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02:58
@user346760 yes?
 
2 hours later…
04:52
Is this working?
depends on what you mean by 'working'
It’s working! Yay! I missed you all. Been 13 years.
Jasper Loy and Asakiri are cool. Asakiri isn’t his name. He’s a set theorist. Think he knows JM. Can’t remember. Quaicjiu Yuan is cool, too.
And Bill Dubuque (water under the bridge)
I’m sure no one remembers me, though. I’m easily forgotten.
Anyway, see you later, folks
Schwartz reflection principle in the unit circle can be proven using power series expansion..?
$f\in\mathcal{H}(\Bbb D)$ then $1/\overline{f(1/\bar{z})}\in\mathcal{H}(\Bbb C\setminus\overline{\Bbb D})$
Just saying naively ${\partial\over\partial\bar{z}} =0$
05:19
with a distinct user name how could one be so easily forgotten?
05:34
@copper.hat All personality.
@onepotatotwopotato So how is this power series?!?!
@TedShifrin I mean expressing the reflection function as a quotient of some power series and saying 'well there's no $\bar{z}$ term here, so holomorphic'
05:48
I wouldn’t mention power series. Of course, you have to look carefully at boundary points.
@TedShifrin Then how? Using the definition of holomorphic function?
The original Schwartz reflection principle in a symmetric domain w.r.t. real line can be proven easily using power series so I was expecting something similar here.
 
2 hours later…
07:24
If I have a manifold $M$ and an open set $U$ of $M$. It doesn't necessarily follow there is a coordinate chart $\phi$ defined on $U$ right?
27
Q: How do you prove Well-Ordering without Mathematical Induction? (and vice-versa)

Alexy VincenzoHere is my attempt to prove the Well-Ordering Principle, i.e. that any non-empty subset of $\Bbb N$, the set of natural numbers, has a minimum element. Proof. Suppose there exists a non-empty subset $S$ of $\Bbb N$ such that $S$ has NO minimum element. Define $A = \left\{n\in \Bbb N : (\forall s...

I don't know why well ordering and induction not equivalent?
I think Induction implies well-ordering
But don't know why well-ordering doesn't imply induction
@leslietownes i know my question is super open ended in the first place, but what information is required for there to be a coordinate chart on any arbitrary open set $U$?
I don't get it why "Suppose $P(0)$ is true, and $P(n+1)$ is true whenever $P(n)$ is true. If $P(k)$ is not true for all integers, then let $S$ be the non-empty set of $k$ for which $P(k)$ is not true. By well-ordering $S$ has a least element, which cannot be $k = 0$. But then $P(k-1)$ is true, and so $P(k)$ is true, a contradiction." is wrong. Why is P(k-1) wrong?
lemon: i don't know. note that taking U = M this includes or is the question of when an n-manifold embeds in R^n, which is already not elementary even for surfaces.
if you don't want it to hold for all U but just want to know 'how big' U can be relative to M without being the whole thing, that also seems interesting, but i don't know.
math.stackexchange.com/questions/322027/… is semi related (maybe not what you are thinking about) but involves a smooth structure.
07:40
Does anyone know why in Rieman normal coordinates one requires an isomoprhism $B$ determined by an orthononormal basis $(b_i)$ for $TpM$? That is Normal Coordinates defined by the coordinate chart $B^{-} \circ Exp^{-1}$ (assume Exp is a local diffeomorphism) where $B$ is defined by $B(x^1\dots x^n) = x^i b_i$ (all notations are borrowed from Jack Lee (p131). It seems to me orthonormal isn't that important.
@leslietownes I just realized my problem. $U$ (doesn't have to be all the way $M$) is at least the intersection of two open sets that ARE from coordinate charts. BUt none of those maps $\phi_i$ have to be defined on all of the set $U$.
 
