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12:00 AM
@MatheinBoulomenos Why question is that "Is is true that $\int_a^b \lim\limits_{n \to \infty} f_n(x)=\lim\limits_{n \to \infty} \int_a^b f_n(x)$ even if $f_n$ does not converge uniformly?" We know that uniform convergence implies the integral limit exchange. But is it true the other way around?
 
oh
now I understood your question
I thought you wanted an example where you can't interchange the integral
the example $x^n$ on $[0,1]$ from ultradark works. This converges non-uniformly to the function which is $0$ on $[0,1)$ and $1$ at $1$ (convergence has to be non-uniform since the limit is not continuous), but the integral limit exchange works still
if you go further in real analysis, you will get to stronger theorems which allow exchanging limits and integrals, such as dominated convergence and monotone convergence
 
@MatheinBoulomenos What about the example $f_n(x)=\frac{2x}{n}+\frac{1}{n^2}$? Does it work?
 

 Group Theory

Let's discuss group theory!
 
@MatheinBoulomenos Thank you so much.
 
@user330477 this converges uniformly to $0$ on each closed interval $[a,b]$
 
12:21 AM
Is it kosher to raise a number to a probability
 
what's a probability
 
a number between $0$ and $1$
 
more generally, for $a, b \in \mathbb{R}$, is $a^b$ well defined?
hint: yes
 
okay good
so if $p(x)$ is a function that gives a probability, how does one interpret $n^{p(x)}$?
is there any interpretation?
 
12:45 AM
well, what is $n$, a natural number?
 
yeah
 
you actually have the burden of defining $n^{p(x)}$
and we haven't answered what $a^b$ is
venture a guess
 
1:03 AM
I am going to guess that raising a natural number to a probability function, acts as an isometric map on $p(x),$ such that a bijecition can be formed between $p(x)$ and a target region. This target region encodes information about $p(x).$ The benefit of such a map is that there is a way to go back and forth between the probability function and the encoded probability in the target region
 
yeah.. can you define it explicitly?
forget the probably function for a second. What's $a^b$?
 
its a number raised to another number
 
i know what $2^3$ is. but on the face of it, i don't really know what $\pi ^ e$ is
does it even make sense to raise an irrational to the power of another irrational?
 
oh
 
Or $2^{1-2i}$, for that matter.
 
1:12 AM
yeah, that's another story in and of itself. complex exponentiation is a bit different
 
okay let's say $p(x)$ is some function $1/\ln(x)$
 
(Yeah, my mind is on generalizations. Like, how do you know what you're doing can even make sense in the first place? How do you define $2^s$ where $s$ is an element of the dihedral group on the n-gon?)
 
yuh
 
taking $n^{p(x)}$ yields transcendental numbers
 
@Ultradark you haven't circumvented the issue
 
1:17 AM
what's the issue
 
you dont know if $\pi ^ e$ is even well defined
 
$n$ is a natural number
 
and $\frac{1}{\ln x}$ is certainly going to give you nasty numbers
unfortunately the base isn't the issue
 
Like, how do you know if it yields transcendental numbers? How do you know it yields a number at all? What if it yields a chicken?
 
so, ok, what does $n^e$ mean?
 
1:19 AM
@TedShifrin maybe whenever you get a chance you can look at my question.

https://math.stackexchange.com/questions/3122924/comparing-sigma-algebras-with-topologies
 
oh wait, even $1/\ln(x)$ gives transcendental numbers
that might be a problem
it is unknown whether $n^{1/\ln(x)}$ is transcendental
solution: round the number to $4$ decimal places
now it is rational
 
that's the solution of the physicist
 
so now we have transformed $p(x)$
 
im not sure im following
hows this. whats the verbatim problem statement you are trying to solve
 
sounds like you would do: step 1: define exponentiation for nats, step 2: try defining for positive rationals, step 3: try defining for positive reals. and then it would take some more work for showing there is some natural way to raise $n^{P(x)}$ where P(x) is some distribution...
doesn't sound easy lol.
 
1:33 AM
well this allows us to set up a bijection between the target region and the region outside, which I'll denote, $\zeta$ and $L$ respectively
$\zeta \in (0,1) \times (0,1)$
and $L \in (1,\infty) \times (1,\infty)$
these two regions have the same size
 
@Dair yeah..
@Ultradark let's drop all the fancy language
let's follow @Dair 's suggestion instead
 
but the bijection
 
forget the bijection
you haven't even defined the object at question properly
and you were almost there
 
really?
 
you can define it for 4 decimal places
(can you?)
(...how?)
 
