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Divergent geometric series


In mathematics, an infinite geometric series of the form :\sum_{n=1}^\infty ar^{n-1} = a + ar + ar^2 + ar^3 +\cdots is divergent if and only if |r| = 1. Methods for summation of divergent series are sometimes useful, and usually evaluate divergent geometric series to a sum that agrees with the formula for the convergent case :\sum_{n=1}^\infty ar^{n-1} = \frac{a}{1-r}. This is true of any summation method that possesses the properties of regularity, linearity, and stability.

Examples

In increasing order of difficulty to sum:

Motivation for study

It is useful to figure out which summation methods produce the geometric series formula for which common ratios. One application for this information is the so-called Borel-Okada principle: If a regular summation method assigns \sum_{n=0}^{\infty} z^n to 1 / (1 - z) for all z in a subset S of the complex plane, given certain restrictions on S, then the method also gives the analytic continuation of any other function f(z) = \sum_{n=0}^{\infty} a_n z^n on the intersection of S with the Mittag-Leffler star for f(z).

Summability by region

Open unit disk

Ordinary summation succeeds only for common ratios |r|

Closed unit disk

  • Cesàro summation
  • Abel summation

Larger disks

  • Euler summation

Half-plane

The series is Borel summable for every z with real part

Shadowed plane

Certain moment constant methods besides Borel summation can sum the geometric series on the entire Mittag-Leffler star of the function 1/(1 − z), that is, for all z except the ray z ≥ 1.

Everywhere

Notes

References

References

  1. Korevaar p.288
  2. Moroz p.21
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