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2:00 PM
why should I make a distinction
 
Is the empty set finite ?
Is 0 a natural integer ?
 
okay, we can generalize max
to an element of the set in question, that reaches the sup
 
well, I'm saying that my preferred definition of max and sup agree for non-empty finite sets, but not for the empty set
 
then this presupposes inhabitedness
 
precisely
 
2:01 PM
but why accept this for inf then
 
a max should be an element of the set larger than any other element and the empty set doesnt have elements
 
then you should reject inf for the empty set as wekk
 
no, I reject min for the empty set
inf and sup work fine in any case
 
@Astyx this is really not a definitional thing,
@Thorgott ah yeah sorry, min
 
yeah, the empty set is finite, we should all agree on that
 
2:03 PM
totally french to argue about that
 
:(
 
gottem
 
what things get easier when you reject min/max for the empty set
extreme-value theorem?
 
pretty sure this is more about min/max having to be in the set you're looking at whereas inf/sup not having to be in the set you're looking at
 
dunno, I never had to make a distinction
consciously, at least
 
2:07 PM
give it a shot
 
why
 
could be good for learning purposes
 
stop trolling me
lmao
 
I'm not saying anything gets easier
it's just what I believe is right
 
smh really
I thought you had any reason at all
any pragmatic one
I blindly accept 0^0 = 1 for series to work
 
2:10 PM
so do I
also there's precisely one function from the empty set to itself
 
@Thorgott I was really hoping no one mentions this
 
That's undeniable
 
but it's the correct justification
 
the real number 0 is not the empty set
facts and logic
 
The integers are not a subset of the real numbers
 
2:12 PM
why should I care about permutations in a frickin power series
I accept 0 factorial = 1 on that basis, but 0^0 is shaky
 
@user2103480 this is why everyone hates set theorists
 
@Thorgott 90% of the people that mention this are type theorists
and people that read about HoTT on reddit
 
someone who is neither can't tell the difference
 
someone who is neither still feels offended
we are talking about ourselves in third person right
 
I learned type theory encapsulated topology
 
2:17 PM
grrr only because topologists try to hijack the area
type theory encapsulates inner logics of (infinity?) categories
 
No, but actually because IT people were struggling very hard to answer questions that seemed "simple"
 
Which questions do you mean
 
You can do homotopy on type theory
 
so similar setup as a little while ago, $k$ algebraically closed of characteristic $2$.

Is $f'' = 0$ for any $f \in k[x]$? I think so.

Also, $f(x) = \Sigma_{i = 0} a_i x^i$, $f'(x) := \Pi_{i = 1}^t ((x-b_i)^{r_i})^2$ is true.

Given this, why would $\alpha_i = \frac{\sqrt{f(b_i)} - \sqrt{f(x)}}{(x - b_i)^{r_i}}$ be integral over $k[x]$?
 
From my (vague) understanding, questions as defining equality between types, and equality between equalities of types etc
Which has concrete applications to type checking programs and stuff
@BigSocks Deriving $x^{n+2}$ twice gives $(n+1)(n+2)x^n$ and one of $n+1$ and $n+2$ is even
 
2:21 PM
right, that's why I thought so, that's good.
 
Simplicial sets and other topological structures give semantics for martin-löf type theory + univalence so if one reasons within the latter, one can not infer false statements (in the language of type theory) about these structures
 
You can also use your previous question twice
 
yeah I just thought they were assuming it, but it's actually a consequence of char $2$, which is neat I guess
 
"Encapsulate topology" is a strong statement though
 
Why don't Mobius strip lovers need arguments?
 
2:23 PM
granted
 
ncatlab.org/nlab/show/Awodey%27s+proposal this is the more or less precise form of what HoTT encapsulates
 
Because they are all on the same side
:]
 
@Semiclassical deep
 
@user2103480 cool!
 
2:28 PM
@user2103480 Damn Ayoade got a long way from the IT crowd
 
@Astyx use my previous question twice? for the integrality of
$\alpha_i = \frac{\sqrt{f(b_i)} - \sqrt{f(x)}}{(x - b_i)^{r_i}}$ over $k[x]$?
 
Should've stopped before it was too late
 
something something homotopy type is determined by the fundamental infty-groupoid
 
@BigSocks no, for showing f''=0
 
oh lol yeah
 
2:31 PM
@Thorgott please no
big urs schreiber vibes emanating here
 
"Let $a,b,c \in \mathbb{Z}. Then at least one of the numbers a + b, a + c,$ and $b + c$ is even."