 
4 hours later…
5:24 AM
@Ted: I'm having a hard time on proving that basis of different finite cardinalities don't exist; i.e., that theorem you told not to use matrices.
I guess I'll have to use some equivalent statement of the rank-nullity theorem
 
I think I just solved the Tao conjecture again
 
5:43 AM
@Lucas: You can write out the proof of Theorem 4.1 just with summations and without using coordinates (in those matrices) for the vectors $v_j$ and $w_i$.
 
I don't think I know how.
I said that "has basis of cardinality $n$" iff bijective linear map $\phi: \Bbb F^n \to V$
 
Just write $w_j = \sum a_{ij} v_i$ and consider $\sum c_jw_j$. Rewrite that as a linear combination of the $v_i$.
 
analogy to linear independence, but only injective linear map
 
I'm proving specifically the theorem I stated, not a different approach. From that you conclude that dimension is well-defined (as in Theorem 4.2).
 
I'm sorry beforehand since it's 2:45am here and my classes start... tomorrow.
 
5:45 AM
Well, I'm not staying around long, anyhow.
Happy classes.
Pretty much every treatment of linear algebra I know shows that if you have linearly independent vectors and spanning vectors, then there are fewer (or equal) of the first than of the second.
 
@Ted: I'm not currently with the book. We have more $w_j$ than $v_i$, is that right?
 
Right.
 
Hmm, ok. So $\operatorname{Span}(w_1, \dots, w_n) \subseteq \operatorname{Span}(v_1,\dots,v_m)$
That's basically what we get when we rewrite a linear combination of $w$ in terms of $v$
Or being explicit (no pun intended), $\sum c_jw_j = \sum\sum a_{ij}c_jv_i$
 
Right ... And because the matrix $A = (a_{ij})$ has more columns than rows, there's a nonzero vector $c$ ....
(So we're not avoiding matrices entirely. But this proof works fine in abstract vector spaces ...)
 
6:08 AM
thanks god lmao
just the way I was thinking. thanks, @Ted. :)
 
You're welcome, Lucas.
 
is there a bijection between these two parts?
 
Hi guys, I have a simple question https://math.stackexchange.com/questions/3124499/are-the-points-that-make-the-function-fx-non-differentiable-the-same-as-the-po

I am sure many of you know the answer as it is from very basics of mathematics. Could you answer it please?
 
6:47 AM
Quick what's 40.44% of 25 (do it in your head)
 
I cannot think of any way to do such a complicated number on the head
 
19
*14
 
@Secret When you see it you'll kick yourself
 
except maybe noting the fact that 25*4 gives 100, but I cannot do that fast enough
 
OK want a hint
 
6:50 AM
10.98
 
sure
 
What's 1/4 of 40.44?
 
10.11
 
Now notice that X% of Y is the same as Y% of X
(because X*Y/100 = Y*X/100)
 
4*0.1011*25 = 100*0.1011 =10.11
ok that's clever
 
6:55 AM
Right - 40.44% of 25 is the same as 25% of 40.44
which is 1/4 of 40.44, or 10.11
 
Makes me think of number theory again, the art of splitting numbers in a suitable way
 
I just solved the Waiters dilemna
 
I'm imagining you waiting a long time in a restaurant and then storming into the kitchen and making the pepper steak yourself
 
lol
 
Wait so what's the waiter's dilemma
I thought it was a math problem but Googling didn't find anything
 
7:02 AM
nevermind I was just saying something related to the percent stuff
 
Oh I thought it was unrelated
 
I want to assign a finite result to an infinite quantity
0
Q: What does it mean to raise a quantity to a probability?

UltradarkLet's say you have a function $p(x)=1/\ln(x)$, that returns a probability. Take $\phi(x)=2^{p(x)},$ and correspond the regions $\zeta_x \in(0,1) \times(0,1)$ and $L_x \in(1,\infty) \times (0,\infty),$ via $f(x)=mx.$ Set $f(x)=p(x)=\phi(x)$ to find the upper bound of the integral, $T$. Do t...

thoughts?
 
