General sum to product formuler not involving circular functions wen
I seem to have narrowed analysis of $e^{-\lfloor\ln b\rfloor} b$ down to finding the relationship of the fractional part of this expression to the fractional part of the logarithm.
What we get is necessarily some $1 + x = e^{-\lfloor\ln b\rfloor} b$ which is interesting considering that the infinite sums available for the logarithm are explicitly of this form.
I wonder... we have $\ln (1 + x) = \ln b - \lfloor\ln b\rfloor$. If we compute the terms $R^n$ as given above for $1 + x$ but with $R = e$, here, $n \leq 0$ for all $n$ which suggests a direct relationship to the fractional part of the RHS as $x = e^{-\lfloor\ln b\rfloor}b - \lfloor e^{-\lfloor\ln b\rfloor}b\rfloor = e^{-\lfloor\ln b\rfloor}b - 1$ to the logarithm itself. There's probably something worth investigating about the logarithm $\ln(1 + x)$, its infinite sum, and its $R^n$ sum.
Has anyone tried computing the limit for certain presumably "nice" respective parts of the logarithm if we take the infinite sum for $\ln(1 + a)$ and modify it to be a sum $\ln(a + b)$ and found anything interesting via the binomial theorem applied to its terms?
Well you have for each term of this function in such case as $\sum_{k=1}^{\infty} \frac{(-1)^{k-1} (a + b - 1)^k}{k}$, and then applying the binomial theorem to each term, we can expand the term for each $k$. I suppose it's equivalent to asking whether or not anything interesting or useful comes out of analyzing $\sum_{k=1} (a + b)^k$, or perhaps the multinomial theorem for our trinomial $a + b - 1$.
In terms of the ways in which it might be simplified or otherwise represented equivalently through the binomial and multinomial theorems when the expressions are fully expanded.
I mean idk... maybe there's a representation here that can be found which we can split into multiple sums with at least one of them having a known closed form behind it that would permit splitting the logarithm into parts of some kind.
The fact that these kinds of hyperubermega transcendental functions that sound like final bosses doesn't make them any less scary you know...
*The Lerch Transcendent: Master of the 8th Dimension Between Worlds* Level: don't bother Health: 😂 Stamina: NaN
Yeah about making them bigger, maybe you might try adding an "expand diagram" button that can enlarge the diagram in-place that makes the card enlarge but makes the other cards force wrap. Make sure it has a quick transition at minimum, though. Instant changes are jarring to the user in general.
Or you might make it bring up a closeable diagram viewer overlay.
Or even simpler: open it in a new page with the diagram enlarged
Which choice of implementation however depends on the objective purpose of this UI and therefore your website.
If it's more of a gallery sort of thing, then opening in a new page wouldn't be appropriate for example.
If it could be for any purpose, then you account for and provide the means for the user to implement whichever choice of possibility they desire since the objective purpose of all UIs is to be a means for a user to bring about some arbitrary end, so everything has to be oriented around that.
And then the rest is just, as a matter of GUI principles as just the same objective purpose as UIs but with graphics, here the practicals to apply consist of 1) directing the focus or awareness of the user to the elements he's looking for, and with regard to what he's looking for, 2) minimize the effort required by the user to find what he's looking for.
Well here principle 2 is applicable. It all reduces to finding information. You want as much information on screen as possible without overwhelming the user.
Hm, well if you can make something like an HTML renderer, you can do whatever you want serverside, then provide an absolute URL to that image representation.
Bassically take a 3x3 grid of objects with grid-like morphism arrangement in an abelian category. The number of equalities is huge and there's no easy way to remember them all. but to rememmber a 3x3 grid is easy
Maybe it's just me, but it seems a lot of times, the pioneer or discoverer of a thing puts in enough effort to get something working, and then no one bothers to improve the thing afterwards... it just gets cemented into society regardless of how well it works (or doesn't).
Phone numbers are still a thing in 2023. Stroads are still built like they are the epitome of road design here in America.
and as perceived from a recent Veritasium video, they look to quantum computers to give them the answer to factoring large prime... residues? I can't quite remember. They give all possibilities, but... have they looked into just applying Fourier arithmetic to the usual stuff and exploiting things like $\frac 1 2 n (n + 1)$?
@DLeftAdjointtoU I mean again, I'd just like to point out that, for example, the 2-adic valuation of the even integers $n$ is $n\land (\neg n + 1)$.
That extends to any number evaluated similarly in higher bases.
The definition of negation for higher bases would have to be modified accordingly.
