I mean, there might be something interesting that comes out of the foundations.
Because a lot of people do the same thing you do; they think about the analytic expressions of functions symbolically, rather than function-theoretically.
We expect that the symbolic approach is feasible
because differential galois theory is a thing
But it would be nice to see it done.
I'm pretty blind to the big picture of analysis.
I don't know how much the floor function, in particular, would be insightful.
Sorry, that sentence was a bit convoluted: I meant "they think about (the analytic expressions of functions) [symbolically], rather than [function-theoretically]."
Not sure what Euler's formula means but I /do/ know that square root halves angles. That's pretty easy to consider. After all multiplying -1 mirrors a point on the number line, so half multiplying should half mirror.
@EricStucky so when you mean bigger monsters what exactly are you referring to? Any piecewise expression based upon numerical x ranges is expressable with floor
Complex will be hard because I am starting from nothing, pretty much :/
I know that there is a thing called the Cauchy-Riemann equations, but I don't know what they are. (I know they are simple, but I still don't know them.)
@EricStucky when you try to define the derivative $f'(z_0) = \lim_{z \rightarrow z_0} \frac{f(z_0 + dz) - f(z_0)}{dz}$ for a complex function, you see you need to ensure that the value of $f'(z_0)$ is the same no matter what direction $dz$ goes in, just as you do this when definin real-valued derivatives, in ensuring this will hold you'll arrive at the Cauchy-Riemann equations.
Any thoughts on 'intersection theory' in differential topology? Seems like it's like a coordinate-free generalization of the fact that you define a system of non-linear equations by the intersection of surfaces?
Yeah, algebra of indicator functions is something I'm pretty familiar with :)
I'm not sure how your calculation has anything to do with subtracting the jump series.
I'm guessing that the difference of the limits is a feature of implied integration, because in ordinary integration this difference will be zero for any "function with a jump series" (as I defined in that one question of yours).
@MikeMiller I don't know how to do this offhand. For irreducible 3-manifolds this is harder than obstructing surgery on a knot (and thats already too hard for me. Seem like there might be some tricky way to do it if you allow reducibility.
You know how, with real functions, you can integrate them over an interval? And, if they have an antiderivative, you can compute it by subtracting the values of the antiderivative at the endpoints?
@EricStucky But, if our function has an antiderivative, it turns out that the exact curve doesn't matter; we can still just subtract the values of the antiderivative at the endpoints! In particular, integrating these over a loop gives $0$.
(Note that $1/z$ doesn't have an antiderivative; $\ln z$ isn't continuously defined over the whole complex plane.)
As it turns out, this is also true of any function that simply has a derivative!, as long as it's defined everywhere inside the loop.
Reason is, you can break the interior of the loop into a bunch of small triangles. And then the integral over the (oriented, by the way) loop is equal to the sum of the integrals around each of the small triangles, since wherever two triangles meet, the orientations cancel out.
"The function has a derivative" means the function is locally linear. So, on each of those small triangles, the function is approximately linear, and linear functions have antiderivatives! This means that the integral around each triangle is doubly small, because it's a small loop and it almost has an antiderivative.
It turns out that these are small enough that, when you add them all up, we can show that the total thing is smaller than $\epsilon$ (for some $\epsilon$ depending on the way we break the interior of the loop into triangles).
Choosing increasingly smaller triangles lets us show that it's smaller than every $\epsilon>0$, and so the whole thing is zero. So the integral of any differentiable function on a loop, as long as it's defined everywhere on the interior, is $0$.
@EricStucky the full function of jump series is just a series of differences of limits being added together. So, it winds up being that the implied integral and jump series is a way of restructuring another method called "splitting the integral".
@EricStucky however, it could still be useful outside the context of integration. Besides, splitting the integral is a way of taking it over continuous periods so as to avoid discontinuity. My method is still right. It's that I can now certifiably prove that it is correct as an integration method.
I see what was missing from what I was saying, now. The observations aren't just a function, they're a statistical process dependent on the current state. If it were just a function's image, we could always just redefine the chain in terms of the image space to make a Visible Markov Chain directly.