3 hours later…
10:25
anyone?
is it illegal to take induction reverse?
@NotTfue what do you mean by "induction reverse"? Do you have an example?
Suppose P(0) is true, and P(n+1) is true whenever P(n) is true. If P(k) is not true for all integers, then let S be the non-empty set of k for which P(k) is not true. By well-ordering S has a least element, which cannot be k=0. But then P(k−1) is true, and so P(k) is true, a contradiction.
I was thinking why is this wrong P(k−1) ?
The comment section got me confused
"@AndrewH.Hunter You are correct, and the proof above is wrong. Induction and well-ordering is not equivalent."
10:44
This is a proof by contradiction, not induction in reverse. The argument is more complicated than it needs to be this way, but it works.
hello. maybe someone happens to know what Pr means here? math.stackexchange.com/questions/503245/…
seeing this for the 1st time
I know it is contradiction but didn't understand why it is wrong but seems justified.
11:03
@Peter judging by the context it must be conditional probability, but it's strange way to denote that. maybe the author meant projection on sigma-algebra generated by the latter which may lead to the same statement
11:33
I would assume Pr means probability, yes
the vertical bar is standard notation for conditioning
@Lemon that condition simplifies the components of the metric at $p$
11:50
Not complaining (sorta complaining…$ but it’s hard to read thin words in a sentence without a clear magnifying glass or Bette glasses
better glasses*
@copper.hat I don’t know if I know what you meant.
@robjohn can you advise me how to fix up my tensor question? I b struglin
 
1 hour later…
13:13
Who wants to join in the search of a twin prime pair ?
What is the smallest $s$ such that $$10^{5000}+9^{5000}+s\pm1$$ is a twin-prime pair ?
14:11
What is the fascination with twin primes?
14:49
@TedShifrin One might be walking with a bunch of little canines, one of them happens to be a female and, well, there's that... really gets one to appreciate the collective efforts aimed at the common goal of synergizing all instances of such cases, doesn't it?
 