If we wanted to prove this by contradiction, we would prove the statement:

$\forall a,b,c \in \mathbb{Z}, a + b$ odd $\land b + c$ odd $\land a + c$ odd.

But what is the contrapositive of this statement?
 
52
Q: Intuition behind Snake Lemma

TunococI've been struggling with this for some time. I can prove the Snake Lemma, but I don't really “understand” it. By that I mean if no one told me Snake Lemma existed, I would not even attempt to prove it. I believe I am missing some important intuition that tells me that the lemma “could” be true b...

All these diagram chasing lemmas (snake lemma, 3x3 lemma, four lemma, five lemma, etc.) follow directly from the "salamander lemma" due to George Bergman, see salamander lemma.

And that is pretty transparent. It is so transparent that for instance it is immediate to see (which no textbook ever mentions) that there are just as easily 4x4 lemmas, 5x5 lemmas, 6x6 lemmas. etc. In other words: once you see the simple idea of the salamander lemma, you can come up yourself with more such diagram chasing lemmas at will.
The corresponding nlab article:
me, having seen the snake lemma shortly before and knowing singular homology for like two days:
 
The ice wyrm lemma
 
@politeproofs Maybe: If $a+b,a+c,b+c$ are all odd integers, then at least one of $a,b,c$ is not an integer.
 
2:35 PM
I'm sure this is all just diagram chasing but nonetheless this is completely opaque
 
@Semiclassical But that doesn't even make sense to me.
 
what about it doesn't make sense?
 
Why would that be it? I don't see why that would mean at least one of $a,b,c$ is not an integer/
 
write it all out, add 2 equations, find the third one on one side, LHS is odd, RHS is even
 
Because the negation of "a+b,b+c,a+c are all even" is "at least one of a+b,b+c,a+c is not even"
 
2:38 PM
If $a,b,c$ are all integers, can it be that none of $a+b,a+c,b+c$ is even?
 
that said, i'm not sure i'm dealing with the universal quantifier properly
 
yeah man, the snake lemma is pretty clear once you understand spectral sequences
 
@Semiclassical That's not even what I wrote
 
erm. you're...right
wait
 
@Thorgott it's the most straightforward explanation
 
2:40 PM
the negation of "at least one of a+b,b+c,a+c is even" is "none of a+b,b+c,a+c are even"
 
Indeed. That's what I wrote.
I claim that is the contradiction that we would need to prove, if we wanted to prove the original statement.
 
So the contrapositive should be "If none of a+b,b+c,a+c are even, then at least one of a,b,c isn't an integer."
 
@Semiclassical I don't follow. What are $a+b, a+c, b+c$ elements of then?
 
yeah, that's the chink in my statement
I figured I wasn't dealing with the quantifier correctly
you can take the case of them being real numbers but I'm not certain that's legit
 
Yeah, you're right about the fact that it doesn't seem legit.
 
2:44 PM
(as in, "If a,b,c are real numbers such that none of a+b,a+c,b+c are even integers, then a,b,c can't all be integers." that's a fine statement but i'm not sure it's the contrapositive)
 
Since saying they're elements of R seems rather arbitrary, as "even" and "odd" are not really defined in R, but in Z
 
I'm a bit puzzled how to think of this in $P\implies Q$ form, come to think of it. Verbally I see it but it seems like the correct statement is just $\forall a,b,c\in\mathbb{Z}(a+b\in 2\mathbb{Z}\vee b+c\in 2\mathbb{Z}\vee a+c\in 2\mathbb{Z})$
 
Sounds like you need to read an intro proofs book, just like me. ;)
 
contrapositive should be if all these sums are even, it is not the case $a, b,c \in \Bbb Z$
 
that's what I said to begin with
 
2:48 PM
why was it wrong
 
@BigSocks Because what are they then?
 
How do you describe a+b,b+c,a+c? What are a,b,c elements of?
 
could be rationals idk
 
No, again
Rationals is very arbitrary
 
I don't make the rules, that's the contrapositive
I didn't say they were but they could be
you have a diophantine predicate involving $a,b,c$
 
2:49 PM
could take them to be reals as well, for that matter, which makes it seems as if the contrapositive is not unique
 
Clearly it's not the contrapositive since the contrapositive has to still make sense, but we have unquantified things in your statement
 
it's $D(a,b,c)$
the antecedent is $a,b,c \in \Bbb Z$
so you just do $\neg D(a,b,c) \Rightarrow \neg [ a,b,c \in \Bbb Z]$
 
But the antecedent isn't $a,b,c \in \mathbb{Z}$?
 
