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6:01 AM
That's not quite how I'd think about it.
 
@AlexBecker Correct me, please.
 
A key idea in topology is you want to capture as much information about a space as necessary, but no more than that. Essentially, a stronger topology has more "information" about a space and a weaker one has less. You want to work with the weakest possible topology that still does what you need.
 
@AlexBecker OK. So now we have this good ol $f$.
The author now gives some examples, such as "Attaching a space $X$ to a space $Y$".
And "Shrinking a subset to a point".
@AlexBecker Now, I have a question.
Because in the examples the author always "ends up" with "a resulting space"
For example, he takes $I=[0,1]$, and defines $I/\partial I=(I-\partial I)\cup \{a\}$ where $A$ is a new point. Then we define
Now we give $I/\partial I$ the indentification topology determined by $f$.
 
And he says this is the circle, and you want to know how this is the circle?
 
@AlexBecker Actually he says $p(t)=(\sin 2\pi t,\cos 2\pi t)$ is the desired function that induces $p^*:I/\partial I\to S^1$
@AlexBecker So quotient spaces provide a tool to do some twisting and turning on the spaces =P
 
6:13 AM
@PeterTamaroff I would prefer to say "gluing" instead of twisting or turning. This is a term that is often used.
 
@AlexBecker Well, in this case we "glue". He uses "pasting".
(Old book)
@AlexBecker The exercises for example, have terms like "cone over $X$", "suspension of $X$", "equator"
I could visualize the "cone over $X$" thing. It is quite an abstract generalization though, it seems.
 
7:10 AM
Hmm... where is it
 
7:36 AM
@AlexBecker I am trying to prove that if $G$ is a free abelian group, then $G$ is torsion free. Would it be helpful to know that $T(G)$, the torsion subgroup is the kernel of the map $f : G \to \Bbb{Q} \otimes_\Bbb{Z} G$ is precisely $T(G)$?
If $G$ is free then $G \cong \oplus_{n \geq 0} \Bbb{Z}^n$
Since tensor products distribute over direct sums and $\Bbb{Q} \otimes_\Bbb{Z} \Bbb{Z} \cong \Bbb{Q}$
This is effectively asking if some associated map $f' : G \to \bigoplus_{ n \geq 0} \Bbb{Q}^n$ is injective
I am now treating $\bigoplus_{n \geq 0} \Bbb{Q}^n$ as a $\Bbb{Z}$ - module.
 
8:00 AM
@AlexBecker It's ok I have posted a question
 
um....if a free abelian group had a torsion element, it wouldn't be free.
because you would have the relation x^n = 1
you can look at it this way: every subgroup of a free abelian group is free abelian. if x was a torsion element, then <x> is finite, that is: not isomorphic to Z. contradiction.
 
8:56 AM
Hello!
 
9:48 AM
@sos440 hey there (if you're still around)
guess not :-)
 
@ZhenLin Hey
 
hi
 
I posted an answer here
I did not know if you do it like that the proof becomes almost trivial at the end
@ZhenLin Is there a simpler proof of this fact?
 
10:26 AM
Hi
 
11:04 AM
Hi folks
 
11:33 AM
I'm a bit confused... because TeX seems not work here! So sad :(
 
@sos440 LaTeX does work here - but you need to get the "bookmarklet" thing to do it
You can get it from here
 
@OldJohn Thanks! Now it's a whole new world!
 
@sos440 Yep :))
Hi @KannappanSampath - how are things?
 
@OldJohn Pleasant, so far, today.
Thanks for asking.
How about you?
 
@KannappanSampath Not so bad, thanks - just chilling out, and not doing too much :)
 
11:54 AM
@OldJohn Do you interpret the sign over the exit door to the pure maths department that read "Beware!! - you are now entering reality" as a statement that pure math is not about reality?
 
@skullpatrol It was meant as a joke - but I guess that was the implication (not necessarily to be taken too seriously)
 
@OldJohn Roger Penrose wrote a book called something like The Road to Reality, do you think it should be taken similarly?
 
@skullpatrol I'm not sure about that - he maybe didn't intend the book to be a joke! - and probably expected the book to be taken seriously - but I have not read it, so I really can't judge
Ah - but he was a physicist, so probably had a different perspective on reality - compared to a pure mathematician
 
@OldJohn So, maybe the physics department has the same sign as the math department but theirs is over the entrance?
;-)
 
@skullpatrol Haha - never thought of that - quite possibly :)
 
12:08 PM
Bye folks.
 
