@BalarkaSen I am little bit confused about finding inverses for the extension fields. Suppose we have F is some field and K is extension obtained by $F[x] / (p(x))$ suppose we have a an element of this field how do you determine its inverse ?
@LeGrandDODOM Rudin's Real And Complex Analysis is pretty good. If you want to go deeper into measure theory, and you can read German (mathematics, not necessarily prose), I can strongly recommend Maß- und Integrationstheorie by Jürgen Elstrodt.
you know that gcd(g,p)=1, by the extended euclidean algorithm there exist t and s such that gt+ps=1, mod p you ignore the second term and t is the inverse of g
The whole $\frac{\mathbf{A} + i \mathbf{B}}{2}$ you do in a Lie algebra seems to be a way of saying $\mathbf{A}$ represents a real rotation, and $i \mathbf{B}$ a complex, i.e. hyperbolic, rotation, and they are distinct in the Lorentz group, weird
@DavidZhang Take a chart in RP^n, call it U. U --> R^n be the chart homeomorphism. Project to a coordinate to get U --> R. Extend to RP^n by making it zero outside a closed neighborhood of U by partition of unity.
@BalarkaSen Perhaps I should clarify that I'm writing some expository notes, and my "application" for such a function is to fill in the following sentence: "Not all homogeneous smooth functions are polynomials. For example..."
@SylentNyte Well, I was getting at the fact that the second derivative (the quadratic) should look like something like $C(x-3)^2$ for some constant $C$
I don't know how that translates to the original function, though
@SylentNyte No? The second derivative is $12x^2+6ax+2b$, right? The above means that it should equal $12(x-3)^2=12x^2-72x+108$. This tells us what $a$ and $b$ are.
@Null The "render ChatJax" command was the only one that worked before, so I had to click it every time new math was posted. But I got the "start ChatJax" to work now :)
I assume the function's domain is all real numbers. So I was able to derive a system of equations: $a^2=d^2; \;\; c(a+d)=0; \;\; b(a+d)=0$. The book agrees with this, but I got different results. (in form, at least)
I parametrized the solutions, so I said $u,v\in\mathbb{R},[(a,b,c,d)=(u,0,0,u)]\,\lor\, [(a,b,c,d)=(u,v,v,-u)]$. But the book has $$\dfrac{ax+b}{cx-a}\ne \dfrac{a}{c}\,\text{ or } \, a^2+bc\ne 0.$$ Question is... Is my answer equivalent?
@Null Hmm, I can sorta see the thought process, more like $f(f(x))=f(x)$ instead of $f(f(x))=x$ though
Okay! I figured I'm close but wrong, since $(u,0,0,u)$ for freely varying $u\in\mathbb{R}$ includes the 4-tuple with all zeroes, but that makes $f(x)$ not defined. Similar issue for $(u,v,v,-u)$. The book solution is like mine but removes these "problem points"
@BalarkaSen I want to clarify something. We say that $\alpha$ isn't algebraic over field F if there doesn't exist both an extension K of F and polynomial $p(x) \in F[x]$ for which $p(\alpha) = 0$ when evaluated in K right ?
I think Spivak is a bit careless with the notation here. He asks $$\text{Prove that }f=f^2\text{ if and only if }f=C_A\text{ for some set A.}$$ But he himself stresses the distinction between a function $g$ and its value $g(x)$. Isn't $f(x)=f(x)^2$ more correct?
So, I see. So, $\alpha \in K$ where K is field extension over F for which there is a polynomial $p(x) \in F[x]$ for which $p(\alpha) = 0$ when evaluated in K.
@Astyx I don't know. He's written to distinguish a function $f$ which a set from the function value $f(x)$, but here he's not even doing that as far as I see.
@Brody: Spivak does a good job of getting you used to functions the way mathematicians work with them. Standard calculus books are very sloppy in their notation, writing $y=f(x)$, $dy/dx$, etc.
@Ted Could we quickly talk about the question I had yesterday (or the day before, I can't remember) about the subsets of $U$ to which $\overline D$ has a deformation retract ?
