinite subsequence of zeroes
Unrelatedly:
(I wonder if there's a book or article on the Riemann Hypothesis with the title "From Zeroes to Heroes")
 
@AkivaWeinberger Thanks!
 
1:50 PM
@AkivaWeinberger because people don't thank the bus drivers enough?
 
because the bus drivers have to thank each other
 
did you type that in 10 seconds
 
i'm ... pretty fast at typing?
 
No because they're just horrible
I JUST missed a bus three times in a row today
three separate busses
 
lol
 
1:52 PM
Oh also they changed the law on how you have to pay them
You can't use cash, you have to have a card, and there are very few places where you can actually refill the cards
It's annoying
Not like a credit card, a special card specifically for public transport
 
can you pay them by thanks?
 
cash, card, or fortnite
 
I do yell "Todah!" before stepping off but I think I'm the only one in the country who does this
 
why is cos(nx) n>=0 and sin(nx) for n>=1 a countable basis for continuous functions on [-1,1]?
 
I'm too Canadian American
 
1:56 PM
IME spending over a decade in a Catholic school also does this to you
 
'Cause Fourier? @LeakyNun
 
why does Fourier work?
 
Should really be an interval of length $2\pi$ or something
 
[-pi,pi] then
 
The proofs work a lot easier if you use $\{e^{inx}\}$ instead
and it's equivalent
 
1:59 PM
ok why does {e^inx} work?
 
But uh you find a formula that says, if it is a sum of the thingies, this formula gives you the coefficients. And then you can go the other way and prove the formula always gives you things that add up to the function
 
well I understand the first part because they're all orthogonal to each other
 
And if you use sin/cos then you need the formula for $\sum^N\sin nx$ or something
 
and int fg dx is just the inner product <f,g> in this Hilbert space
 
which makes me think if you use $e^{inx}$ you just need the geometric series which is easier
 
2:00 PM
i mean, $\sum \sin nx$ is just two copies of that, just a bit messier
 
I think you're just transforming my question into equivalent statements
 
I don't remember the details but work it out, if $f=\sum a_ne^{inx}$ for $n$ from $-\infty$ to $\infty$ then what's the formula for $a_n$?
 
multiply it by e^{-inx} and integrate
 
because they're orthogonal
it's like extracting a coefficient using the dot product
 
2:02 PM
So then define define $\bar f$ to be $\sum a_ne^{inx}$ where $a_n$ is defined by that formula, and then show $\bar f=f$
I honestly don't remember any more details on this
 
and that's my question...
 
Well, a good start would be to write out what $\bar f$ is
That's probably not the official notation or whatever
 
$\displaystyle \overline f = \frac1{2\pi} \sum_{n=-\infty}^\infty e^{inx} \int_{-\pi}^{\pi} f(z) e^{-inz} \ \mathrm dz$
 
Any way you can switch the integral and summation signs?
 
M?
 
2:05 PM
?
 
LDC?
Weierstrass M-test or Lebesgue Dominated Convergence
 
Uh probably
I don't remember
 
maybe @MikeMiller will know
 
$f$ is bounded anyway
'cause it's a continuous function on a compact interval
 
sure
 
2:06 PM
so that probably helps
 
ok...
 
I don't remember the criteria
 
@LeakyNun Do you understand why they are L^2 orthogonal?
 
yes
 
You need to show that the L^2 norm of \sum a_n sin(nx) decays as you start the sum from larger n
 
2:08 PM
Oh, am I over the Green Line right now?
I think I might be
 
You know those are orthogonal. So the L^2 norm is just the sum of a_n^2
 
I'll cross it again before I get off the bus
but right now I think I'm in the West Bank
 
The assumption that sum a_n^2 converges implies that the sum from N to infinity goes to 0 as N goes to infinity
(basically just definition of convergence of sums)
 
Yep, I am
 
@MikeMiller would it be easier to do with e^inx?
 
2:12 PM
The argument would be the same - the essential point is orthogonality
 
It would actually be incredibly easy for me to go into Ramallah at any point, just take the 218 bus
Obviously I'm not gonna do that, but I could
 
I would probably do that using the Fourier transform as it takes multiplication to convolution and vice versa
 
(Would probably not be a fun bus ride)
 
@MikeMiller and then?
 
Oh, a soldier with a huge gun just went inside briefly, I assume that means we crossed the border again
Yup
Also I missed my stop 'cause I was distracted by checking the map for that
 
2:19 PM
@LeakyNun I'm confused - the argument is finished. What do you mean?
 
you showed that the sum converges
I don't see why it would converge to the original function
 
Aha I now see what you mean
 
Like, if we removed an element from our list, it would no longer be a basis
but they would still all be orthogonal
 
Yes I got it :)
Gimme a minute to fix my thoughts
 
17 mins ago, by Leaky Nun
$\displaystyle \overline f = \frac1{2\pi} \sum_{n=-\infty}^\infty e^{inx} \int_{-\pi}^{\pi} f(z) e^{-inz} \ \mathrm dz$
Wait, so start here, swap the thingies
 
2:22 PM
The problem is that this is a nontrivial theorem and I was trying to prove it with trivial facts...
 
