mm k im supposed to just look at the degrees of the exponentials i guess
makes sense
lol
nvm im still confused
$$\frac{Nk_B(\varepsilon\beta)^2 \exp(\beta\varepsilon)}{(\exp(\beta\varepsilon)-1)^2}\approx Nk_B(\beta\varepsilon)^2\exp(-\beta\varepsilon)$$ since $\beta\varepsilon\to\infty$ as $T\to 0$ idk how this follows
I'll let others speak to it the math way. For the physics way you simply observe that $(\exp(\beta\varepsilon)-1)^2 \to (\exp(\beta\varepsilon))^2$ in this large $\beta$ limit. Then cancel one factor of $\exp(\beta\varepsilon)$ from the top and bottom.
A "soft" question about math writing for folks here: how do you deal with nested brackets? For example, suppose I wanted to write an aside in brackets, and in that aside I refer to some equation, say equation (2.65). Would you choose square brackets in this case or is that bad form?
(This follows from equation (2.65)) or [This follows from equation (2.65)]
I think the former is perfectly fine, but when Xander arrives, he will probably be able to point you to the precise subsubsection in the AMS style guide where this is addressed
@Thorgott There isn't actually a ton there, though the inference I draw is that "This follows from (2.65))" is the preferred style (note that is just "(2.65)", not "equation (2.65)").
E.g. section 6.4
> Identifying letters ((a), (b), (c)), including their parentheses, are roman in all text. The AMS will allow italic identifying letters only if consistent throughout.
Section 13.14:
> In cross-references, equation numbers are enclosed in roman parentheses to match the original label and the parentheses are always roman.
(which only says that equation numbers should always be in parentheses, not other kinds of braces).
On the other hand, the only references that the style guide has to brackets is in the context of citations and "fences" in mathematical contexts. I do not think that AMS editors would be too happy with square braces for parenthetical content.
Personally, I would seek to rewrite the phrase.
@Obliv No. This is wrong. Again, see section 13.14 of the AMS style guide.
@leslietownes Just quickly coming back to this conversation -- as regards the $T$-periodic space of functions which are spanned by the trigonometric functions, I guess I gave the wrong norm right? It should be induced by an inner product looking something like $<f,g> = \lim_{T \to \infty}\frac{1}{T}\int_{-T/2}^{T/2} fg$?
EE18 if you are looking at periodic functions the usual norm of <f,g> would be an integral of fg over one period (which is arbitrary but usually fixed, e.g. [0,T] or [-T/2,T/2]). you might be able to write out some limit over increasingly large that ends up being the same thing because of the periodicity, but i don't know why you would want that
you can also define inner products of not necessarily periodic functions in terms of integrals over all of R, usually with some kind of "decay at infinity" hypothesis floating in the background to ensure that the thing makes sense and is finite, and sometimes (not always, and not usually by definition) expressions for those sorts of norms are written as limits like that
@leslietownes Though in a lot of cases, those won't really be inner products, but the dual pairing (which devolves to an inner product in spaces which are self-dual. (Not that this really matters).
@leslietownes Actually sorry for perseverating on this Leslie, but I've been searching around and not able to find a wikipage or something like that for this. What term should I be using to learn more about this equivalence between the two possible inner products on this periodic function space?
maybe just prove it? i could see it as a homework problem in an analysis book. if f is periodic with period T then the average value of f on [-L, L] goes to the average value of f on [0,T] as L goes to infinity. it should make intuitive sense.
there are several duplicates of that question on the site too, all with similar looking proofs. it's maybe an expository challenge to make the argument look good. it might clean things up a little to assume T = 1 or something like that
I realized I have no idea how to glue together closed subsets bounded by analytic boundary S^1's when I'm not in the Top Cat. Do I operate in the Top Cat and then use some deformation or rigidification process to deform the topological surface into smooth/real analytic manifold? I think that is the right direction because there are theorems guranteeing a topological manifold and smooth manifold can be deformed to a anlaytic one. I'm lost on the details though
not sure where to start exactly but maybe in Top, and generate a topological surface S^2, and then sequentially layer on smooth then analytic structures. If the S^2 here is obtained through a gluing and one can obtain an analytic metric compatible with the base (unwrapped quotient), related through the section/exact projection correspondence allowing for a direct analytic quotient metric on the S^2. I think I should go for the low hanging fruit and that would be recovering a well defined
analytic manifold with a well defined analytic quotient metric
In mathematics, the complexification of a vector space V over the field of real numbers (a "real vector space") yields a vector space VC over the complex number field, obtained by formally extending the scaling of vectors by real numbers to include their scaling ("multiplication") by complex numbers. Any basis for V (a space over the real numbers) may also serve as a basis for VC over the complex numbers.