@TedShifrin "Prove $f=f^2$ iff $f=C_A$ for some set $A$." But it should be $f(x)=f(x)^2$. The function value equals its square, but $f$ equal to $f^2$ looks misleading when earlier he stresses $f$ denotes a function, i.e. a collection of ordered pairs.
@Ted My question was more about he formalisation of the existence of a deformation retract from the disk to a closed proper connected subset of $U$, as I could not find a "simple" way of writing it
There is no simple way to write it, @Astyx. There needs to be a piecewise definition, and you probably want to rotate the picture and put it in some particularly nice position first.
I did it quite painlessly with $\{e^{it}, t\in [0, \pi]\}$ hoping I could go from this particular subset to all of them, but it didn't work out that way
Random question: With regards to sphere eversion, is there a polyhedral version? Starting with a polyhedron with triangular faces homeomorphic to the sphere, and moving the vertices continuously such that no dihedral angle becomes zero and such that it ends inside-out.
No, @Astyx, so let's make sure you have the picture right. Say the interval is a quarter circle $\pi/4\le\theta\le 3\pi/4$. How're you going to map to it?
So I was able to prove the statement. It's interesting though. So characteristic (i.e. indicator) functions are really the only functions for which their function value and the square thereof are equal?
@AkivaWeinberger Let me get this straight. If you want to inside-out, you have to go through the surface (self intersect). You're asking if this can be done without making nbhd of the vertices flat at some point?
Also, you're not restricting the moves of the faces? You can bubble it up and down so that it goes through itself? That seems to wreck the idea of doing it for polyhedra.
@Balarka, DogAteMy: Based on what I'm reading in wikipedia (I never read Smale's original paper), I'm guessing it'll work PL. Homotopy groups vanishing tells you that there is a regular homotopy between the original embedding and its eversion.
@TedShifrin I guess you could draw parallel lines going through the disk which would make a "beam" between the two boundaries of your arc, and connect the points of the disk not reached by this beam to the closest of the boundaries ?
Hello I have a question, here en.wikipedia.org/wiki/Vieta_jumping#Standard_Vieta_jumping in the first step we assume that there are solutions for which k is not a perfect square, why can't why assume that there are solutions for which k is a perfect square and follow the same reasoning?
@user379685: It's a proof by contradiction. So if you're trying to prove the number is a perfect square, you won't arrive at a contradiction by assuming it is :)
Of course, this is the extension of $f(x)$ to complex numbers. I don't even want to try Spivak's exercise with $x\in\mathbb{C}$ and complex coefficients.
ted i still dont get it, let's say i don't know if k is or is not a perfect square, what's wrong with following the reasoning given in the wiki but assuming that there are solutions for which k is a perfect square
@TedShifrin Ah sorry, 3.8 was the exercise I was talking about. If $f(x)=(ax+b)/(cx+d)$, for which numbers $a,b,c,d$ is $f(f(x))=x$ true? I imagine allowing everything to be complex makes the exercise significantly harder.
Here's a neat intuition for sphere eversion though. Immerse an RP^2 inside R^3 (say the Boy's surface). Take the normal bundle and look at the unit circle bundle (t = 1). That's an S^2 inside R^3 because that's what double covers RP^2. Now slowly make t smaller. At t = 0 it agrees with the zero section, RP^2. Now move it backwards till t = -1. That's the sphere, "everted". I think this can be made rigorous in some sense.
@MikeMiller Given a polyhedron in R^3, can you homotope it through polyhedron (aka1-parameter family of PL-embeddings of a polyhedron) so that the end map is the same polyhedron, embedded so that orientation is reversed, and that you don't have to "push one face onto another" at any stage in the middle. (by which I guess you don't want to fold a paper through a line so that both the square faces fall into themselves).
This is not possible for the tetrahedron say, visually speaking. If you push a vertex to the base, everything falls flat onto the base.
@BalarkaSen When you're working with PL immersions, you'll be subdividing the triangulation you started with as you go forward in time. This is the natural thing to do. So as long as you're willing to further subdivide the tetrahedron, yes, you can do this. (Recall that a PL immersion is just a locally injective PL map.)