2 hours later…
16:26
Thank you @robjohn
@TedShifrin can you give an example of problem in lin alg
where
one can naturally think
"oh if i had a alternating multilinear function on matrices i would solve this problem"
I.e. Is there a synthetic motivation of the det
16:53
not gonna happen
@Thorgott
why?
cause it's a silly idea
it's not how mathematics develops
if you knew what you needed to a solve a problem before solving it, there'd be almost nothing left to do
so the only way to motivate the det is using volume?
Im wondering if there is a synthetic motivation not a geometric one
@Thorgott
Here's a stupid one, but it is what you deserve. Test (without solving a system of linear equations or using row operations) whether $n$ vectors in $\Bbb R^n$ are linearly dependent/independent.
Asking if $v_1\wedge\dots\wedge v_n = 0$ or $\ne 0$.
how does a multilinear alternating function arise from that?
17:04
It's wedge product or ... determinant.
As I said at some point earlier, the high school motivation for determinants is Cramer's rule. Maybe you should settle for that.
cramers rule only motivates for 2x2 3x3
i like the oriented volume interpretation
No, it works in all dimensions. How could you not realize that?
It works, but how on earth would you motivate it?
The same way you do in the $n=2$ case.
You want the value of some particular $x_i$ when you solve $Ax=b$.
right and then you define the nxn determinant as what?
17:08
The unique alternating multilinear function ...
I think you need to get past this obsession. I'm done with it.
i agree @TedShifrin
i like the volume approach in your lectures
@TedShifrin
If it didn't show up naturally with differential forms and integration theory, I doubt we'd be as interested as we are.
there's plenty of motivation, I am simply objecting to the notion that it should be possible to materialize the right notion out of thin air
in mathematics, concepts are usually best understood in their applications and, in the same way, their applications usually precede their definition in the first place
Yes, abstraction usually follows after some concrete implementation.
only problem is that the natural motivation i get from that is that the det is the unique function preserved under column ops, etc. we can then derive that it is multilinear and alt. but then why most texts start with multilinear and alt. instead of preserved under column ops and all that. @TedShifrin
^from the vol interpreattion
17:11
Because you don't need matrices to talk about multilinearity.
And the volume interpretation is about vectors, not matrices.
I care a lot more about differential forms and exterior algebra than I do about determinants of matrices :D
Except for the Vandermonde determinant, maybe :D
yeah, the exterior algebra is the conceptual approach
@TedShifrin ah cuase it works for matrices in general fields as well
general commutative rings, in fact. Someone made a big point of this last week when you were harping on this.
it's a pretty genius idea in all honesty, but I don't think it's outlandish to attempt and understand a linear map not just by its action on vectors, but also by its actions on parallelotopes spanned by those vectors
I actually knew a lot of the history when I wrote the linear algebra book 25 years ago, but I'd have to reread the historical stuff at this point.
17:20
I don't know much history, but I do know that these ideas go all the way back to Grassmann 178 years ago
he was more or less postulating anticommutativity of the exterior algebra as a consequence of orienting parallelograms
Determinants were first developed (by Cardano!) to solve systems of equations. Leibniz wrote in a letter to L'Hôpital in 1683 that in the 3x3 case the determinant would determine whether $Ax=0$ has a nontrivial solution. Cramer did Cramer's rule in 1750 in an appendix of a treatise on algebraic curves. Lagrange noticed the link with volume later in the 18th century.
Jacobi elevated the theory in 1841.
Surprise, surprise. He "discovered" the Jacobian determinant.
that's the point where the volume interpretation really shines
it gives an intuitive explanation of the change of variables formula, I always loved that
Given 3 normals to 3 planes in a 3d world n1,n2,n3 where n = {a,b,c}, how can I find the origin of this coordinate system?
Normally the origin, o = {0,0,0} but this is true only for the "default" coordinate system
The origin is arbitrary. How can I know from normals to planes?
Im trying to use a projection function, which requires a point, normal to the projected plane and origin. If the normal to the plane changes (i.e the coordinate system changes), wouldnt the origin paramer change as well?
17:28
Go back to lines in the plane. Make your question explicit.
Projecting a point onto a line does not depend on coordinates. But it depends on the geometry (orthogonality).
If you change coordinates and compute both ways you’ll get the same answer.
Im not sure what you mean
The projection of a point onto a line (plane) doesn’t depend on the coordinate system.
Hmm that is kinda weird since the function does get an origin parameter :)
Because you're using equations for the line (plane), so you need vectors and an origin. What I'm saying is that if you change the origin (and get different equations) or change the orthogonal coordinate system, you will get different numbers everywhere but the same geometric solution of your problem.
Just draw some pictures (2D is easier).
Again, since the function gets both normal and origin as parameters (and uses them), this seems weird that changing one or the other wont change the final result.
17:47
0
Q: Riemann Extension Theorem proof question zero set contained in smaller ball

MathematicallyInterested$B_{\epsilon}(0)$ denotes polydisk in $\mathbb{C}^n$, where $\epsilon= (\epsilon_1,...,\epsilon_n)$. Statement of theorem: Assume $f:B_{\epsilon}(0)\subseteq \mathbb{C}^n\rightarrow \mathbb{C}$ is holomorphic and $g:B_{\epsilon}(0)\backslash Z(f)\rightarrow \mathbb{C}$ is holomorphic and bounded....