I have just discovered that I actually own a coopy of Penrose's book - but not got round to reading it yet
 
How did you discover that?
 
By looking through one of my bookshelves :)
 
It has a lot of nice diagrams.
 
I have quite a lot of books that I bought when I saw them in second-hand bookshops, but have not found time to read them all yet
Now that I have retired, I hope to get through some of them :)
 
12:15 PM
How old is the oldest actively teaching Professor that you know of?
 
Not sure - I am not in academic circles these days, so I really can't answer that one
 
 
2 hours later…
1:46 PM
Hi guys :-).
 
Hello~
 
@sos440 Haven't seen you here before, so: hi!
 
@JonasTeuwen Hi Jonas @sos440, @J.M.
 
Hey, not-very-young John.
 
@J.M. :)
 
2:19 PM
@J.M. So far I've seen them say "Hello" :-) Now that I look back a bit, I see more...
Last time I greeted sos440, all I saw was "Hello" and here I see it, too. But somewhere in between, they were asking about ChatJax
@sos440: did you finally get the ChatJax bookmarklet?
 
@robjohn Yes, I believe he got it
 
It seems MO will be moving to SE 2.0. This should be interesting...
 
@OldJohn Good. It is hard to exist here without it sometimes.
 
said it made it "a whole new world" :)
 
especially with things like $f' : G \to \bigoplus_{ n \geq 0} \Bbb{Q}^n$ floating about.
Now that I have awoken, I need to take Lilly to the park :-)
bbl
 
2:30 PM
Monkey, yeah.
I woke up at 3:14 PM.
 
hi folks!
 
2:46 PM
hello
 
quiet day in here, i guess :D.
 
trying to count the zeros again, this time by integration.
zeta zeros
 
user19161
@JonasTeuwen You woke up at $\pi$!
 
Well... kinda.
 
user19161
@JonasTeuwen There are about 10 times when I woke up at 9.37 am, I wonder why...
 
3:01 PM
I usually wake at night, and fall asleep right after my alarm goes off
I tried fixing that by setting my alarm for 10pm :D
 
user19161
Is MO part of SE? Was it and will it?
 
MO?
 
user19161
Math Overflow.
 
@JasperLoy I suppose so, just older software.
 
3:07 PM
my understanding is that they are not "part of" SE. but then, i'm a newbie here
 
user19161
@JonasTeuwen I am not talking about the software but the organization.
 
@JasperLoy Well... They write the software right?
 
user19161
@JonasTeuwen But MO is not listed as one of the SE sites.
 
@JasperLoy They use a different license iirc.
 
Hello J.M. and robjohn! Sorry for late response. I was AFK, reading books...
 
3:13 PM
@JonasTeuwen The software is hosted in a different set of servers, too.
 
user19161
@J.M. So technically they are not part of SE am I right?
 
@JasperLoy Not part of the 2.0 network, yes.
 
user19161
@J.M. OK I should go read up more on this. I thought they were strictly not related at first.
 
So what are all the aggregate SE type sites? I know of stackexchange.com, stackoverflow.com, superuser.com, and askubuntu.com. Are there more?
 
"aggregate"?
 
3:23 PM
aggregate: like how stackexchange really includes a bunch of other site, such as math.stackexchange and englishusage.stackexchange, etc.
 
@Jeff Well, SO and SU and Ask Ubuntu aren't aggregate sites, in that sense.
They're within the SE umbrella also.
 
oh. you're right. hmmm.... i guess i mean top-level SE-like sites
 
@JonasTeuwen Hey bro.
@JonasTeuwen Are there any functions for which one cannot compute a Fourier series? (not necessarily convergent)
 
@Matt Convergent in which mode?
@J.M. Thanks :-).
 
@JonasTeuwen Not necessarily convergent at all in any mode. Like if the lecturer asks me in the exam for which functions I can compute Fourier series I'm tempted to say any function he can possibly think of if he doesn't want any sort of convergence.
But I wonder if that is correct.
 
3:36 PM
@Matt It almost always converges pointwise a.e..
So does "converges a.e." qualify as "not convergent"?
 
Yes.
 
Otherwise, you need an $L^1$ function and you can prove the existence using PUB.
 