7:41 AM
Is that the correspondance you asked in the h bar?, if so it is already answered
 
Oh
wonder why it got downvoted
 
not a downvoter ( I am too lazy to vote now in the main), but I think the comments have voiced some concerns on the unclear on what p(x) is doing.
Also, for me specifically, it is not clear what is N
In fact without that diagram you use in the h bar, I will not be able to figure out you are asking whether there is a bijection between two areas
 
oh i thought people would plot it
maybe I should delete it
So you think it's true, yet people are downvoting?
 
8:23 AM
You need to be clearer on articulate your question
 
The average of 1, 2, and 3 added to the average of 10 and 20 is the same as the average of 1+10, 2+10, 3+10, 1+20, 2+20, and 3+20
$\operatorname{avg}(1,2,3)+\operatorname{avg}(10,20)=\\ \operatorname{avg}(1+10,2+10,3+10,1+20,2+20,3+20)$
Thinking about linearity of expected value
though I suppose the more surprising case is that it still works when the variables aren't independent
It's a bit weird that $\Bbb E(X-\Bbb E(X))\Bbb E(Y-\Bbb E(Y))=\Bbb E(XY)-\Bbb E(X)\Bbb E(Y)$.
It's almost like claiming $(a-a')(b-b')=ab-a'b'$
 
Im going to put it on meta
 
9:05 AM
 
8 hours ago, by Rithaniel
(Yeah, my mind is on generalizations. Like, how do you know what you're doing can even make sense in the first place? How do you define $2^s$ where $s$ is an element of the dihedral group on the n-gon?)
$🌀(\text{exp},\text{Group})$
 
The problem is $s$ has finite order
I think
I know that you can't raise things to elements of $\Bbb Z/n\Bbb Z$ because even if $a\equiv b\pmod n$ we don't usually have $2^a\equiv2^b\pmod n$
 
Z/nZ is easy to see what's going on, but it is not clear what will 2^s where s is a finite group element really mean. I do recall the exponential map is quite nice on a variety of objects though, so perhaps something like 2^s = exp(s ln 2)
 
Or maybe you can get stuff to work
You can definitely take the exponential of matrices
 
but then I do not remember what ln means in the context of groups, ln is much less well defined compared to exp
(and likewise, ln of matrices only make sense for some subsets of them)
 
9:15 AM
Do the Taylor series, it'll end up as an element of the group ring (I think that's what it's called)
 
a group version of a taylor series??
 
or maybe division by $n!$ messes things up when an element has order $n$
@Secret Take a multiplicative group, add formal addition, you get the group ring
 
Ah, so we extend the group into a group ring
 
Oh never mind division by $n!$ should be fine
and if it has finite order then it's kinda a finite sum
 
yeah, because eventually a $a^n = e$ will be encountered and those terms will basically vanish
 
9:18 AM
Well no because $a^{n+1}=a$ again
but you can collect all the $a$ terms
If $s^2=1$ then $e^s=\frac{e+e^{-1}}2+s\frac{e-e^{-1}}2$
which works if we substitute in $s=1$ or $s=-1$ which is good
AKA $e^s=\cosh1+s\sinh1$
(The equation $e^{\pm1}=\cosh1\pm\sinh1$ is kind of like a "poor man's Euler identity")
$e^{\pm x}=\cosh(x)\pm\sinh(x)$
 
yeah, that's basically the hyperbolic version of Euler's identity
hmm... so by collecting the terms together, we basically have n finite sequences
one for each power of a
meanwhile ln s is harder to deal with, because there could be convergence issues depending on what s is
 
The problem is, the group ring doesn't have commutative multiplication, so $e^ae^b$ won't equal $e^{a+b}$ in general
but that's fine, that happens with matrix exponentiation also
and it'll work if $a$ and $b$ commute
 
yup, such is to be expected when we generalised to more abstract structures. Something nice is bound to fall apart, though it does not bother me because I am used to the weirdness
 
