psie: any proof oriented textbook would have to spend some time defining what "a^b" is before a statement like "a^b = c" becomes something meaningful in the context of that book, let alone something "to be proved." but yeah it is basically up to the author
what's going wrong here, maybe, is your expectation that rudin should define it. why? does he need to use it anywhere?
if he somehow makes an appeal to 0^p for general positive real p somewhere, okay, he should have defined it. if he doesn't, it's just.. i don't know. something it is OK for the book to be silent on. i don't imagine that it's actually that common for real or complex analysis books to have a need for 0^p for general positive real p
@leslietownes I think it is important, especially in regards to his other books. Consider the $p$-norm. How do you prove $\|x\|_p=0\iff x=0$ for $x\in\mathbb R^n$ say? Well, for $\implies$ direction, we have $\left(\sum_1^n |x_j|^p\right)^{1/p}=0$. Now I'd like to raise both sides to the power of $p$, a real number between $1$ and $\infty$. But we can't, because $0^p$ is not defined.
he implicitly defines it for positive integers in a remark about notation in general fields (1.13 (a) in the edition i'm looking at now), where he treats it more as a notational thing than something that needs formal definition. implicitly he is assuming that the reader will be OK with the fact that this remark might be all he says about the case for positive integer powers
psie: i see that as a good case for, there certainly would have been good reasons for him to include it. but he certainly doesn't need to define it in one book because of what he might have used or done in another book. that isn't how anything works.
it's also fine for an analysis book to introduce the p-norms without defining any of this stuff. i don't imagine folland does, for example. it's just part of the assumed background for a given book, or not. which is something that varies, sometimes considerably, from book to book
"this might be referenced in another book, so it has to appear in this one" is just, no. not at all. shouldn't every real analysis book also be a complex analysis book by that measure?
if the background motivational question "why is rudin so worried about what a^b is for some values of a and b and not other simpler values of a and b" it's because, first and foremost, rudin is addressing the cases he actually intends to use in his book (and i don't think he introduces p-norms in PMA), and second, he is focusing where he thinks his reader may need to invest time and effort to make good sense of things, and apparently in his view, 0^p is not one of those cases
and he's not getting into that any more than he sets out in a formal definition what a^m is when a is an element of an abstract field and m is a positive integer. he just does stuff. it's his vision of an analysis book and not whatever book you want it to be
jakobian: well, in a later chapter he uses the exponential function to define a^b for a more sensible domain (which admittedly still excludes 0)
he may even refer to how he's going to do this later in the earlier chapters
i wouldn't say he is half-assing it unless he actually makes use of something that he didn't define, or defined only partially in an exercise
if he's just deferring discussion of something he doesn't actually use until later, he's just, organizing a textbook differently from what other people would have done
working through the partial definition he hid in that exercise is a pretty good education in why it maybe isn't that great of a definition to work with, particularly for beginners
maybe a rare moment of pedagogical insight from walter rudin
Calculate the following double integral (directly and with the Gauss Green formula)
$$\iint_D xy\,\mathrm{d}x\,\mathrm{dy}$$$$D={(x,y)|y\le x \le \sqrt{y+2}, 0\le y \le 2}$$
directly: $$\int^2_0\int^\sqrt{y+2}_y xy \ \ \mathrm{dx} \ \mathrm{dy}$$$$\int xy \ \mathrm{dx} = y \ \cdot \int x \ \mathr...
Is there a way to essentially have a sequence of positive integers and determine how many structures that can remain balanced can be built if the bottom row has the first number of perhaps squares or rectangles and then the next is stacked as so forth
Thinking squares but then there's a question of whether they should be flush and additionally how would having a row of 1 affect
Let $u, v\geq 0$ and $s, t > 0$. 1. $u^tu^s = u^{t+s}$ 2. $(u^t)^s = u^{ts}$ 3. $u < v \iff u^t < v^t$ 4. $0^s = 0$, $1^s = 1$ 5. $u > 1, s > t \implies u^s > u^t$ 6. $0 < u < 1, s > t \implies u^s < u^t$ 7. $u^n = \prod_{i=1}^n u$ 8. $u^{1/n}$ is the unique non-negative $n$th root of $u$
In the past I've came up with those conditions for what a function $(u, t)\mapsto u^t$ where $u\in R$ is an element of a partially ordered ring and $t > 0$ is a real number is ought to satisfy in order to be considered exponentation
my text (Mathematical Physics by Arfken) defines a singular point of a complex variable function $f(z)$ as a point $z_0$ such that $\frac{df}{dz}\lvert_{z=z_0}$ does not exist.