So then for $b$-adic valuation of $n\equiv 0 \mod b$, $n\land_b (\neg_b n + 1)$
Because the number of trailing zeros of $n$ represented in base $b$ are directly proportional to the number of factors of $b$ in $n$.
See now if I just knew how to algebraically compute the number of digits a number requires for its base $b$ representation, including zero terms interspersed between non-zero terms, ...
But that's why I'm looking into the relationship of $\ln x - \lfloor\ln x\rfloor$ to $x$ itself.
$1$. If $D$ is a special divisor over a compact Riemann surface with degree $2g-2$, then $D\sim Z$ (equivalent). So $D$ is contained in a canonical class. In particular, $D$ is a canonical divisor.
$2$. If $Z = (\omega)$ for some abelian differential $\omega$, then $\Omega(Z) = \{\eta:\eta\text{...
I hope I'm correct
If $f:M\to\Bbb C_{\infty}$ is a meromorphic function then $f(z)dz$ in local coordinate $z$ on $M$ defines an abelian differential. If $\omega$ is an abelian differential and $1$ is an abelian differential with $dz$ for each local coordinate $z$, then $\omega/1$ is a meromorphic function so the coefficient function of $\omega$ defines a meromorphic function. Does it make sense?
The proof shows $Q(\sqrt 2, \sqrt 3)$ is isomorphic to $Q(\sqrt 2 + \sqrt 3)$ as vector spaces over $Q$. But how does that show the fields are equal? It doesn't make any sense to me.
First of all, why do so many algebra proofs not draw a distinction between stuff being equal and stuff being ismorphic? This proof actually shows that these two fields are isomorphic and not equal, right?
uh, it isn't that clearly written to begin with, but i don't think the basic logic of the argument intends to show isomorphism, it intends to show equality
@gewbDog5 You already know that both are subfield of $\overline{\Bbb Q}$, so you only know to show that they contain the same elements to show that they are the same field. Obviously $\sqrt2+\sqrt3\in\Bbb{Q}(\sqrt2,\sqrt3)$, so only the other inclusion is not needed
@gewbDog5 Usually this doesn't matter, but in this case the fields are actually equal
the argument explicitly or implicitly uses that Q(sqrt(2) + sqrt(3)) is a subfield of Q(sqrt(2), sqrt(3)), and also that Q(sqrt(2) + sqrt(3)) is degree-4 extension of Q, and concludes from the apparently known fact that Q(sqrt(2),sqrt(3)) is a degree-4 extension of Q (indeed, with a particular basis) that Q(sqrt(2) + sqrt(3)) = Q(sqrt(2), sqrt(3))
it isn't clear to me how much of that is being proved vs. assumed by the writer of that post
but if F is a finite extension of Q, and E is a subfield of F that contains Q, one way of showing that E = F is to show that [F:E] = 1 or equivalently that [E:Q] = [F:Q]
we're definitely using the fact that E is a subfield of F in this style of argument, it's not just some random other extension of Q that is out there flapping in the breeze
or to be clear, in general, if E and F are just random finite extensions of Q, the fact that [E:Q] = [F:Q] would not be enough to conclude E = F, or even that there is a field isomorphism between E and F
for example even within this example we have [Q(sqrt(2)):Q] and [Q(sqrt(3)):Q] both being 2, while the fields Q(sqrt(2)) and Q(sqrt(3)) themselves are neither equal nor isomorphic
Consider a smooth, closed convex surface $f(x,y)\subset [0,1]^3 $ where $\mathrm{max}(f)=f(0,1)=1$ and $\mathrm{min}(f)=f(1,0)=0.$ Define the collection of level sets of $f$ as:
$$L_c(f)= \big\lbrace (x,y) ~| ~f(x,y)=c\big\rbrace $$
where $c\in [0,1].$
Define the strict sublevel set: $$L^{-}_c(f)...
What exactly is the data here? We have a fundamental system $\mathcal V$ such that the group operation is defined for each $x\in V$ for any $V\in\mathcal V$? If that is the case, how do we define the group structure on the total space $G$? It's clear to me how to define a topology (translating the fundamental system to any other point)
Hm, never mind, I think they mean that given a (discrete) group $G$, we have a topological group iff we have these data
So the (discrete) group operation is in that sense not determined
Is the intuition at least clear? e.g. "a contraction mapping $f$ moves all points closer together, so if you pick any point $p$, then $\lim_{n\to\infty} f^n(p)$ seems like it converges to something"?