and then $2^s=\exp(0.69315 s)$
 
sounds good
Unrelated, now I am starting to wonder...:
Conjecture: Given any mathematical object $M$ with structure $S_M$ that is not invariant under the Cyclone Operator 🌀, then $🌀(M) \leq M$ where $\leq$ is a partial order that corresponds to the degree of "niceness" of $S_M$
Or put that in plain terms, if $M$ is a mathematical object which its niceness is not preserved when generalised, then its niceness must be nonincreasing the more it is generalised
For example:
Field < Ring < Semiring < Nearring < Ringnoid
or more concisely:
Field < 🌀(Field) < 🌀🌀(Field) < 🌀$^3$ (Field) < 🌀$^4$ (Field)
Since Rithaniel is thinking about exponentiation of group elements, and we are talking about $e^x$ and its taylor series, it is then logical that a generalisation like the following can occur:
$$e^🌀 = \sum_{k=0}^{\infty} \frac{🌀^n}{n!}$$
however, there are a lot of issues with the well defineness of this expression. To start with:
1. Objects under the action of more cyclone operators is more generalised than those that are operated on less, thus the formal addition will need to be able to account for that
2. A notion of the limit of objects is needed to evaluate an infinite sum of basically arbitrary mathematical objects. The direct limit in category theory might be able to handle that to some extent
3. It is not clear what does $r🌀$ means when $r$ is an irrational
What's interesting is that if the conjecture is true, then $e^🌀$ is easy to evaluate because the infinite series will eventually end up with a lot of terms that is a supremum of the generalisation of the object being operated which has minimal structure (i.e. approaching a set). For example:
Let $M$ be the object and $M_{\infty} = \sup_{🌀} (M)$. Then if the conjecture is true:
$$e^🌀M = \sum_{k=0}^{N} \frac{🌀^n}{n!} M + M_{\infty}\sum_{k=N+1}^{\infty} \frac{1}{n!}$$
and thus the exponential cyclone map of M largely derive its structure on the first few terms of the taylor series expansion and hence its "niceness" is in a sense bounded to the first few generation of generalisations
@Rithaniel Why stop at generalisation of an object when you can generalise the generalisation itself ad nausem lol
 
9:52 AM
Are you guys discussing the exponentiation to the power of an element of the dihedral group? I was presenting it as something I suspected you would never be able to define exponentiation for.
Also, I don't know this emoji operator.
 
Yes we are. Akiva and I are the most weird people in this chat, thus we figured out a way to sort of define it
I invent this Cyclone Operator so I can systemise the art of generalisation itself, because the Explosive Generalisation Operator is too powerful to be useful
 
Well, weird is relative.
I'd say your probably pretty resourceful if you managed to actually define it. That's a little mind blowing.
Yeah, I'm not quite following the definition of the "explosive generalization" either.
 
Well... tbh, I don't think us human beings can ever be able to use it in its entirely, as you will need to somehow knew the to be discovered mathematics in the future or otherwise, which is unknowable by definition. Basically the idea of explosive generalisation is, given an example of some mathematical object with some property, find all generalisation of said object that also have that property. For example:
 
Though, that's generally the case when a person first encounters a new definition. I need to see it utilized a few times and understand the results achieved from it's use, in order to really understand it.
 
We knew that addition is a relation that puts two objects together to make one object, such as 1+1=2
One can then started to think, what is an object that is more general than addition, yet preserve its basic properties
Multiplication is one example because $a+\underbrace{\cdots}_{\text{n times}} + a = n\cdot a$
 
10:02 AM
Well, first, you need to define "more general"
Like, what is the quality of "generalness" which addition has? How do you increase it? How do you decrease it?
Perhaps counting (addition by 1) is more general and multiplication is more specific.
Perhaps they are all three of equal generality.
 
I have not put much thought into that, but I guess one can define it this way: Given two mathematical objects M, N satisfying some axioms and theorem, then N is more general than M if they share at least one axiom or theorem, but N satisfy far less axioms than M, and hence less constrained.
For example, noncommutative rings is more general than commutative rings since for the latter, ab=ba has to hold
Thus a commutative ring is a specific example of a noncommutative ring where ab=ba holds for all elements in the ring
They both otherwise share most of the ring axioms and hence most properties
 
Okay, that can be an interesting approach. but what about arbitrary axioms? Like the axiom of "no 5s" where, given polynomials in a field k, to satisfy the axiom of "no 5s," 5 cannot be a solution to any such polynomial.
(My explanation might be a little bit gibberish, it's kind of late for me)
In this sense all objects satisfy infinitely many axioms, one still might satisfy more than another, but how do you count them?
 