@Matt Might it be hard to calculate a Fourier series for a non-measurable function? :)
 
@Matt Easy. Just take a step function. $-1$ for $x < 0$, $1$ for $x \geqslant 0$.
Does not converge to $1$ in $x = 0$.
 
@OldJohn Ah good point. Of course the function has to be measurable otherwise I cannot compute the integral for the coefficients.
@JonasTeuwen Yes but if I don't want the series to converge to the function then that is not a counter example.
 
3:38 PM
Will be pretty hard to cook up a non-measurable one as well.
 
@Matt I thought you were asking for one where you could not compute the series???
 
@Matt It does not converge to the function... so you need to be more specific.
 
@OldJohn Yes exactly. And you told me the answer! : )
 
Mofo's will kick me out of the building in 20 minutes 8-(.
 
@JonasTeuwen I'm not sure what you mean.
 
3:40 PM
@Matt I mean: I don't understand what you want.
 
Unless the function is not measurable I can always compute a series.
 
@Matt OK! - I mis-understood your response - sorry :)
 
@Matt You can - but it can be divergent.
 
@JonasTeuwen If the lecturer asks me "For which functions can you compute Fourier series" and I say "for any measurable function if you don't make any convergence requirements" I want to know from you how many points from 0 to 10 where 10 is max do I get?
 
maybe you need "integrable" rather than "measurable" (tell me to shut up if I'm talking rubbish)
 
3:42 PM
No no, never mind integrable, if I don't want convergence I might as well have coefficients that are infinite, no?
@JonasTeuwen And then I'd add "If you want $L^2$ convergence of the Fourier series then the answer is for $L^2$ functions".
 
@Matt For all $L^p$ functions with $p > 1$.
@Matt Right, just make sure the lecturer also understands that you know how $L^p$ spaces are embedded on spaces of finite measure.
 
@JonasTeuwen To get finite coefficients? (because $L^p \subset L^1$ if space has finite measure?)
 
@MattN Because of the Carleson-Hunt theorem (it is highly non-trivial, so perhaps they did not teach you this).
 
They did not.
But I need to know for which functions I can compute Fourier series. And now I guess I'd have to say $L^p$ for all $p \geq 1$ and finite measure space if we want the coefficients to be finite but not necessarily want convergence of the Fourier series.
 
@Matt Yeah, the question is too vague for me.
 
3:46 PM
My dad bought me a Kindle Fire, it broke and I returned it. I got the replacement yesterday. Today the replacement broke! grrr.... :(
 
You can probably compute it end end up with garbage.
@Jeff How did you break it?
 
@JonasTeuwen i didn't break it. it broke. it stopped working.
 
@JonasTeuwen Well that's what I was trying to say: I get garbage but I can compute it if the function is measurable.
 
@Jeff That's quite a shitty device (or bad luck) 8-).
 
...although i think i broke the first one by leaving it near the microwave.
 
3:47 PM
@Matt Yes.
 
So it doesn't have to be in $L^p$ it just has to be measurable.
 
@JonasTeuwen well, the replacement was probably a refurbished one. refurbished machines never last.
 
@Jeff near the microwave? Unless your microwave is broken and you didn't actually put it inside that would make no sense.
@Matt The integral needs to make sense.
 
The integral makes sense if the function is Lebesgue measurable.
It might be infinite.
 
@jonas that was what i thought, too. but microwaves leak and may have caused damage to the chips.... maybe
 
3:48 PM
But that's ok.
 
@Matt Just measurable is fine I think.
 
Then the Fourier series is also infinite.
Yep, me too.
 
@Jeff Well... pretty sucky microwave.
 
@jonas i think all microwaves leak a little bit. don't they? (is there a stackeschange site where i can ask that? :D ).
 
@Matt Okay, I agree. The point is not the correct answer for oral exams, but to know what you are talking about and you seem to do that.
 
3:49 PM
And then if I want the coefficients to be finite I require $f$ to be in $L^p$ and require the space to have finite measure.
 
@Jeff They do, but that should not be enough to destroy a device.
 
@JonasTeuwen No. I want to give the correct answer in the oral exam!
 
@jonas in that case, then i didn't break either one of my kindles
 
@Matt There is no good answer to the question you pose, bro...
 
If he tells me that what I am saying is complete rubbish I'll immediately go into panic mode.
 
3:50 PM
If that microwave leaks enough to fry a Kindle, I would not want any part of my anatomy near it !
 