@Ajay Okay, so explain it to us. I am happy to ask annoying questions about your explanation. This kind of interrogation is often a good way to solidify your own understanding.
And realize $\langle\sigma_1,\sigma_2,\sigma_3\rangle\simeq\langle\sigma_1,\sigma_2,\sigma_3\mid\sigma_i^2 = (\sigma_i\sigma_j)^3 = 1\rangle$ which is a Coxeter group
Say we have a nonempty complete metric space and a function defined in the metric space. say we have two points that exist in this metric space. If we plug each point into the function and find the distance between them, we see that the distance is less than or equal to the distance between the points themselves times some constant.
Since this is true, this means that there is some unique point that exists within the metric space such that when you plug in the value of the limiting point into the function it produces that limiting point.
Consider a spacetime $(\zeta^{3,1},g)$
where $$g=\frac{du\,dv}{uv}-\frac{dr^2}{r^2}-\frac{dw^2}{w^2} \quad \forall u,v,r,w \in (0,1)$$ Now this is just Minkowski space in different coordinates (related to Dirac/Light cone coordinates/null coordinates). I'm looking to take a Cauchy foliation of $\...
Like, for example, $\sin(x)$ on $[0,\pi/2]$ (or where ever $\sin$ is contractive). This is my goto example, because you can hit the $\sin$ button on the calculator over and over again.
@Ajay you tell me! If you are unsure about why a certain ingredient is important, you should dig deeper into it and try to figure out why it is important.
Let $\cos^n$ denote the $n$-fold composition of the cosine function with itself, e.g.
$$ \cos^3(\theta) = \cos(\cos(\cos(\theta))). $$
Note that this is not usually what this notation means in, for example, introductory calculus texts. However, it is convenient in the current context.
What you ...
@Ajay Think of an example of a very common, useful space which is not metrically complete.
@XanderHenderson As a result, I assume we need handbooks that provide information. Having read a number of elementary textbooks on linear algebra, I am getting bored with any new book because of the details.
@CroCo I don't understand why you "need handouts".
As I said above, you learn the results you have to use. While you are learning a new topic, you should be assigned a fair amount of work which requires you to use the theorems you are studying, hence those theorems should become familiar to you.
You'll likely forget them eventually (once you stop using them), but while you are learning them, you should learn them.
For an example: Theorem : For any square matrix A, there exists \epsilon >0 such that A-\epsilon I is invertible. Proof: To show det(A-\epsilon I)\not 0 .Observe that det(A-\epsilon I) =0 implies \epsilon >0 is an eigen value. What happen if we choose 0<\epsilon<|\lambda| where \lambda is the non zero eigen value ,smallest in absolute value in spec(A).
@CroCo Has nothing to do with doing math for a living. I am sure that I have forgotten more theorems than you will ever learn. :P
There is a moment in my career when I had a lot of results memorized and ready to go. That was the quarter I took all of my qualifying exams. I've lost a lot of that fluency over time.
My usual method of learning is to rewrite the theorems of the textbook and then save them. It's surprising to me that I can read the book again with so few pages.
@user977780 I totally agree.
As a mathematician, I assume this isn't the case since you teach math and have a great memory.
@CroCo You don't remember the things you don't use every day. I haven't thought about the Sylow theorems in ages, and can't remember a bit about them (something something a group of order something something subgroups dividing something something...).
As a tutor at my university, I have tried to teach basic math at a lower price to avoid forgetting something vital. In spite of this, tutoring can be exhausting, so I'm looking for alternatives like handbooks that provide immediate results.
It surprises me how few books are available on this subject.
I am fairly certain that there are actually more analysis texts out there than there are actual analysts. Because every analyst has written at least one book of their own.
Forgetting vital things sometimes causes so much trouble, some days ago, in the final exam of this semester, i forgot which classroom i was sitting at when I left to use the washroom :/
@PNDas a standard example would be the sequence e_n in in ell^1(positive integers) given by letting e_n's nth entry be 1 and have its other entries be 0. converges weak-star to 0, but not weakly. here you think of ell^1(positive integers) as the dual of the sequences indexed by positive integers that tend to 0 (itself normed by the sup norm).
OK, Obliv. Now, fix a point inside the circle of radius $2$. For that point (fixed $r,\theta$), what does $z$ do? When do you enter the region? When do you exit the region?
Go back to basics and how you set up limits of integration in the 2D case. You're not thinking. How do you set up the integral between $y=x^2$ and $y=4-x^2$ in $xy$-coordinates?