A contrapositive is "$\forall a, b, c, \in \Bbb Z$, (a+b odd and a+c odd and b+c odd )$\implies$ False"
 
The $a,b,c \in \mathbb{Z}$ is a quantifier for a,b,c
I don't see how it's an antecedent.
It's like saying $\forall x \in S, P(x) \implies Q(x)$.
 
2:53 PM
boddanda
 
$\forall x \in S$ is not an antecedence here.
 
i don't know why that amuses me
 
@Semiclassical What?
 
lol
 
momentary typo in what Astyx had
 
2:53 PM
Oh okay, sorry didn't see
 
yeah, it went quick
 
The fastest latex correction in the west
 
I am going to start my undergrad soon, so I have to learn this basic logic stuff before I do.
Help me out, please. :D
 
@politeproofs do you not agree with what I wrote ?
 
2:55 PM
is $\forall x\in S (P(x))$ equivalent to $(x\in S)\implies P(x)$?
 
@Semiclassical From my intro to basic math proofs book, I would say so
@Astyx Well, I don't see why it would imply false.
 
Because P is equivalent to $True \implies P$
 
then one would think that the correct contrapositive is $\neg P(x)\implies \neg (x\in S)$
hrm
what's the latex notation for negation
 
neg
 
2:57 PM
But how do you negate $P(x)$ without knowing the domain of $x$
 
I'm not sure you can instantiate elements out of thin air though
 
Sounds like we all need to read an intro to proofs book. :(
 
for reference, i'm a physics guy
so i'm never so happy as when i can shut up and calculate
 
@politeproofs But why do you not agree with what I said ?
 
@Astyx You haven't justified why it implies false
 
2:58 PM
I have
Because P is equivalent to $True \implies P$
 
too bad our logician just left, I'm sure this can be made more complicated
 
I think the issue is that I'm not remembering how to deal with quantifiers when doing contrapositives
 
@Semiclassical But I think that it's actually $\forall x \in S (P(x)) \equiv x \in S \implies P(x)$
And then the contrapositive would be, $x \in S \implies \neg P(x)$
 
To define the contrapositive you need to know what implication you're dealing with
The contrapositive is simply the statement that $P\implies Q \equiv \neg Q \implies \neg P$
 
Since the contrapositive of, for example, let a, b be integers. if a + b > 0, then a > -b would be Let a,b be integers. If a ≤ -b, then a + b ≤ 0.
We don't magically turn a,b into real numbers, or rational numbers, or some other magical thing
 
3:00 PM
Here the only implication I can see without expanding the ambiant set of a,b,c is $True \implies P$
 
one assertion I'm seeing online is that the contrapositive of $\forall x\in S(P(x)\implies Q(x))$ is $\forall x\in S (\neg Q(x)\implies \neg P(x))$
 
its contrapositive is $\neg P \implies False$
Which is what proof by contradiction is
 
@Semiclassical That's exactly my point
 
in which case the form of your statement, per Astyx's point, is that the statement is $\forall a,b,c \in S(\top\implies P(x))$
 
Grr. Why T, though?
 
3:02 PM
if you mean notation, it's because I dunno how to do "true" in latex
other than \text but that's ugly
 
I'm gonna channel my inner Ted for a second and remark that you are very likely making this needlessly complicated by writing it in terms of opaque symbols
 
How are you meant to look clever if what you say is not opaque ?
 
yeah, $\forall x \in S [P(x)] \leftrightarrow \forall x [x \in S \Rightarrow P(x)]$
 
as a matter of logic, though: you've specified the domain of a,b,c as even integers. once you've done that, it's a tautology that a+b,b+c,a+c are even
so you don't need any premise other than "true"
in which case, per Astyx, the correct contrapositive is $\forall a,b,c\in S(\neg P(x)\implies F)$
 
I see. I guess it makes sense. But that basically means contrapositive = contradiction in this case
 
3:05 PM
yeah
 
I don't think that's right
 
But the problem is badly phrased, because you never take the contrapositive of a statement, but of an implication
 
Okay, that's fine. Thanks for the help, everyone.
@Astyx It was just my idea to take the contrapositive of this.
 
i guess the upshot is that, if your statement is a tautology when expressed as an implication
 
Because ultimately, it could be done, right? But I couldn't tell for sure how to do it correctly
 
