there's a definition: a Sylow System is a collection of Sylow subgroups $S_p$, one for each $p$ dividing $|G|$, such that $S_pS_q=S_qS_p$ for each $p,q$
They made the observation that e is the "natural base" for exponential functions because the derivative has the "nicest form"....and I was like: uh, how do you differentiate $b^x$ and what's e?
sylow systems exist (and are conjugate) for all solvable groups. so this style of argument, the prime by prime product you're doing, shows up a lot in solvable group theory. you might like it.
@seaturtles So, if the order of $G$ is a prime power we're done. Suppose then it has composite order, say ${\rm ord}\, g=p^a m$ with $m$ coprime to $p$.
my argument shows that every element is in some product of sylows, not that every element is in the product of any fixed full set of sylows. error was spotted later.
"I assume you mean the last element to be $(12)(34)$. In this case, $H$ has order $4$, so there are $3$ cosets. The first is represented by $e$, the second by $(13)$, and the third by $(24)$. Now, just check that the cosets of these three elements are disjoint, and you are done. "
wikipedia just intimates its a vector bundle over the same base space whose fibers are iso to tensor products of the original fibers. which doesn't seem very helpful.
@TedShifrin if the tensor product is just a vector bundle whose fibers are isomorphic to the tensor product of the fibers of the original two vector bundles, then how does that even depend on the geometry of the original two vector bundles?
Homotopy theory without torsion ... Sullivan's minimal models are all based on diff forms with rational coefficients. Griffiths, Morgan wrote a Birkhäuser book in the 80s
@TedShifrin "We also saw in the above proof that the embedding of $M$ as a submanifold of $\Bbb P^3$ can be achieved by using 3 or 4 linearly independent $q$-forms ($q$=1 except in the few exceptional cases.) We will show in IV.11 that every two meromorphic functions on $M$ are algebraically dependent. Hence we also have that every compact RS of genus $\geq 2$ can be realized as an algebraic submanifold of $\Bbb P^3$.
sounds like Chow's theorem, which you suggested for me for that a while back, is overkill
@TedShifrin if $E_1\xrightarrow{\pi_1}B$ and $E_2\xrightarrow{\pi_2}B$ are two vector bundles over $B$ then what is the underlying space $E$ of their tensor product, and what is the projection $E\xrightarrow{\pi}B$?
We were talking about analytic submanifolds of $\Bbb P^N$ being algebraic. Of course there are non-projective ones. Hodge Theory gives you necessary topological conditons.
@sea: An important example is the tensor product of the cotangent bundle with itself. Sections are bilinear forms on tangent vectors, e.g., Riemannian metrics.
I can't give you a global description of $E$ As a top space in general. But you usually can't with vector bundles, either.
They're described intrinsically, often, and constructed by gluing together trivializations by transition functions.
I want a definition or description for which it is obvious that the tensor product's geometry will depend on the geometry of the original two vector bundles. Saying the tensor product is a vector bundle over the same base space whose fibers are tensor products of the original two fibers doesn't seem to imply this.
@TedShifrin After doing some Cech cohomoloy and singular homology I definitely appreciate group cohomology more. Things seem more natural (even though it's far less canonically defined)
@Pedro: Did anyone point put to the OP that he wrote continuous, not uniformly continuous? I think you're answering the wrong question because the OP messed up his quantifiers.
A prolate spheroid is a spheroid in which the polar axis is greater than the equatorial diameter. Prolate spheroids are elongated along a line, whereas oblate spheroids are contracted. The prolate spheroid is defined by the equation \mu = c for some arbitrary constant c, in prolate spheroidal coordinates.
Properties
A prolate spheroid with b > a has surface area
S_{\rm prolate}=2\pi a^2\left(1+\frac{b}{ae}\sin^{-1}e\right)\qquad\mbox{where}\qquad e^2=1-\frac{a^2}{b^2}
and volume V_{\rm prolate} = \frac{4}{3}\pi a^2 b.
The prolate spheroid is generated by rotation about the major ...