The $e$s combine to $e^{in(x-z)}$ and you're summing over $n$
 
The nontrivial input is Parseval's theorem, which says that Fourier transform preserves $L^2$ norm
 
that's not very non-trivial right, that's just swapping integrals and sums
let's assume we can swap them
 
I haven't thought about the proof of that theorem in a long time
So I will have to take your word of it
 
it's still only saying that the things are orthogonal
maybe orthonormal
 
2:25 PM
Wait, hold on, I'm confused again
because summing a geometric series from $-\infty$ to $\infty$ never makes sense
I guess you interpret it as the limit of the sum from $-N$ to $N$ as $N\to\infty$?
 
the coefficients are not geometric?
 
$e^{in(x-z)}$?
 
there is an integral term...
 
Yeah, we're swapping them
You know what
Let's think of the finite sum for now
Define $\bar f_N$ to be $\sum_{-N}^Na_ne^{inx}$ 'cause I forget the actual notation
 
OK I'm too far behind so I'm going to go do something else, sorry I wasn't much help. Deserves more thought than I remembered.
 
2:28 PM
And we just need $\bar f_N\to f$, and then we don't need to worry about weirdness involving swapping sums and integrals
 
ok
 
$\displaystyle \overline f_N = \frac1{2\pi} \sum_{n=-N}^N e^{inx} \int_{-\pi}^{\pi} f(z) e^{-inz} \ \mathrm dz$
$\displaystyle {}= \frac1{2\pi} \int_{-\pi}^\pi f(z) \sum_{n=-N}^N e^{in(x-z)} \ \mathrm dz$
 
this really shouldn't be that hard but i am utterly blanking lol
i've seen this proof so many times
 
I mean clearly the next step is to simplify that sum, no?
 
i know i said i was doing something else but then i got embarassed that i couldn't figure out why the standard basis of L^2 is a basis
 
2:36 PM
Get rid of the $\sum$
 
@AkivaWeinberger what are you going to do, turn it into dirac delta?
 
$\dfrac{e^{i(N+1)(x-z)}-e^{-iN(x-z)}}{e^{i(x-z)}-1}$, right?
Ugh, maybe doing the real version would have been simpler
What are the real and imaginary parts of that?
Or
 
I don't really think doing the real case would be simpler
anyway, the common ratio of the geometric series has norm 1 so it doesn't converge
 
What's $\left(e^{iN(x-z)}-1\right)\left(e^{-iN(x-z)}-1\right)$?
 
terrible
 
2:44 PM
I really feel some dirac delta business going on there
 
Never mind, doesn't equal what I thought it would
What's $\left(e^{i(N+1)(x-z)}-1\right)\left(e^{-iN(x-z)}-1\right)$?
 
@LeakyNun That's definitely what goes on in Parseval
 
Hm, the signs aren't right
 
@MikeMiller what's parseval's theorem?
 
The Fourier transform is an isometry $L^2 \to L^2$. One should be able to use this to then show that the Fourier series is an isometry $L^2 \to \ell^2$. Unfortunately I am a doofus and do not see how
 
2:46 PM
$\left(1+e^{i(N+1)(x-z)}\right)\left(1-e^{-iN(x-z)}\right)$?
 
Alternatively I am scrunched on a plane with 4h sleep so that's my excuse
 
Yeah that's what I want
 
maybe my notes stated a bogus version of Parseval
no that's the same as what wiki says
In mathematics, Parseval's theorem usually refers to the result that the Fourier transform is unitary; loosely, that the sum (or integral) of the square of a function is equal to the sum (or integral) of the square of its transform. It originates from a 1799 theorem about series by Marc-Antoine Parseval, which was later applied to the Fourier series. It is also known as Rayleigh's energy theorem, or Rayleigh's Identity, after John William Strutt, Lord Rayleigh.Although the term "Parseval's theorem" is often used to describe the unitarity of any Fourier transform, especially in physics, the most...
so is wiki's version also bogus?
 
$\displaystyle \frac{e^{i(N+1)(x-z)}-e^{-iN(x-z)}}{e^{i(x-z)}-1}=\\ 1+\frac{\left(1+e^{i(N+ 1)(x-z)}\right)\left(1-e^{-iN(x-z)}\right)}{e^{i(x-z)}-1}$
I think I made it worse
 
definitely not, I'm probably just misremembering names
Oh I see, your point is that it assumes the basis already
I am about 80% sure that the theorem is not supposed to assume that
No series in this just transforms
So still need to figure out why the map to $\ell^2$ is also an isometry
 
2:51 PM
@MikeMiller hey that's not discrete
 
If I parse correctly that's what I meant by my last two lines
thanks for your patience with me this morning lol
 
@MikeMiller indeed
so I now have one more equivalent statement
$\displaystyle \overline f = \frac1{2\pi} \sum_{n=-\infty}^\infty e^{inx} \int_{-\pi}^{\pi} f(z) e^{-inz} \ \mathrm dz$
so I guess the idea is that after you switch it, the terms become zero except around z=0 and when n=0
 
If a continious function is increasing from [a, b], does it mean it will also increase from (a, b)
 
3:08 PM
@GENESECT What is the definition of increasing function on a subset of R? Let's call the subset I for convenience (I stands for interval, but we don't need to restrict to intervals).
 