That's actually where I initially ran into problems when trying to define it, and deduce the resulting generalisations cannot form a linear ordering but has to be some kind of partial order. Specifically, say you want to retain the "no 5s" axiom, there are so many ways to generalise from polynomials by throwing away one or more axioms (or to consider objects where polynomials is one example), and
 
(Of note, they might satisfy axioms vacuously)
 
when the number of axioms are infinite like those in an axiom schema, then yes there will be an issue. I have not figured out how to get around that yet
 
10:14 AM
Fair enough, then sounds like you've work to do on your theory. But you're not stumped yet.
Anyways, I came up with a very dumb algebraic construct, which I will share:
(Note, this is just for fun)
 
$+,\oplus,\int,\sum,\sum^{\infty},...$ all share the same property of summation, but they are different generalisation from one or more, and it is not clear how to keep track of it yet. What 💥(+) does is it gives the above list including all the partial ordering that relates them to give a notion on how general they are wrt to each other
@Rithaniel show it
 
(I'm typing, give me a moment)
A "Brick" is a set $B$ equipped with a binary operation ($\circ$) satisfying the Brick axioms:
1. Axiom of closure: $a,b\in B\iff a\circ b\in B$
2. Axiom of divisibility: $c\in B\implies\exists a,b\in B$ such that $a\circ b=c$
3. Axiom of deadweight: There exists a pair of elements $\square,\blacksquare\in B$ satisfying $a\circ b=\square\iff a=\blacksquare$ or $b=\blacksquare$ and this is the only pair of values for which this holds.
4. Axiom of anti-associativity: $(a\circ b)\circ c=a\circ (b\circ c)\iff a=c$
 
anti associativity.. that's interesting, never thought of that
 
A completely useless construct, as far as I can determine.
 
Let me think...
 
10:26 AM
But I had fun thinking about it.
 
(NB, when thinking about algebraic structures, I tend to omit mentioning the closure axioms, because they are so obvious have to hold for an self defined algebraic structure to be useful)
 
Now you're gonna make me think of a structure where closure isn't required.
 
well, some of these do exists, for example, the irrationals are not closed under any ring operations
but the interesting thing is there seemed to always exist a larger structure where the closure holds again
 
Yes, the "completion" of the set.
 
It will be really interesting if there exists some "non amenable" algebraic structure such that closure is violated and cannot be fixed by completion and still remain useful
I am not ready to deal with "incompletable algebraic structures" however
Hmmm... $a\circ b = \square \implies \blacksquare \circ b = \square$ or $a \circ \blacksquare = \square$
for ease of writing, I am going to omit the $\circ$ since your structure is at least a type of magma as it has only one binary operation
 
10:34 AM
Not quite. If $a\circ b=\square$, then either $a$ or $b$ has to be $\blacksquare$
 
isn't that what I am showing above?
 
and, if you combine $\blacksquare$ with anything, you immediately get $\square$
Ah, I thought you were saying something a little bit weaker.
nevermind
The way you were writing it doesn't necessarily disallow $ab=\square$ for arbitrary $a,b$
 
ah ok
Also:
In mathematics, particularly abstract algebra, a binary operation • on a set is flexible if it satisfies the flexible identity: a ∙ ( b ∙ a ) = ( a ∙ b ) ∙ a {\displaystyle a\bullet \left(b\bullet a\right)=\left(a\bullet b\right)\bullet a} for any two elements a and b of the set. A magma (that is a set equipped with a binary operation...
I think this is what your anti associativity is trying to say
Other interesting thing is, what happens after reaching the deadweight $\square$. What is $\square a$ for any $a$?
 
$\square a$ isn't defined in the axioms, you could go anywhere. It's just that $\blacksquare$ is the only way to get to $\square$ and always takes to $\square$
 
ah I see
Also glad that your divisibility axiom does not stress it has to be unique a,b else you will have problems as $\blacksquare b = \square$ for any $b$
 
10:42 AM
Anti-associativity is saying that it satisfies the flexible identity, but is otherwise never associative.
Also, yeah, I had to be careful with anti-associativity, too.
 
Hi. Is $f : \mathbb{R}^n \to \mathbb{R}^m$ always in $C^1$ if and only if its partials $\partial_j f$ exists and be continuous?
 
hmm...
 