The formula for the answer looks different. The geometric point is the same.
Try doing a simple example where you move the origin and rotate the coordinate system by some angle.
18:00
@Thor Do you think it's OK for me to "forget" to respond?
18:12
Can any one help with my question?
18:24
If there is a real world condition that may or may not be present, i.e., a medical condition ($C =$ condition, $N =$ no condition), and an indicator signaling a prediction about that condition ($+ =$ condition predicted, $- =$ no condition predicted), then there are four unconditional probabilities, $\Pr(C)$, $\Pr(N)$, $\Pr(+)$, and $\Pr(-)$, and eight conditional probabilities, $\Pr(C | +)$, $\Pr(N | +)$, $\Pr(+ | N)$, $\Pr(- | N)$, $\Pr(N | -)$, $\Pr(C | -)$, $\Pr(- | C)$, and $\Pr(+ | C)$.
In this order, a nice cyclic pattern emerges in the conditional probabilities, whereby one can solve for each subsequent conditional probability by alternating between Kolmagorov's Axiom of Normativity and Bayes' Theorem, with wrap-around at the end.
It is easy to see that there are two degrees of freedom among the unconditional probabilities, with the remaining two being taken care of by Normativity. It is also easy to see that the applications of Bayes' Theorem pull at least one of the unconditional probabilities into the conditional probability cycle.
My question is, how many degrees of freedom exist in such a framework overall? How many probabilities must be given to solve for all of them, and does it matter which ones are given?
@monoidaltransform No. I find it confusing (confused) from the very first sentence.
I guess my question reduces to the following: If $f:B_{\epsilon_1}(0)\subseteq \mathbb{C}\rightarrow \mathbb{C}$ is holomorphic and $f$ has no zeros at $\partial{B}_{\frac{\epsilon_1}{2}}(0)$ then does it follow that $Z(f)\subseteq B_{\frac{\epsilon_1}{2}}(0)$?
@TedShifrin
Well, of course that is wrong.
But the setting here is that we're looking at a hypersurface in $\Bbb C^n$ and we're fixing other parameters.
So the proof starts by assuming that $f(0)=0$ but that $V(f)$ does not contain the $z_1$-axis? So by the identity principle, it cannot contain an open neighborhood of $0$ in the $z_1$-line.
18:41
In the third paragraph how is he sure that $Z(f_w)$ is finite?
Your "rendition" of this proof in your question is just very sloppy.
Yeah, that's why i'm asking about it here. So I can understand it better
Whoever that is didn't define $f_w$ in that paragraph.
Huybrechts, $f_w(z_1)=f(z_1,w)$ for $w\in \mathbb{C}^{n-1}$.
and $w=(z_2,z_3,...,z_n)$.
He's just using the Cauchy integral formula to do this. Why do you care if $f_w$ has any zeroes inside?
18:45
Because how else would he extend it to a holomorphic function on $B_{\epsilon_1/2}$ if not by the Riemann extension of one variable?
Riemann extension doesn't talk about zeroes; it cares only about boundedness.
It doesn't talk about zeroes, but it does talk about finite sets. In particular, if $f:B_{r}(0)- \{a_1,..,a_n\}\rightarrow \mathbb{C}$ is holomorphic and bounded then it extends to holomorphic $B_r(0)\rightarrow \mathbb{C}$
Here $B_r(0)\subseteq \mathbb{C}$, ofcourse.
But he said $f(z)\ne 0$ if $|z_1|=\epsilon_1/2$ and $|z_j|<\epsilon_j/2$ for $j>1$.
Oh, so if we let $|z_1|<\epsilon_1/2$, there will be zeroes, but there cannot be infinitely many by the identity principle.
The zero-set of $f_0$ contains no neighborhood of $0$ in the $z_1$-line.
I still don't see why we can't have zeros of $f_{w}$ in $\frac{\epsilon_1}{2}<|z_1|<\epsilon_1$.
$f_{w}$ is, after all, a map $B_{\epsilon_1}(0)\rightarrow \mathbb{C}$, no?
18:54
@Thorgott well that's one of the implications. BUt I m asking why does it start with an orthonormal basis in the first place? We could've just began with any basis $(b_i)$ and defined an isomoprhism $B(x^1\dots x^n) = x^ib_i$ and still define coordinates on the norml neighborhood and call this "normal coordinate". If $(b_i)$ is not orthonomral does that make B not isomoprhism?