3:05 PM
then the contrapositive is necessarily that the contradiction is false
 
yeah you somehow have to phrase it as an implication and the only way to do that is to interpret universal quantification as containment of elements in a set
 
As I already wrote above, the contrapositive is the logic equivalence between $P\implies Q$ and $\neg Q\implies \neg P$
 
@Astyx right, and we're specifying to the case when $P$ is true and therefore $P\implies Q$ is a tautology
so the question is basically "how do you take the contrapositive of a tautology"
 
It depends what you mean by tautology
 
and I don't think there's anything wrong with the initial thing. saying something is not in a set does not say where they are. I don't think there are any ontological debts to be paid
 
3:07 PM
one way to get around it is probably to modify P(x) so that it already has a domain
which i take our rational/reals thing to be
 
@Semiclassical Have you taken measure theory, as a physicist?
 
taken? no
been trying to learn a bit of it myself tho
 
Read a book, whatever
 
mostly so that i have a grasp on measure-theoretic probability theory
Kolmogorov foundations etc
I do QM stuff, especially stuff in the realm of history
so having a grasp on foundations isn't a small thing
(I'm not very good at it.)
 
At this point in physics, not understanding the maths is a plus amirite
 
3:10 PM
Hm, I need to deal with $(-\Delta)^\gamma$, where $\Delta$ is the laplacian and $\gamma > \frac14$. Is this just the function to the power of $\gamma$ pointwise? Or are there other sensible definition for this
 
@user2103480 context?
that could be some kind of fractional derivative
the upshot is that you define $(-\Delta)^\gamma f$ in terms of what it's Fourier transform looks like
 
Not much more context. It's a simple setting so we look at functions in "$L^2(0,1)$" (I'm not sure whether this being an open interval is intention) for which the laplacian on $[0,1]$ with dirichlet boundary conditions is defined
 
hmm. my impulse would be that it's a fractional derivative
 
And we should prove that this fractional laplacian is a hilbert-schmidt operator
ah this looks sensible
damn prof, define the stuff
 
3:14 PM
@Semiclassical Is there anywhere where I can ask you that's slightly more ontopic about physics textbooks?
 
the obvious hot-spot is the physics chat room: chat.stackexchange.com/rooms/71/the-h-bar
but here is probably fine
 
@Semiclassical thanks btw
 
np
@user2103480 waving my hands a bit, is it obvious how "finite H-S norm" translates from $f$ to its Fourier transform
if so, then it'll presumably just amount to "prove it on the Fourier transform side"
 
I have not tried yet. I'm watching a recording right now and the prof states that minus the laplacian is positive definite so one can take arbitrary powers and I'm not sure how that works
 
@LHC2012 Please describe in complete detail
 
3:22 PM
"Taking the root" of a pos def operator I know, but I haven't seen any generalizations of that
 
Why should the first derivative be 0.If it is zero then why check the second derivative?
 
can't you do the same thing for arbitrary powers as for roots
 
Apparently?
 
not having a definition doesn't help here
 
Who was the logician that just left, by the way?
The one you referred to earlier who was here
 
3:29 PM
@politeproofs Did u mention me?
 
6
Q: Fractional powers of positive self-adjoint operators

zhangConsider two positive unbounded operators $A$ and $B$ densely defined on a Hilbert space $H$ self-adjoint on a domain $\mathcal{D}(A) = \mathcal{D}(B) = H_1$. By the spectral theorem, we can define the fractional powers of $A$ and $B$ as self-adjoint linear operators on $H$. My question is, is $\...

 
I don't think so?
 
By the spectral theorem, apparently. I'm getting closer
 
Or was that supposed to be a joke? In which case, it wasn't too funny.
 
I think $(-\Delta)^\gamma$ refers to the operator $\tilde f\to\tilde k^{2\gamma}f$ in Fourier space
The point being that in general, the action of an auto adjoint operator is isomorphic to the multiplication by a function in a certain function space
 
3:33 PM
@politeproofs impolite proofs
 
@user2103480 I'm only polite during proofs. ;)
 
For $-\Delta$, this function is $k^2$ and the space is the fourier space
As a matter of fact, for any function on $f:\Bbb R_+\to \Bbb R$ you can define $f(-\Delta)$ (because $-\Delta$ is positive definite)
(if my memory doesn't fail me completely)
 
You need to phrase this a tad bit more down to earth since my functional analysis knowledge mostly ends after the spectral theorem for compact, self-adjoint operators
 
What's your statement for the spectral theorem ?
 