I believe so, ChoMedit. I'm actually going over that stuff in a class this semester, so I'm still learning it.
(In other words, don't take my word for it)
 
The interesting sets that will give you a lot of information about Brick will be the set of all g,h such that $gh= \blacksquare$
Also anti asosciativity have interesting interactions with $\blacksquare$ for example if $ab=\blacksquare$ then $(ab)c=\blacksquare c = \square = a(bc)$. By deadweight, it means $a=\blacksquare$ or $bc=\blacksquare$
 
11:04 AM
Well, anti-associativity means that $\square\neq a(bc)$ unless $a=c $
Also, yeah, there must exist a pair which takes you to $\blacksquare$, by divisibility, and I agree, that's an interesting feature.
Of note: it is impossible to have a brick of fewer than 3 elements. Can you achieve a 3 element brick?
 
Truchet tiles FTW
 
@AkivaWeinberger but I can :P
 
I need to try and sleep soon.
 
11:22 AM
Lang makes Dummit and Foote look like child's play.
 
11:45 AM
Brick with two elements. In detail:
Let $x$ be anything
$\blacksquare x = x \blacksquare = \square$
$\square\square = \blacksquare$
$(\blacksquare\blacksquare)\blacksquare = \blacksquare(\blacksquare\blacksquare) = \square$
$(\blacksquare\square)\blacksquare = \blacksquare(\square\blacksquare) = \square$
$(\square\blacksquare)\square = \square(\blacksquare\square) = \blacksquare$
$(\square\square)\square = \square(\square\square) = \square$
$(ab)c\neq a(bc)$
Let (a,b,c) be the associator, i.e. the map $(ab)c \mapsto a(bc)$. Then:
$(\blacksquare,b,c) = (\square \to \square c)$
 
12:02 PM
You didn't cover $\square (\square\blacksquare)$, but I believe you're right, actually.
 
I will cover those cases eventually, I am still computing the associator. It takes time
The associator, similar to the commutator, tells you whether associativity or its wekaer version holds. If a given associator is the identity map, then that associative law for that example holds
Usually, it only appear in lie algebras where it is defined as $(ab)c-a(bc)$, but I generalise it so it can be applied to any magmas
$(a,\blacksquare,c) = (c \to a)$
$(a,b,\blacksquare) = (\square \to a\square)$
$(\square,b,c) = (bc \to \square (bc))$
 
12:30 PM
how do you write the notation for a bijection
 
$\cong$ ?
 
Isn't it a double arrow?
$\to$
actually this is it $\mapsto$
I wonder what a common example is for a bijection between areas is
given by integrals
 
o f888
typo
$(a,\square,c) = (a\to c)$
 
12:51 PM
So... what is the context of doing this? It looks like something fundamental in mathematics.
 
how can I prove associativity of addition in $\mathbb{F}_p$ (prime field) if $a+_p b = \gamma_p(a+b)$, where $\gamma_p$ is remainder of division a+b by p?
 
We are exploring a kind of flexible magma known as a Brick, and I am trying to calculate all its associators to characterise the Brick with 2 elements
 
1:12 PM
$(a,b,\square) = (ab \to \square b)$
Thus the Brick of two elements is fully characterised by the following:
1. $xy=yx$
2. $\blacksquare x = x \blacksquare = \square$
3. $\square^2 = \blacksquare$
4. $(\blacksquare,b,c) = (\square \to \square c)$
5. $(a,\blacksquare,c) = (c \to a)$
6. $(a,b,\blacksquare) = (\square \to a\square)$
7. $(\square,b,c) = (bc \to \square (bc))$
8. $(a,\square,c) = (a\to c)$
9. $(a,b,\square) = (ab \to \square b)$
 
