Here's what you could do (I wrote it in haste so I am not responsible for mistakes). Consider a nice function f with Mellin transform hatf(s)=intinfty1tsf(t)textdt
(most importantly we don't want our hatf to have poles and this is why I integrate from 1 to infty rather than from 0 to infty). Now consider frac12piiintc+iinftyc−iinftyzeta(s+1)2hatf(s)cdotfractextdss
(with c>0). On the one hand expanding zeta(s+1)2 into a Dirichlet series and hatf into an integral and interchanging both sum and integrals, we obtain that the integral above is equal to sumngeq1fracd(n)nintinfty1f(t)frac12piiintc+iinftyc−iinftyfractsnsfrac1stextdstextdt=sumngeq1fracd(n)nintinftynf(t)textdt
(The interchange might be difficult and I describe a way around it, below). On the other hand we can estimate the integral appearing in the second formula in this post, by shifting the contour and picking up residues. For instance, the residue at s=0 gives
intinfty1(fraclog(t)22+2log(t)+2gamma)f(t)textdt
[Warning: I might have messed up the residue calculation] and this is the "expected main term" (if not an exact expression!) for the integral in the second formula. Thus for example when f(t)=e−epsilont you expect the third formula to be asymptotic to the fourth formula (as epsilon goes to zero) [actually in this case, the two are probably identically equal].
The important feature of f(t)=e−epsilont is that hatf(s) has no poles!. The method described here, should work equally well for any nice smooth function which is not too different from e−epsilont.
Also, note that instead of using frac1s in the second formula, you could use Gamma(s). That would lead to a messier formula (you would need to take into account the poles of Gamma(s) at -1,-2,...) - but interchanging sum and integral in the third formula would be much much easier.
No comments:
Post a Comment