I was asking because I've proved that in a real-closed field $f$ is square-free iff $\gcd(f, f') = 1$ using that the irreducible polynomials in a real-closed field have at most degree $2$, so they can't have repeated roots. Then I looked at wikipedia and found about perfect fields, and they said it holds for any field of characteristic $0$.
Because $(x-a)^2 = x^2-2ax+a^2$, so it can't be irreducible, $a$ in algebraic closure
(again, this relies heavily on what you mean by "the $p$-adic heat equation", as $p$-adic analysis is quite different from real analysis; no least upper bound property, the space is totally disconnected, etc)
I think that the usual approach is to use the (inverse) Fourier transform to turn multiplicative operators into pseudo-differential operators, via the spectral theorem. And yes, I am throwing around a lot of big words. I used to understand what they all mean and how they all fit together, but I am using them today just to feel smart.
But I am pretty sure that what I have written is no entirely nonsense.
@geocalc33 I don't think I understand the question. What do you mean by "composite $p$-adic functions"? What is the region of convergence of such an object?
@XanderHenderson Yeah I guess it doesn't have to be composite (two functions composed together) I guess what I'm asking is do you think it is more laborious to determine region of convergence of p-adic functions, than for real functions?
Maybe you are thinking of a function given by a power series, and asking where that power series converges? If so: no, I don't think that the problem is very different in the $p$-adic when compared to, for example, the reals or the complex numbers. This is because you will ultimately be looking at series like $$ \sum \|a_n x^n\|_p, $$ which are series of real (well, rational) numbers.
But I'm not sure if that is the question you are asking.
@Jakobian Over a fixed field every irreducible polynomial is the minimal polynomial of all its roots. In characteristic zero this means an irreducible polynomial and its derivative cannot share a common factor for degree greater than one because this would contradict the property to be the minimal polynomial. Only in characteristic non zero the derivative can be the zero polynomial with every element as a root and it doesn't yield a contradiction.
Probably this is the detailed proof that Ted Shifrin had in mind.
@robjohn You know, a group of archaeologists recently exhumed Beethoven. When they opened his coffin, they found him madly erasing his works. When asked what he was doing, he responded, "Decomposing."
i'm going to need to see more vast expanses of white space around the pointer and at the bottom of that image before i can give that the proper amount of attention
@AkivaWeinberger I made a HTML / JavaScript thing you can use to make diagrams for your domino puzzle. It can dump the diagram to SVG (and copy it to the clipboard). Click on a cell edge to place a domino that straddles that edge. Click a domino to delete it.
It doesn't bother to check for overlaps, but hopefully that's not a problem. ;)
I also updated my polyomino exact cover code to do SVG output. I haven't done a version (yet) for the domino puzzles, but here's an example of a tromino cover:
More generally, $E[X] = \int_{\Omega} x f_X(x)\,\mathrm{d}x$, where $\Omega$ is your sample space.
@geocalc33 I don't understand your claim.
What does it mean for there to be "only one natural way to measure the mean in the normal distribution"? Are there unnatural ways? Is the normal distribution somehow unique? What do you mean?
@XanderHenderson Well my claim is about divvying up the density for density functions by halving it in 2 distinct ways. For example, the normal distribution has that reflection symmetry about a vertical line. That's clearly the natural way to find the mean (or balancing point)
and doing $\int_{\Omega} xf_{X}(x)~dx$ clearly supports that
You have used the word "clearly". I believe that I have make my opinion about that word quite... clear.
What you are observing is that the mean / expected value coincides with the center of mass. This is a more generally true result, if you consider $\Omega$ to be a physical object and the pdf to represent an actual density.
@XanderHenderson If $f_{X}(x)$ is a self inverse function then you could halve the area by slicing with the identity function. And because of this I think you could define the mean differently than the classical definition