I honestly don't know for this case of densely defined unbounded positive operators. I only know there exists a spectral theorem which apparently quickly gives the construction of the power of the operators
I'm following the SE link above and what the statement is, is what I'm currently looking for
 
3:41 PM
The most general statement I know says that an auto adjoint operator $(A, D(A))$ on a separable Hilbert space $\mathfrak h$ behaves isomorphically to the multiplication by some real valued function $a\in L^{\infty}_{loc}(B, d\mu)$ on $L^2(B, d\mu)$
 
That may even be too general
 
Where B is a subset of $\Bbb R^d$ for some $d$
 
better than it is for physicists, including myself. a footnote on a book draft i'm involved in:
"Physicists tend to use these terms interchangeably but there is a subtle difference between self-adjoint and Hermitian operators. When in the 1960s, a mathematician (Kurt Otto Friedrichs of the Courant Institute in New York) mentioned to Heisenberg that another mathematician, von Neumann, had helpfully clarified this difference for physicists, Heisenberg purportedly asked him: ``What's the difference?''"
(my own answer to that question is roughly "boundary conditions")
 
So in the specific case of $-\Delta$, the $a$ in question is $k\to k^2$ and B is the Fourier space
 
Is there any way to get the power of the operator given an eigenvector basis? There is the obvious easy eigenvector basis of sines
 
3:44 PM
That means that $\overline{-\Delta f} = k^2\bar f$
 
Behaves isomorphically in the sense unitary equivalence?
 
Now if you want to define $u(-\Delta)$ for some function $u$, this will be $\overline{u(-\Delta)f} = u(k^2)\overline{f}$
 
and what is $k$ here?
 
Oh sorry, yeah that's not clear
k is the variable
 
frequency?
 
3:46 PM
If you want, yes
 
in physics you'd say that $x$ is position and $k$ is wavevector
or $t$ is time and $f$ is frequency
 
What I shoudl write is that $\overline{u(-\Delta)f}$ is $k\mapsto u(k^2)\overline{f}(k)$
 
specializing to the 1D case momentarily, i'd want it to be the case that $(-\Delta)^\gamma \sin(kx)=k^{2\gamma} \sin (kx)$
 
In your specific example $u:k\mapsto k^{\gamma}$
 
i'm not wholly sure my statement makes sense tho
 
3:48 PM
(I too thought this was dark magic when I first learned it)
 
and the overline is the fourier-transform?
 
Yes
 
so what, do I fourier transform and then back-transform to obtain the fractional thing
 
I'm not sure what you want to do
 
if you're trying to prove that $(-\Delta)^\gamma$ is a H-S operator, then i still think it makes sense to prove that its Fourier transform is a H-S operator
and then transfer that statement back to the original space
 
3:52 PM
I just want to find a defintion of the fractional operator that I can work with. Since you defined $f(-\Delta)$ using the fourier-transform, I assumed I get the actual operator by transforming this back
 
which I think is plausible, because going from position space to wavevector space usually plays nicely with the norm
 
Yes you do, but it's way nicer to work in Fourier space
 
@Semiclassical that sounds indeed like a plausible and probably pretty nice, high level approach
I'd need to know a few results that ensure that this works, though. I may try to just figure out what happens to the basis vectors to define this shite
thank you people in any case!
That helped a lot
 
what's the latex symbol for logical equivalence. not the three bars but the left-right arrow
(and not \leftrightarrow)
 
$\iff$?
 
3:55 PM
\iff
 
Working with a basis maybe makes hilbert-schmiddity easy
I reserve the rights for that adjective
 
the whole momentum-space vs. position-space representations of the wavefunction in QM basically revolves around the fact that $\int |f(x)|^2\,dx<\infty \iff \int |\overline{f}(k)|^2\,dk<\infty$
 
Those are equal right ?
 
which i think is all you need here
depends on your convention
 
3:57 PM
Yeah right
 
which i hate but i have to leave open
i do prefer $\int |f(x)^2\,dx=\int |\overline{f}(k)|^2\,dk$ though
 
itô- and fourier-isometry are maybe my favourite analytical facts
 
Before trying to unify QD and gravity, they should try and unify conventions for the Fourier transform
 
never happen
 
impossible
 
3:58 PM
i mean, the sad fact is that there's no way to write the Fourier transform conventions without it occasionally being gross
 
Given circle of radius d, how do i find jdf of distance from origin?
Say d is distributed exponential with 2a
 

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