Okay.. I would say that if a, b €I and a<=b then f(a) <=f(b)
 
Let's use different letters than you used above, so maybe x, y instead of a,b
 
Okay. If x, y €I and x<= y then f(x) <=f(y)
 
Okay. So you know that's true for x, y in [a,b] by assumption.
Is it true for (a,b)?
 
Going by the graph... Yes
But at the end points the function is not differentiable
 
3:14 PM
I don't know anything about the graph, though. We never said anything about that.
I just know that when x <= y are both elements of [a,b], then f(x) <= f(y).
I am asking if when x and y are both elements of (a,b), then f(x) <= f(y).
 
Yes
 
Why is that true?
 
Because it falls under the closed interval and we know the closed interval is increasing.......?
 
yeah!
So that's the answer to your question
If one interval sits inside another, and your function is increasing on the bigger interval, it's definitely increasing on the smaller interval too
 
Okay got it. Thanks for your help sir
 
3:18 PM
Sure thing. There's no need to call me sir. I am no knight.
 
@MikeMiller that's answering a question by citing a more general fact...
 
@LeakyNun We answered the question first and the same logic implied that statement
I certainly did not cite that, but rather said the statement in an appropriate level of generality
 
alright
 
3:41 PM
Riemann's lemma: if $g$ is integrable then $\lim_{\lambda \to \infty} \int_a^b g(x) \sin(\lambda x) \ \mathrm dx = 0$
@MikeMiller maybe this is the key
also do you know the complex version of this lemma?
 
4:28 PM
$\begin{array}{cl} & \displaystyle \frac1{2\pi} \sum_{n=-N}^N e^{inx} \int_{-\pi}^{\pi} f(z) e^{-inz} \ \mathrm dz \\=& \displaystyle \frac1{2\pi} \int_{-\pi-x}^{\pi-x} f(z+x) \sum_{n=-N}^N e^{-inz} \ \mathrm dz \\=& \displaystyle \frac1{2\pi} \int_{-\pi-x}^{\pi-x} \frac {f(z+x) [\exp(i(N+1)z) - \exp(-iNz)]} {\exp(iz)-1} \ \mathrm dz
\\\approx& \displaystyle \frac1{2\pi} \int_{-\delta}^{\delta} \frac {f(z+x) [\exp(i(N+1)z) - \exp(-iNz)]} {\exp(iz)-1} \ \mathrm dz \\\approx& \displaystyle \frac1{2\pi} \int_{-\delta}^{\delta} \frac {f(x) [i(2N+1)z]} {iz} \ \mathrm dz \\=& \dfrac {2\delta (2n+
parts of this is clearly bogus
 
Hi all, can you please help me in proving this statement? let $L: H\to H'$ be a continuous linear Fredholm map between hilbert spaces, and let $c : H\to H'$ be a compact map. prove that L+c is proper when restricted to any closed bounded subset $A \subset H$.
The idea of proof given was to consider the following factorisation of the map. First we have $A \to H' \times \overline{c(A)}\times \overline{\rho(A)}$ $a\mapsto (L(a),c(a),\rho(a)$ where $\rho(A)$ is the orthogonal projection $H\to ker(L)$. The claim is that this map is injective and CLOSED. Injectiviness is clear, I've problems proving that this map is closed, in particular that the map $a \mapsto c(a)$ is closed
 
@LuigiM I may be spewing complete nonsense, but does it help that compact subset of hausdorff space is closed?
 
@LeakyNun I thought about it, but A is not necessarily compact if the hilbert spaces are infinite dimensional :(
 
I just saw "c, compact, c, closed"
 
nono, c is just a compact map, i.e. images of bounded are precompact
 
4:43 PM
maybe if you care to define the terms for me then I can help you think :P
 
mmh I think I'll write a question then, so everything will be written in a more clear way
 
5:20 PM
Does anyone have an example (or just experience) of how to refer to a result in a talk that is not online yet. Like if Jane Smith is giving the talk but hasn't posted things on the arXiv yet, should it just say "(Smith, unpublished)" near the statement? Is "(Smith)" presumptuous/implying too much?
 
5:47 PM
Problem: Let $T_X$ and $T_Y$ be topologies on $X$ and $Y$, respectively. If $T = \{U \times V \mid U \in T_X \mbox{ and } V \in T_Y\}$ is a topology on $X \times Y$, then either $T_X$ or $T_Y$ is trivial.
I could use a hint on this. I tried a proof-by-contradiction, trying to show that the union axiom fails, but I had no luck...
 
5:58 PM
@user193319 Draw a picture of simple examples (e.g. what if X and Y have only two points?) to get an idea of how your proof must go. Then carefully work out the logical consequence of "neither T_X nor T_Y is trivial" and write the proof based on the intuition your picture(s) gave you.
 
Okay. I can try that again.
 
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