strangerep said:
Since Borel seems not to have been mentioned yet...
It is not the most powerful - but still is very powerful. I did a post explaining it in another thread. Need to head off now for physio but will elaborate when I get back.
Ok after being physically tortured I think this sheds light on divergent sums in general and Ramanujan Summation as another example of what is going on so to speak. IMHO this makes it on scope for this thread.
So let's go into Borel Summation.
To detail about Borel summation ∑an = ∑(an/n!)*n!. n! = Γ(n+1) = ∫t^n*e^-t so ∑an = ∑ ∫an*t^n*e^-t/n!. In general you can't interchange the sum and integral but under some conditions you can so we will formally interchange them and see what happens. So ∑an = ∫∑(an/n!)*t^n*e^-t. This is called the Borel sum and we will look at when it is the same as ∑an.
If ∑an is absolutely convergent by Fubini's theorem the sum and integral can be reversed and the Borel sum is the same as the normal sum. Consider the series S =1 + x + x^2 + x^3 ... It is absolutely convergent to 1/1-x, |x| < 1. Then the Borel Sum is S = ∫∑(x^n/n!)*t^n*e^-t = ∫e^t(x-1) = 1/1-x < ∞ if |x|<∞ - not only for |x|<1. In other words - when S is convergent in the usual sense then it is equal to its Borel Sum but S is only valid for |x| < 1, however the Borel Sum is still the same - but true for more values of x. Borel summation has extended the values of x you get a sensible answer - in fact exactly the same answer. This is the characteristic of analytic continuation ie if a function in a smaller region it is exactly the same function in a larger region. Borel summation has extended the region the series has a finite sum. Normal summation introduces unnecessary restrictions on the sum that Boral Summation removes - at least in part. This of course works for similar series like 1+ 2x + 3x^2 +4x^3 ... and is left as an exercise to show its Borel and Normal sum are the same ie 1/(1-x)^2.
There is also another way of looking at this by introducing what's called the Boral exponential sum. Personally I don't use it much but sometimes its of some use. It is defined as limit t → ∞ e^-t*S(t). Here Sn = a0 + a1 +a2 +...+an so limit n → ∞ Sn = S, and S(t) = ∑Sn*t^n/n!. Note for each single term in the sum limit t → ∞ e^-t*Sn*t^n/n! = 0. Using that its not too hard (but a bit tricky and not totally rigorous) to see if Σan converges normally to S then its exponential sum also converges to S. We divide the sum into two parts - the sum taken to N very large and the rest. But while large, since N is finite each term is zero in the finite part of the sum. But since N is large Sn in the rest of the sum can be taken as S so FAPP we have the infinite part of the sum as S*limit t → ∞ e^-t*∑t^n/n! with the sum being N+1 to infinity. However since the previous terms before N+1 are all zero the sum can be taken from 0 to infinity to give S*limit t → ∞ e^-t*e^t = S. Thus if ∑an converges in the usual sense to S then S is also the exponential sum.
Now we will show something interesting - if the exponential sum S exists then the Borel Sum exists and is also S. However the reverse is not true.
Let B(t) = ∑an*t^n/n! = a0 + (S1-S0)*t + (S2-S1)*t^2/2! + (S3-S2)*t^3/3! ++++++. Hence B(t)' = S(t)' - S(t) .
S - a0 = e^-t*S(t)| from 0 to ∞ = ∫d/dt [e^-t*S(t)] = ∫e^-t*(S(t)' - S(t)) = ∫B(t)'*e^-t = e^-t*B(t)| (o to ∞) + ∫e^-t*B(t) = -a0 + ∫e^-t*B(t). On cancelling a0 we end up with what was claimed S = ∫e^-t*B(t) which is the Borel Sum. We also have shown if ∑an normally converges to S then the Borel Sum is also S.
What this is saying is the Boral Sum is exactly the same for normally convergent sums. But if it's not normally convergent it can still give an answer. Not only this but if ∑an*x^n has any non zero radius of convergence the Borel Sum is exactly the same as the normal sum in the radius of convergence. It is an analytic continuation for all x. Analytic continuation is simply removing an unnatural restriction in the way the sum is written. So, one way of viewing Borel summation is simply removing an unnatural restriction in the way a series is written so it be expressed in a more natural way.
Looking at it this way we see that summing divergent series is simply analytic continuation of a function that is written in a restrictive form - analytic continuation allowing us to find the function that has not been restricted.
How does this work with Ramanujan summation? Well let's have a function, say the zeta function that depends on a parameter s. It is not hard to calculate the Ramanujan Sum for the zeta function. You get C(s) +Rn(s). If s >1 then Rn goes to zero and everything is fine. But if not ie Rn does not converge to zero, then we know the function for for other s - it must be the same by analytic continuation. So C(s) is the analytic continuation of the Zeta function for s<1 since it is the function when s >1. Its not a rigorous argument but I am sure can be made rigorous eg we need to show C(s) is analytical.
So what is the most powerful. Well Ramanujan summation will sum the zeta function - Borel will not.
BTW there is a lot of argument if 1+2+3+4... really does equal -1/2. I had a lot of trouble with that one, and my view has changed a bit over time. Now it for me is really quite simple - the integers can be interpreted as being part of the real line or complex plane. If you consider it just part of the real line then it can't be summed for |x| > = 1. For the complex plane you have analytic continuation and it can be done. So it enirely how you look at the problem.
I could say a bit about this and renormalization but will limit myself to only one comment. Sometimes it is said that renormalization is another trickier way of taking the limit in the infinite sum. Divergent sums are simply another way, namely considering the terms in the complex plane, of taking the limit in the infinite sum. In fact Hawking showed that zeta function summation and dimensional regularization are basically equivalent. Now that is interesting.
Thanks
Bill