Bloody monkey, need to leave the building in a couple of minutes.
 
@JonasTeuwen The question as posed by me is a one-to-one faithful copy of an exam protocol and was asked by Manfred as is.
 
@Matt Yes, so it is a question to see if you know what you are talking about 8-).
 
Anyway, I think you bros have helped me quite a lot.
 
@Matt Purrrrrfect.
 
3:51 PM
I will say for measurable functions as long as he doesn't want any sort of convergence : )
Then I can restrict and require more stuff
Then eventually say that if we want a nice life we want them to be in $L^2$.
Ok.
So much for Fourier stuff.
Now I have to go back to Sobolev spaces.
 
Need to leave the building.
 
Thank you very very much, bros! @JonasTeuwen @OldJohn
@JonasTeuwen See you later?
 
@Matt No problem - not sure I was really much help
 
Yes you were!
 
@JonasTeuwen Later!
 
3:53 PM
@Matt Sure :-) @OldJohn Bye.
 
4:04 PM
@Matt Then I'll say it now: this is nonsense. If your function isn't integrable then your Fourier coefficients aren't well-defined in the first place. (oscillations may lead to computing $\infty - \infty$.)
Or stuff like that.
 
Exactly. So the F. series is infinite.
Why is that non-sense?
 
No, $\infty - \infty$ is not defined at all.
 
Hi : )
 
Hi.
 
Where does this $- \infty$ come from?
Ah.
Yes. But the answer is still right: you can compute the series. But it might be garbage.
 
4:07 PM
No you can't even define the series.
 
The series is defined to be $\sum \langle f, e^{ikx} \rangle e^{ikx}$. I thought.
 
This is not well-defined if your function is only measurable.
 
Yes, that's what I mean by garbage.
So I am not allowed to say something like that?
 
You'd better not.
 
Scary. : (
But then it's boring. If I have to require my space to have finite measure and can only do it for $L^p$ functions for $p \geq 1$.
Maybe I can do reverse engineering and say for any function for which all the Fourier coefficients are finite defined?
 
4:11 PM
Well, if you want to go general say for a tempered distribution.
 
No, then he asks me what that is.
I don't want to be asked about tempered distributions.
 
Then don't go general. The most straightforward thing is integrable functions.
Second-most straightforward is $L^2$-functions.
 
That was my originally planned answer, $L^2$, but then I realised that I can do it for any function with finite coefficients.
I'll go for integrable then, I guess.
No.
Yikes. I'll have to think about this more carefully.
 
I take it he only discussed the Fourier transform on the circle. Then integrable is just fine (as is $L^2$). Both give no problems whatsoever. I don't know what you mean by "finite coefficients". If you have finite coefficients then finiteness of the zero'th coefficient tells you that your function is integrable.
 
True : (
 
4:16 PM
Why is that bad?
 
(referring to your last sentence)
@t.b. Because even though I know how the coefficients are computed I didn't make the connection : (
Thank you.
 
Don't panic! Others didn't make that connection either.
 
We don't know that. You probably did, for example.
Back then when you were where I am now.
Anyway. Thanks a lot.
I am going for a walk now, been doing futile attempts all day. Need some fresh air now : )
Take care and see you later (or another day)!
 
Well, we had a year-long Fourier drill with your favorite professor.
See you, I should go, too.
 
@Matt Back.
 
4:25 PM
@Matt Oh no. I missed t.b.
 
@Matt Right, so tb told you the integral must make sense 8-).
 
$\Huge \text{Brian Scott is back}$
 
@PeterTamaroff Where was he?
 
@JonasTeuwen I don't know. His Ki was very dim.
@JonasTeuwen How is the health over there?
$$\mathop { \odot \odot }\limits_ \cup $$
 
@PeterTamaroff Health sucks. Girlfriend better.
 
4:34 PM
@JonasTeuwen Did you find out what you got?
 
@PeterTamaroff No.
 
@BrianMScott
@JonasTeuwen $$\mathop {\bullet{\text{ }\bullet}}\limits_ \sim $$
 
@PeterTamaroff 8-).
 
@JonasTeuwen You need to code some TeX smileys
 
@PeterTamaroff Too high-tech.
 
4:38 PM
Maybe we can get like a small panel with some codes =P
 
@PeterTamaroff I'll stick with 8-).
 
oh that's a smiley. i thought it meant "flash an antenna dish". my bad.
 
