Infinite series question: Does anyone have an idea as to what the following series is equal to? \[1+\frac{x^2}{2^2}+\frac{x^4}{2^2 \times 4^2}+\frac{x^6}{2^2 \times 4^2 \times 6^2}+ \dots\]
well, it would have to most likely equate to some function since its got an x in it ....
the coefficient function might look scary tho .. why do you need to try to find a function for it?
It's for an integral that I need to evaluate.
can we see the integral to determine that this power series applies to it?
\[\int_0^\infty \left(x-\frac{x^3}{2}+\frac{x^5}{2\times4}-\frac{x^7}{2\times4\times6}+\dots\right)\times\\\left(1+\frac{x^2}{2^2}+\frac{x^4}{2^2 \times 4^2}+\frac{x^6}{2^2 \times 4^2 \times 6^2}+ \dots\right)dx\] I already evaluated the first term. It's on the second term where I am having trouble.
i assume that "x" means these are multiplied together ...
Yes, that's multiplication.
and your instructions (assuming this is for a class) tell you to remodify each series into ... what, a certain type of function perhaps? or was that your own concept to approach a solution?
It's just my idea for the solution since I was able to simplify the first term into \(xe^{-x^2/2}\). I figured I would be able to do the same to the second term.
hmmm \[\sum_0 \frac{(-1)^n}{f(n)}x^{2n+1}~~\sum_0 \frac{1}{[f(n)]^2}x^{2k}\]
can you show me how you got the first one modified?
It went like this: \[\large \sum_{n=0}^\infty (-1)^n \frac{x^{2n+1}}{2^n n!}=x\sum_{n=0}^\infty (-1)^n \frac{\frac{x^{2n}}{2^n}}{n!}=x\sum_{n=0}^\infty \frac{\left(\frac{-x^2}{2}\right)^n}{n!}=xe^{-x^2/2}\]
nice .... so the next one should amount to \[\sum\frac{x^{(2n)}}{(2^n~n!)^2}\]
do you know what a bezel function is by chance?
if we can show that one is the derivative of the other, this would amount to undoing a chain rule
if not, then a by parts is an idea that might simplify the structure
No idea what a bezel function is. I'll try the other two ideas for now.
i cant be certain but i believe the chain rule is working on this stuff
I finally solved the integral! I didn't simplify the series and just multiplied each term by \(xe^{-x^2}\). I then let \[\large I_n=\int_0^\infty \frac{1}{2^{2n}(n!)^2}x^{2n}xe^{-x^2/2}\ dx\] so that the original integral becomes \(I=\sum_{n=0}^\infty I_n\). I then got a closed form expression for \(I_n\) by letting \(u=x^2/2\) so that \(du=x\ dx\): \[\large I_n=\int_0^\infty \frac{1}{2^{2n}(n!)^2}2^nu^ne^{-u}\ du\\ \large=\frac{1}{2^nn!}\int_0^\infty \frac{1}{n!}u^ne^{-u}\ du=\frac{1}{2^nn!}\] because that last integral is the area of the gamma pdf \(f_Y(y)=\frac{\lambda^r}{\Gamma(r)}y^{r-1}e^{-\lambda y}\) with \(\lambda=1, r=n+1\). The integral then becomes \[I=\sum_{n=0}^\infty I_n =\sum_{n=0}^\infty \frac{1}{2^nn!}=\sum_{n=0}^\infty \frac{\left(\frac{1}{2}\right)^n}{n!}=e^{1/2}\].
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