Negative cardinality can be defined, there's a question in MSE on that. You just have to be ready to give up something
Otherwise, if I recall one of my past experiments correctly, a set of negative cardinality (defined as some S and P such that |S|+|P|=0) breaks either axiom of regularity or de Morgan's law of set operations
First you need to ask yourself what is cardinality? It's a mathematical notion which is designed to give us a way to measure the size of a set.
When you want to extend cardinals to negative integers you need to ask yourself, what is the purpose of this extension? Can we measure "more sets" now?...
Ah sorry I mean axiom of extensionality
but it is much worse than that. Most of the set operation identities no longer work if you have negative cardinality
@Fargle Yeah, that one is cool because the operations are accessible examples of things that make ring operations, but they didn't have anything obviously to do with addition and multiplication.
Yeah, that's exactly why I like it! It can be easy to imagine that rings only arise from numbers, but this is a case where a ring is not numerical from the outset.
@LeakyNun One of them definitely had to be a countably infinite field, and I think I must have made another countable, and I realized the last two may very well be fine as finite... so after some extra checks I'm going to make those two finite
Hmm, maybe that's a bit too easy but if you give some massive polynomial and just take its splitting field, then there won't be an especially obvious basis. This question also depend on how things are presented to you
Let $f:R^n\to R^m$ be differentiable at a point $\vec v$. The gradient at $\vec v$ points in the direction of greatest increase. Is it possible that there is other direction where $f$ increases fastest? In other words, if we know that function increases in a direction fastest at a point $\vec v$, then, can we infer from this information that gradient is pointing in that direction?
$$f(x_1,x_2,...x_n):\mathbb{R}^n \rightarrow \mathbb{R}$$
The definition of the gradient is
$$ \frac{\partial f}{\partial x_1}\hat{e}_1 +\ ... +\frac{\partial f}{\partial x_n}\hat{e}_n$$
which is a vector.
Reading this definition makes me consider that each component of the gradient correspon...
I had a confusion while exchanging summation and integral. If f is a number-theoretic function then $$\int_1^x \sum_{n\le y} f(n) dy = \sum_{n\le x} \int_n^x f(n) dy$$ how did the change of limit in integral take place? I am a bit confused. Please help.
Let $R$ be some integral domain, $N$ a nonzero $R$-module, and $R^n$ free module of rank $n$. I am trying to show that $R^n \oplus N \simeq N$ implies $n=0$. I could use a hint.
@LeakyNun Ah, a counterexample? Hmm...perhaps I need to be more specific. I am trying to show that $R^n \oplus R/(a_1) \oplus ... \oplus R/(a_m) \simeq R/(a_1) \oplus ... \oplus R/(a_m)$ implies $n=0$, where $a_i \in R - \{0\}$ are not units and $a_1 | a_2 |...|a_m$.
By what? If I take the torsion of both sides of $R^n \oplus R/(a_1) \oplus ... \oplus R/(a_m) \simeq R/(a_1) \oplus ... \oplus R/(a_m)$, both sides are $ R/(a_1) \oplus ... \oplus R/(a_m)$, right?
@AlessandroCodenotti oh! That explains it :) . But yeah, if you ever see something that looks wrong please let me know. I do want to make sure there aren't serious mistakes.
@LeakyNun Actually, what permits me to quotient by sides by their respective torsions? Isn't the following generally false, which we are implicitly making use of: if $M_1 \simeq M_2$ and $N_1 \subseteq M_1$ is isomorphic to $N_2 \subset M_2$, then $M_1/N_1 \simeq M_2/N_2$.
As for your question: Concentrate on the bottom right dotted square, see how there are 4 atoms at the corner and one at the center
Now movve this plane one step to the top left, now in the second slice, you see 4 atoms arranged in a diamond shape. Now move the plane again so it is at the top left, there are now 5 atoms in it.
This 4 5 4 arrangement is exactly what you expect for a FCC
@LeakyNun I'm struggling to remind myself about this: if $F$ is a finite field, then the cardinality of a $\kappa\geq\aleph_0$ dimensional $F$ vector space should be $\kappa$ exactly right? I think I remember learning that a union of a chain of $\kappa$ many sets with cardinality strictly less than $\kappa$ cannot exceed $\kappa$, but that's only a fuzzy memory.
What's an easy way of seeing ringtheory.herokuapp.com/rings/ring/92 is uncountable? I am not good with completions, but I seem to remember them as being described as a subring of an infinite product.. or maybe it isn't. Can I see it that way somehow?
$R\oplus S$ is a ring whose underlying set is $R\times S$ and the operations are defined coordinate-wise, meaning $(r,s)+(r',s')=(r+r',s+s')$ (note that the first addition is in $R\oplus S$, the second in $R$ and the third in $S$)
@LeakyNun I know the cardinality of continuous functions on $\mathbb R$ is $\mathfrak c$, and I guess a similar argument does the same thing for $\mathbb C$, and hence the ring of holomorphic functions?
I know nothing about that, but I believe it's a theorem that the Krull dimension of the Ring of holomorphic functions on an affine complex variety is either 0 or uncountably infinite.
Consider a connected holomorphic manifold $X$ and its ring of holomorphic functions $\mathcal O(X).$
My general question is simply: in which cases is the Krull dimension $\dim \mathcal O(X)$ known?
Of course if $X$ is compact $\mathcal O(X)=\mathbb C$ and that dimension is $0$.
There are also ...
@MikeMiller That's pretty interesting. I believe it, but how can it become $0$ if it's even $\mathfrak c$ on $\mathbb C$? I guess sometimes it's just exactly $\mathbb C$?
Does the case of holomorphic functions from $\mathbb C\to \mathbb C$ not a case where the domain is compact? I guess I'm not sure what topology is going on
That post is also implying the Krull dimension is $0$, if $\mathbb C$ is compact. But as I understand it, the ring is a nonfield domain @MikeMiller
Clearly I don't have a grasp on the whole context :/
Yes, I wouldn't talk to you about something that wasn't a manifold :)
If $M$ is a compact complex manifold without boundary such as the Riemann sphere, there are no nonconstants holomorphic functions. This is because they must have compact image in $\Bbb C$, which is closed; however the open mapping theorem says that nonconstant functions have open image. Thus we are constant.
If my assumption is correct, are there any other (important) instances like this in diff geom where authors call something, something else without telling the reader?
I have a hopefully rather simple question: I want to experiment with different geometries of flowlines and equipotential lines in a 2-Dimensional space in order to fit experimental data. Flow lines and equipotential lines are always orthogonal to each other, and hence form a basic rectangular gri...
I haven't taken complex analysis yet, so there may be many words to sift through and not much concrete mathematical notation. I do know a little math though. Anyway, to prepare for my complex analysis course I'm trying to find the conformal mapping that corresponds to the picture.
Given a local...
A group of $N$ miners trying to mine a block, I am one of them. In one scenario they are using a POW(proof of work) algorithm and in another, they use a ROW(race of work) algorithm.
The mining process is to execute the function $m()$. It returns a random hash number between $0 - 2^{32}$. In case...