saratchandra said:
If you assume that the answer is x, then 1-x = x and the answer is 1/2.
To demonstrate what saratchandra is talking about, let S be the value of this series,
[tex]S=\sum_{r=0}^{\infty} (-1)^r[/tex]
Then
if S exists, we can compute 1-S by adding 1 and the additive inverse of S:
[tex]1-S=1-\sum_{r=0}^{\infty} (-1)^r = 1+\sum_{r=0}^{\infty} (-1)(-1)^r<br />
= 1+\sum_{r=1}^{\infty}(-1)^r = \sum_{r=0}^{\infty} (-1)^r = S[/tex]
or 1-S=S, yielding S=1/2. This is of course illegal; just because an operation is valid when applied to a convergent series does not mean it can be applied to a divergent series. However, this value of 1/2 appears in many other forms when evaluating this series. For example,
[tex]\frac 1{1+x} = \sum_{r=0}^{\infty} (-1)^rx^r[/tex]
Evaluating this at x=1 yields
[tex]\frac 1{1+1} = 1/2 = \sum_{r=0}^{\infty} (-1)^r[/tex]
Hah! 1-1+1-1+... = 1/2! Yet another place this series arises is in the eta function,
[tex]\eta(z) = \sum_{r=1}^{\infty} \frac{(-1)^{r+1}}{r^z}[/tex]
At z=0, this becomes
[tex]\eta(z) = 1/2 = \sum_{r=0}^{\infty} (-1)^r[/tex]
So once again, 1-1+1-1+... = 1/2. Another way to look at the eta function is via its relation to the zeta function,
[tex]\eta(z) = (1-2^{1-z})\zeta(z)[/tex]
Thus [itex]\eta(0) = -\zeta(0)[/itex]. The series representation of the zeta function is
[tex]\zeta(z) = \sum \sum_{r=1}^{\infty} \frac{1}{r^z}[/tex]
Evaluating this series at z=0 yields
[tex]\zeta(0) = -1/2 = 1+1+1+1+\cdots[/tex]
This shows how the series 1-1+1-1+... is related to the series 1+1+1+1+..., which every physicist knows has a value -1/2 (zeta function renormalization).
Some very nasty tricks were employed here, several of them illegal. On the other hand, analytic continuity is a very legal operation, and this was used underneath the hood to find several of these evaluations. Several divergent series can indeed take on well-defined, consistent values when analyzed in the context of analytic continuity.