He may be omitting some stuff with the preparation theorem or something. He's assuming that $f=0$ intersects the $z_1$-line only at the origin. So it should just be a continuity argument to know that for small $w$, $f_w$ has no zeroes if we restrict to a small compact set.
@Lemon Of course it's an isomorphism, but you for the applications of normal coordinates it's not convenient. You want the metric to be the identity at the center (for convenience) and to have some nice formulas for curvature, for example. If you pick a random basis, that's a mess.
I don't know, monoidal. My head isn't wanting to do this today.
No worries. I'll post a clearer question on main. Thanks in any case.
You can look at other texts, too.
Yeah, I think i'll look at Griffith and Harris
@TedShifrin oh well, I really wonder what a path is
@Lemon no, it's still an isomorphism, but I don't get your point
the thing that is called "normal coordinates" are called as such, because that's how they're defined
I (and Ted) gave you a reason what makes the ones where the basis is orthonormal special
@Thorgott Didn't it say $g$ was the path?
20:14
@TedShifrin He's still around, but life post-corona has had him extremely busy for quite a while as it disrupted school, work, etc. When life slows down in a couple of years or less he'll be back on to say hi
Thanks for the update.
Well, @Pseudo, if you are in touch with anon, please send him my kind regards.
I definitely will - I didn't realize how interconnected he was on this site until I found your profile/book on your profile and shared it with my math group and he then explained everything about MSE from years and years ago. Definitely a lot and interesting
20:31
Oh, that's bizarre. Well, not that many years ago. I think I've been here around 9 years or so.
That's fair, to me anything before 2015 is years-and-years ago lol
So you knew anon from school?
Yeah, we've met and became good/close friends when he mentored a Putnam/Honors Calculus study group in college, which he still does
I'm sure he did a great job of that. He was quite an effective teacher in here before he spontaneously combusted :P
P.S. Which book of mine are you referring to?
The free PDF one on Differential Geometry
20:40
Ah ... I should have guessed.
21:26
When did I start showing up here? I want to say it was around 2013.
Maybe '14.
21:46
I showed up around the same time.
According to my profile, around April 2013.
About a month ago for me
22:10
May I please have some help with my question about multilinear algebra?
I'm trying to understand what tensor equations look like in abstract axiomatic constructions and I am using the Einstein field equations as an example to understand the concept of a tensor equation.
@Fargle your profile says 2014-08-09
I can only imagine that I was as beloved then as I am now.
That was when you first used chat. That was a couple of months after you joined the math.SE.
Write them in terms of vector bundle language, especially since you want to consider differential operators (which will map sections of one bundle to sections of another).
@robjohn is a spy — nothing gets past him.
I don’t think I remember you before UT, @Fargle.
I started there in '13, so that tracks.
I am older than my behavior betrays!
22:22
You behave?
@TedShifrin I only give out secrets for the right price.
Yeah, but you’re cheap.
@TedShifrin Touché.
23:01
Way too hot here in sunny CA.
23:43
i am melting in albany
Can someone check my understanding of this:

The definition of associates in my textbook says: If F is a field, the units in F[x] are the non-zero constant polynomials. f(x) is an associate of g(x) if f(x) = cg(x) for some c $\neq$ 0, $c \in F[x]$.

Then, this questions asks to list all associates of $x^2 + x + 1$ in $\mathbb{Z}_5[x]$. So since the units of $\mathbb{Z}_5[x] are 1, 2, 3, and 4$, the associates of $x^2 + x + 1$ would be

$$x^2 + x + 1 = (1) \cdot x^2 + x + 1$$
$$2x^2 + 2x + 2 = (2) \cdot x^2 + x + 1$$
Finally read through the proof of Sard
Wow, is that a technical proof
I should review the implicit function theorem
23:59
@UnderMathUate wrong …. $c$ must be a unit, i.e., a nonzero constant.

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