The text later goes on to describe "singularities" which are points at which a complex variable function $f(z)$ is not holomorphic.
Are singular points then just special cases of singularities? By the definitions in this book it seems so, but the definitions do not seem very well organized.
Physics is empirical. The epistemological foundation of physics (and all sciences) is that nothing can ever be known for certain, and that all conclusions are tentative and subject to overturning or refinement based on observations in the world. There is no such thing as proof in physics.
A mathematician can prove that a statement is true within the framework of mathematics. But that doesn't prove anything to be true outside of that framework, and there is no way of proving that the "real world" matches the axiomatic framework of the mathematics.
@think_meaning_builds That is one of the questions of epistemology. Where does knowledge come from? How do we generate new knowledge? How do we verify that the things we believe are true are, in fact, true.
It is not about whether or not knowledge "exists" (I'm not even sure what that statement means).
Beyond that, I would suggest that a quick Google search for the word "epistemology" would likely be much more helpful to you. I'll bet that Wikipedia has a good article on it, and the Stanford encyclopedia of philosophy says useful things, too.
@think_meaning_builds If that is your attitude, then you would likely not ever earn more than a C on the exams I write. A and B students need to generate new knowledge, beyond what can be memorized.
@ModularMindset The "correct" use of mathematics in physics is generally "Assume some set of axioms which (hopefully) capture some important facet of the real world; prove some theorems in mathematics; run an experiment to see if those theorems correspond to real world observations".
@think_meaning_builds Not generally, no, because memorization (or routinization) is an important part of knowledge, and you can get a C by simply memorizing a bunch of stuff.
@XanderHenderson I'd argue that a mathematician can't truly prove the validity of their own proof, so they suffer from the same issue. Its just more nuanced. But I get that's not your point
@Jakobian You are going to have to expand on that.
Mathematicians make a certain set of assumed true statements (axioms) and define a process by which they demonstrate that new true statements hold (some system of logic). Within that artificial framework, it is certainly possible to prove true statements.
In mathematics, reading and verifying a proof is equivalent to doing an experiment in physics which would prove the validity of something. Both of these processes are subject to leading to false results
In the epistemology of mathematics, it is possible to make a statement and say, with absolute certainty, that the statement is either true or false, within the framework of whatever axioms have been assumed and whatever logical system is being used.
We can quibble about human error, but that is a distinct issue from the underlying epistemology. Everything done by humans is subject to error. But that is a distinct claim from the nature of mathematical knowledge as compared to scientific knowledge.
The mathematician claims to have proved a statement with certainty; the physicist claims that their experiment is consistent with their theoretical framework, and is therefore evidence that their theoretical framework does a good job of modeling reality.
I've been trying to learn about the multiple theories of truth and I've taken a look at the popular Stanford article. The first section has this to say about the neo-classical theories of truth:
These theories all attempt to directly answer the nature question: what is the nature of truth? They ...
@Jakobian i guess physicists not only have to check that they computed their prediction correctly, but also that it agrees with nature. mathematicians only have to do the former
@RyderRude What do you mean by "like this"? Are you looking for more splatter horror? If so, I'm not sure that I have a lot of recommendations---it is not a genre I like very much. Early Peter Jackson films (Braindead (or Dead Alive in the US) in particular) might be to your taste.
Evil Dead and Evil Dead 2, perhaps?
A little less gloopy, but still in the realm of body horror are Carpenter's The Thing, Scanners, and Cronenberg's The Fly.
(1) Number of pages is not a great metric, particularly in mathematics, where brevity is fetishized.
(2) The actual writing (as in typing it out) is kind of irrelevant. When you say that it took you 2 months, are you talking about the writing, or about the entire process from "Is this theorem true?" to typesetting?
(I can bang out 20 pages of math in an afternoon, but that isn't really where the work is.)
When working on my masters degree, a colleague had twins. I bought them a pair of onsies, each with a single word on the front. One read "epsilon", and the other "delta".
how would you guys try to show that $$ f(x,y) = \frac{x^2y}{|x|^3+y^2}, (x,y) \ne (0,0) \text{ and } f(x,y) = 0, (x,y) = (0,0) $$ is continuous at the origin?
Ok, I've tried with polar coords but I ended up with $\rho g(\theta,\rho), g = \frac{\cos^2 \theta |\sin\theta|}{\left\vert\rho|\cos\theta|^3+\sin^2\theta\right\vert}$ but $0<|g|<1/\sin^2\theta$ which diverges for $\theta = 0 + k\pi$
Hi All, I have a question. The Bolzano-Weierstrass theorem states that "every bounded sequence contains a convergent subsequence". My question is that the theorem does not say that the given bounded sequence is convergent. Is this correct? Suppose we have a sequence (1,-1,1,-1,...). This is bounded but it has a convergent subsequence? May be I am misunderstanding this theorem.