 
2 hours later…
3:27 PM
Leaky's zero reciprocal ring. Attempt at reforming it:
Given zero reciprocal axiom: $\frac{x}{0}=0$ for all $x$, compute:
$\frac{1}{0}+1 = \frac{1\cdot 1 + 1 \cdot 0}{1\cdot 0} = \frac{1+0}{0} = \frac{1}{0} + \frac{0}{0}$
we want $\frac{x}{0} + \frac{y}{z} = \frac{xz+y0}{0z} = \frac{y}{z}$
meaning $\frac{xz}{0z}+\frac{y0}{0z} = \frac{y}{z}$
Assuming $z\neq 0$ we have $\frac{x}{0} + \frac{y0}{0z} = \frac{y}{z}$
$\frac{x}{0}= \frac{y}{z} - \frac{y0}{0z} = \frac{0y-y0}{0z}$
$\frac{0y-y0}{0z} = \frac{x}{0} = 0$
which is not working because $1$ is a two sided additive identity. Since two sided identity is unique, $1=0$
To remedy this, we need to modify $\frac{a}{b}+\frac{c}{d} = \frac{ad+cb}{bd}$
Specifically we don't want $\frac{x}{0}+1=\frac{x}{0}$. Thus define a map $m: X \to X$ such that:
$\frac{a}{b}+\frac{c}{d} = \frac{ad+cb}{bd} + k$
What we need to do now is to find $k$
$\frac{a}{0}+ \frac{c}{d} = \frac{ad+c0}{0d} + k = \frac{ad}{0} + k$
specifically, we want $\frac{ad}{0} + k = 0+ k = k = \frac{c}{d}$
Likewise, we also want: $\frac{a}{b} + \frac{c}{0} = \frac{a0+cb}{b0} + k = \frac{cb}{0} + k = 0+k = \frac{a}{b}$
And thus finally:
$$b=0 \lor d=0 \implies \frac{a}{b}+\frac{c}{d} = \frac{ad+cb}{bd} + \frac{a}{b}+\frac{c}{d}$$
which really does not do anything useful
 
 
2 hours later…
5:28 PM
How can I find k if I know that k+1, 2k+1, 3k+1 and 4k+1 are prime numbers?
 
6:24 PM
Any ideas?
 
6:57 PM
Problem: Let $\{f_n\}$ be a sequence of nonnegative measurable functions that converges pointwise on $E$. Let $M \ge 0$ be such that $\int_E f_n \le M$ for all $n$. Show that $\int_E f \le M$. Verify that this property is equivalent to the statement of Fatou's Lemma.
It's clear that Fatou's lemma implies the above statement. But why does Fatou's lemma follow from it? Is this mistake in my book? In Fatou's lemma there is nothing about the $\int_E f_n$ being uniformly bounded.
 
7:15 PM
@user193319 we want to show Fatou's lemma, so let $g_n$ be a sequence of non-negative measurable functions. Let $f_n=\inf_{k \geq n} g_n$, then $f_n$ is again measurable and non-negative and we have that $f_n \to \liminf g_n:=f$ (monotonously).

Since we have $f_n \leq g_n$ for all $n$, we have $\liminf \int_E f_n\leq\liminf \int_E g_n$.

If $\liminf \int_E f_n = \infty$, then there is nothing to show. Suppose that $\liminf \int_E f_n = M < \infty$, then from monotonicity, we have that $\int_E f_n \leq M$ for all $n$, so by the assumed property, we have $\int_E f \leq M = \liminf \int_E f
 
7:27 PM
Hello!
 
@Daminark Hey! How's it goin?
 
Everything's doing alright, how about you?
 
I'm doing alright as well.
 
Anything new?
 
7:49 PM
hi @Daminark
 
hey guys, what do they mean exactly when they talk about a metric that is induced by a norm? does it always have to mean that we're talking about "the" induced metric, ie $d(x,y)=\Vert x-y\Vert$, or does it mean that the metric is a composition of the norm-function (and sth else)?
 
@ShaVuklia it's precisely "the" induced metric $d(x,y)=\|x-y\|$
 
well I know they usually mean that, but when they say that a norm can't always be induced by a metric, they don't mean that we have to look at $\Vert x\Vert=d(x,0)$ right?
they mean that we could just look at any composite function of the metric, right?
 
Hey Mathein!
 
@ShaVuklia what do you mean by "a norm can't always be induced by a metric"?
not every metric is induced by a norm, but for every norm, there's an induced metric and you can recover the norm from that
 
7:55 PM
my problem is that the argument that bounded metrics can't induce a norm, because such a norm would lack the homogeneity condition, is that it feels hand wavy for me, as it's not clear to me why we wouldn't be able to figure out a function on our bounded metric, that would still yield a norm
 
@ShaVuklia the statement "a bounded metric is not induced by a norm" means that if $d(.,.)$ is a bounded metric, then there is no norm $\|. \|$ such that $d(x,0)=\|x\|$ for all $x$
I think you're interpreting too much into the word "induced by"
 
but why does it have to be $d(x,0)$? why wouldn't we be looking at other functions of the metric to get this norm?
 
because that's how you recover a norm from the metric it induces
it's just a matter of definition
 
well apparently not, because sometimes it fails?
 
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