== Formal definition ==
Let
V
{\displaystyle V}
be a real vector space. The complexification of V is defined by taking the tensor product of...
I keep forgetting the definition of tensor product.
I remember it using its existence property diagram but forget it soon.
V, W - K vector spaces. V tensor W is a K- vector space along with a bilinear map f: V\times W into V tensor W such that every bilinear map out of V\times W into a K vector space U is composition of a unique linear map (from V tensor W into U) with f.
But I never really understood the motivation for tensor products.
suppose $ R $ is a ring and $\mu: R\rightarrow [0,\infty]$ is sigma additive, how can i show that for $ A \subset \cup_i A_i: \mu(A) \leq \sum_i \mu(A_i)$ if the unity need not be in the set (ie i can not use the attribute of sigma additivity)
if it is contained, then its trivial by definition... if it is not contained?
yeah. Tensor products are, first and foremost, applied in differential geometry
"Defined as $(\pi_1\otimes \pi_2)(g, h) = \pi_1(g)\otimes \pi_2(h)$" really should be "Defined as $(\pi_1\otimes \pi_2)(g \otimes h) = \pi_1(g)\otimes \pi_2(h)$"
or in other words, the linear map coming from the bilinear map $(g, h)\mapsto \pi_1(g)\otimes \pi_2(h)$
Hi, I'm studying the uniform convergence of $f_n(x)=n\sqrt{4\pi^2 n^2 +x^2}$ on $\mathbb{R}$. I proved that $f_n(x) \to \frac{x^2}{4\pi}$ pointwise on $\mathbb{R}$. My reasoning to prove that $f_n$ is not uniformly convergent to $\frac{x^2}{4\pi}$ is the following: $\sup_{x \in \mathbb{R}} |f_n(x)-f(x)| \ge |f_n(n)-f(n)|=n^2|\frac{\sin \sqrt{4\pi^2 n^2+n^2}}{n}-\frac{1}{\pi}|$.
Suppose $\overline{E}$ is $\sum_s E(s)P(s) = -\mu BP_{\uparrow}+\mu BP_{\downarrow} = -\mu B(P_{\uparrow}-P_{\downarrow}) = -\mu B\tanh(\beta \mu B)$. I want to set the energy levels to $0$ and $2\mu B$ instead of the $\pm \mu B$ but I'm not sure if that's the same as $$\mu B\left(\frac{1-e^{-2\mu B\beta}}{1+e^{-2\mu B\beta}}\right)$$
which is what u get if you do that. Like is what's in the parentheses a $-\tanh(\beta\mu B)$
I think it should be. I guess there isn't much of an advantage doing it this way since $\tanh$ is more recognizable
@leslietownes This is awesome, thanks so much :) \
So am working with my analysis text this morning which is on a last brief section about vector spaces before the fun with sequences starts next chapter
The book has a brief aside about polynomial interpolation, and proves that the existence and uniqueness of an $m$ degree polynomial to "match" a function at $m+1$ locations
They do it by explicit construction of the Lagrange interpolation polynomials without much motivation, fine
They then mention the following:
What could the last sentence possibly mean? I know things like "simple" or "explicit" can be informal notions but I fail to see why Gauss-Jordan wouldn't give us explicit descriptions of each $p_j$ and, putting them all together, the given polynomial?
The standard formula is that $\overline{X} = \sum_k k\cdot P(X = k)$. But $P(X = k) = \sum_{s:X(s) = k} P(s)$ so the formula $\overline{X} = \sum_s X(s)P(s)$ seems correct
@Jakobian thank you. Instead, if I consider the uniform convergence in $[0,a]$ with $a>0$, that reasoning above is not valid anymore because, even if it's still true that $\sup_{x \in \mathbb[0,a]} |f_n(x)-f(x)| \ge |f_n(n)-f(n)|$, I then must take the limit as $n \to +\infty$ and for fixed $a>0$ I have $n \notin [0,a]$ for $n$ big enough, right?
I mean, it's true for $n \in [0,a]$ but it is not true for each $n \ge N$ for some $N \in \mathbb{N}$ and this is what I need when I want to evaluate $\lim_{n \to +\infty} \sup_{x \in [0,a]} |f_n (x)-f(x)|$