@david lol
 
@DavidWheeler HAHAHHA took me a while to get it
 
4:55 PM
barbecue time :)
 
@OldJohn Enjoy.
 
@JonasTeuwen Thanks! - and later a few beers with some friends - not much maths tonight :)
 
@OldJohn Sure, enjoying life has many aspects - not only maths 8-).
 
@JonasTeuwen Glad to hear girlfriend feeling better!
 
@OldJohn Went up to 41°C, so I called the GP again, he asked a couple of questions and said: well, if it goes up to 41.7°C I will come, but for now it sounds fine!
And now it went down.
 
5:09 PM
@JonasTeuwen Phew!
 
@OldJohn Actually, the doctor said it is not so harmful if that is basically the only symptom and pain does not get relieved from paracetamol.
 
@JonasTeuwen Stop! It's morphine time!
 
@PeterTamaroff I agree!
 
@BrianM.Scott Hello Brian.
 
Hullo. I’ve been up most of the night, so I probably won’t be around too much longer this morning.
 
5:16 PM
@BrianM.Scott What time is it there? It is 14:16 here. =/
 
@PeterTamaroff It’s 13:16, but I’m still thinking of it as morning for some reason.
 
@BrianM.Scott Oh. Well, I'm just reading about identification topologies. And I have a little doubt on the final construction.
 
@JonasTeuwen Her temp is 41°? That is pretty high for an adult. Hopefully, she has seen a doctor.
 
@robjohn No, but talked to one on the phone. (she is 20).
He asked some general questions about other health problems and said: "if it gets worse, call again. Nothing to worry about now".
 
@BrianM.Scott We were just noticing yesterday that you were gone for a while.
 
5:27 PM
Yes, I was offline for about a week and a half.
 
@JonasTeuwen I figured she was an adult :-)
 
@robjohn 20 is legally adult 8-).
 
kids can take a bit higher temp
 
If she would be 40 it might have been more troublesome.
 
@JonasTeuwen Not in USA!
 
5:28 PM
@PeterTamaroff Legally adult to get the chair, but not to drink. Peculiar.
No, in NL 18 is official adult for everything.
 
@JonasTeuwen Same here.
 
But cannot get a drivers license for trains with passengers. Need to be 21 for that.
That's the only thing I think.
Well, you can get it. You can go to the train company at 18 and say: "I want to be a train driver!" they will be: "alright! you get an internal education about trains! Cool eh?". So then the next three years you can do small trains which stop like every five minutes 8-).
 
@BrianM.Scott Could I ask you something?
 
Sure.
 
@BrianM.Scott OK =)
 
5:37 PM
@BrianM.Scott To be pedantic: "You have just done so." 8-).
 
So, the author first talks about what an identification is.
Then he proves a little lemma
If we have an identification $p:E\to B$ and a continuous function $G:B\to Y$
such that $p(x)=p(x')$ implies $G(x)=G(x')$,
We can "induce" a continuous function $g:B\to Y$ such that $gp=G$
 
(often, such a state of affairs is referred to by: "G factors through p")
 
He doesn't make it explicit, but I understand what we do is define $x\sim x'$ iff $p(x')=p(x)$, and we define $g(b)=G(x)$ for any $x\in \widehat {p^{-1}(\{b\})}$
Where $\widehat{.}$ means equiv class
 
@PeterTamaroff I believe that you want $G:E\to Y$.
 
$g$ is "well defined" because $x\sim x'$ means $G(x)=G(x')$, so the choice of $x$ in the equivalence class is irrelevant.
@BrianM.Scott Yes, typo, sorry.
 
5:42 PM
I believe I need to go to Helsinki somewhere the coming weeks. I have lost my plane ticket 8-))).
 
for that even to make sense, i believe p has to be surjective.
 
@PeterTamaroff Yes.
 
@DavidWheeler Yes, identifications are by definition onto.
 
and does he require that identifications are also continuous?
 
@BrianM.Scott OK.
Well, yes, they are "über" continuous =P
$U$ is open $\iff$ $p^{-1}(U)$ is open
 
5:44 PM
@JonasTeuwen Mostly they never look at plane tickets these days - they just ask for your passport, I think :)
 
@BrianM.Scott OK, I move on.
 