Note, also, that this is a statement about the real numbers, and that it doesn't necessarily hold in a more general setting. For example, $\mathbb{Q}$ does not have this property (consider the sequence $$ a_n = \left( \left(1+\frac{1}{n}\right)^n\right), $$ which is bounded in $\mathbb{Q}$ and does not converge in $\mathbb{Q}$. It also has no convergent subsequences in $\mathbb{Q}$ (though it does converge in $\mathbb{R}$).
@XanderHenderson for the sequence of 1s, this means that in the proof of the B-W theorem by choosing successive halfs, somehow we will end up with a sequence of 1s. This part does not seem to come out from the standard proof of B-W.
The proof I have from Stephen Abbott shows, consider [-M,M]. Make two halves [-M,0] and [0,M]. One of them will have infinite points. Choose that half and choose a number. Now divide this into two halves. Again choose a half with infinite points and choose a number that comes after the first number in the original sequence. And keep doing this.
It is not that important but I was somehow wondering if somehow this halving method will somehow produce a sequence ending with infinite 1s for the (1,-1,1,-1,...) sequence. But it is fine. I dont need to understand that.
sure. that argument will provide a convergent subsequence in this case. the language of the summary of the argument maybe makes it sound like no choice is involved - i.e., that there is a unique choice of convergent subsequence, corresponding to whatever choices you "have to" make at each step. but that isn't actually what happens.
sku: at each step of that argument, it might be that both halves of whatever interval you're in contain infinitely many elements of the sequence. in that case you can choose either half. if that helps. i'm not sure if this relates to your difficulty
e.g. if you started with M = 10, you could initially choose whether to begin narrowing to [-10,0] or [0,10]. once you've done that, you are forced to choose whichever subinterval -1 is in (if you initially chose the left half) or 1 is in (if you initially chose the right half).
so this argument doesn't really come close to suggesting the full variety of convergent subsequences of your example. it chooses constant sequences only
your example is a fun (if pretty rare) example of a situation where it is possible to identify both the set of all subsequences, and the set of all convergent subsequences, in "fairly concrete terms"
i.e. any sequence of -1s and 1s whatsoever is a subsequence of your sequence, and the convergent ones are the ones that are eventually constant
sku there's something a little weird about the way that argument is phrased. "one of them will have infinite points" - here "infinite" refers to the set of positive integers n for which x_n is in the given half of the interval, not to the set of real numbers x_n that lie in that interval (which might always be only finite, as it is in your example)
so, of the infinite bag of positive integers for which x_n is in [0,M], you choose one, n_1. then you look at the sets of positive integers n larger than n_1 for which x_n is in [0, M/2] or for which x_n is in [M/2, M], respectively. one of those two bags will also be infinite. your selections from those infinite bags are indices n_1, n_2, .. that you use to form the subsequence, not the values x_{n_1}, x_{n_2}, etc. of the sequence itself
@sku The sequence $(1,-1,1,-1,1,-1,\dotsc) = ((-1)^n)$ is bounded between $-1$ and $1$, so $M=1$. In the first step, note that there are infinitely many terms in at least one of $[M,0]$ and $[0,M]$ (both, in fact). In particular, $a_2 = 1 \in [0,M]=[0,1]$. Take $b_1 = a_2 = 1$.
Then there are infinitely many terms of the sequence in either $[0,1/2]$ or $[1/2, 1]$ (this time, only the latter contains infinitely many terms). So choose some $a_k \in [1/2,1]$. I don't know... maybe $a_{10} = 1 \in [1/2, 1]$. Take $b_2 = a_{10} = 1$.
Now, there are infinitely many terms of $a$ in either $[1/2,3/4]$ or $[3/4,1]$ (again, only the latter this time). So choose some $k$ so that $a_k \in [3/4,1]$. How about $a_{48}=1$? Then $b_3 = a_{48} = 1$.
Keep going. Eventually, you will get the sequence $b$ defined by $b_k = a_{n_k} = 1$.
Let $T$ be a linear and continuous operator $T: L^{2}(\mathbb{R}^{d}) \to L^{2}(\mathbb{R}^{d})$. I wonder to what extent can we conclude if $T$ is strong $(p,p)$, we will obtain that $T'$, the adjoint of $T$, is strong $(p', p')$. For simplicity, we can take strong $(p,p)$ to be restricted to $S...