@OldJohn With me they usually just ask for the ticket and not the passport...
@OldJohn But it would be nice that I know which flight I actually booked.
 
@JonasTeuwen Darn :(
 
@OldJohn Oh, I can just call the travel agency 8-).
 
@JonasTeuwen :)
 
5:45 PM
@Peter: It’s exactly like starting with a group $G$ and a surjective homomorphism $h:G\to H$ and showing that if $K$ is a group, and $f:G\to K$ is a homomorphism such that $f(g)=f(g')$ whenever $h(g)=h(g')$, then there is a homomorphism $g:H\to K$ such that $f=h\circ g$.
 
@PeterTamaroff just wondering...because continuity usually presupposes some sort of topology defined on the domain and co-domain
 
hey all
 
@David: Peter is talking about topological spaces.
 
@BrianM.Scott Oh, that's what Alex becker said when he meant "Categorically correct" maybe :P
 
@PeterTamaroff Very likely.
 
5:47 PM
@BrianM.Scott an "homomorphism" is a map that preserves the "strcuture" of a group, correct?
 
@BrianM.Scott i'd say it's "more like" inducing an equivalence relation on a set from a function...there no notion of "multiplicativeness" in topological spaces.
 
@OldJohn Ah! I found the flight number. Also, why are you not at the barbecue? It will not start itself!
 
@PeterTamaroff Yes. Specifically, it satisfies $h(x*y)=h(x)\cdot h(y)$, where $*$ is the operation in the domain and $\cdot$ the operation in the range.
 
I mean $H(x y)=H(x)H(y)$ and $H(e)=e$
 
@JonasTeuwen I was cooking the food while chatting earlier - now finished eating
had my laptop out in the garden
 
5:49 PM
@DavidWheeler Peter isn’t using any notion of multiplicativeness. His $gp$ is a composition.
 
OK yes I should tell apart the operations and identities, but well.
 
user19161
@peter Your missing BMS has brought him back. You have superpowers.
 
@BrianM.Scott OK, so now we define the identification topology: given an onto function $f$from a topological space $X$ to some set $Y$, the topology $\mathfrak I'$ on $Y$ consists of those sets $U\subset Y$ such that $f^{-1}(U)$ is open in $X$. This makes $f$ an identification.
 
@BrianM.Scott this i know....but as i understand it, Peter's exposure to abstract algebra isn't extensive enough for him to truly appreciate your comparison.
 
@DavidWheeler I got it! It is true I know very little about abstract algebra, if nothing,but I got what he said.
So now comes the "heavy" part of the chapter
 
5:53 PM
No available rooms.
That sucks.
 
@JonasTeuwen In Helsinki?
 
sometimes it's called the "final topology" on Y, because it's the strongest (finest) one that works.
 
@OldJohn Yeah, at the hotel I looked. The other ones a bit too expensive.
 
@JonasTeuwen :(
 
@OldJohn But another hostel is slightly more expensive, but I can use the kitchen! 8-). So I can save on food expenses. Perfect.
 
5:56 PM
@JonasTeuwen Excellent
 
@BrianM.Scott We start with any function $f:(X,\mathfrak I)\to (Y,\mathfrak I')$. We define $x\sim_f x' \iff f(x')=f(x)$. We quotient $X$ by $\sim_f$, and get $X/\sim_f$. $\pi_f :X\to X/\sim_f \;/\;x\mapsto \hat x$ is onto, so we give $X/\sim_f$ it the identification topology determined by $\pi_f$.
 
@JonasTeuwen I ate reindeer last time I was in Finland - very tasty :)
 
Now, note that $\pi_f(x)=\pi_f(x')\iff f(x)=f(x')$, so we induce a continuous function $f^*:X/\sim_f \to Y$ such that $f=f^*\pi_f$
 
@OldJohn i think it tastes a bit gamey, but its ok
 
@DavidWheeler Now comes that part!
 
5:57 PM
@DavidWheeler Yeah - I quite like gamey meat
fits with my paleo diet :)
 
@PeterTamaroff Okay.
 
@DavidWheeler It is easy to see $f^*$ is one one. Since $f^*$ is continuous, we have that $f^*{}^{-1}(\mathfrak I')\subset \Bbb I$ where the latter is the identification topology, and the former the topology on $Y$.
Now, since $f^*$ is one one, this means $\mathfrak I'\subset f^*(\Bbb I)$
 

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