1 + 2 + 4 + 8 + …

In mathematics, 1 + 2 + 4 + 8 + … is the infinite series whose terms are the successive powers of two. As a geometric series, it is characterized by its first term, 1, and its common ratio, 2. As a series of real numbers it diverges to infinity, so in the usual sense it has no sum. In a much broader sense, the series is associated with another value besides ∞, namely −1.

Contents

Summation

The partial sums of 1 + 2 + 4 + 8 + … are 1, 3, 7, 15, …; since these diverge to infinity, so does the series. Therefore any totally regular summation method gives a sum of infinity, including the Cesàro sum and Abel sum.[1]

On the other hand, there is at least one generally useful method that sums 1 + 2 + 4 + 8 + … to the finite value of −1. The associated power series

f(x) = 1%2B2x%2B4x^2%2B8x^3%2B\cdots%2B2^n{}x^n%2B\cdots = \frac{1}{1-2x}

has a radius of convergence of only 1/2, so it does not converge at x = 1. Nonetheless, the so-defined function f has a unique analytic continuation to the complex plane with the point x = 1/2 deleted, and it is given by the same rule f(x) = 1/(1 − 2x). Since f(1) = −1, the original series 1 + 2 + 4 + 8 + … is said to be summable (E) to −1, and −1 is the (E) sum of the series. (The notation is due to G. H. Hardy in reference to Leonhard Euler's approach to divergent series.)[2]

An almost identical approach is to consider the power series whose coefficients are all 1, i.e.

1%2By%2By^2%2By^3%2B\cdots = \frac{1}{1-y}

and plugging in y = 2. Of course these two series are related by the substitution y = 2x.

The fact that (E) summation assigns a finite value to 1 + 2 + 4 + 8 + … shows that the general method is not totally regular. On the other hand, it possesses some other desirable qualities for a summation method, including stability and linearity. These latter two axioms actually force the sum to be −1, since they make the following manipulation valid:

\begin{array}{rcl} s & = &\displaystyle 1%2B2%2B4%2B8%2B\cdots \\[1em] & = &\displaystyle 1%2B2(1%2B2%2B4%2B8%2B\cdots) \\[1em] & = &\displaystyle 1%2B2s \end{array}

In a useful sense, s = ∞ is a root of the equation s = 1 + 2s. (For example, ∞ is one of the two fixed points of the Möbius transformation z → 1 + 2z on the Riemann sphere.) If some summation method is known to return an ordinary number for s, i.e. not ∞, then it is easily determined. In this case s may be subtracted from both sides of the equation, yielding 0 = 1 + s, so s = −1.[3]

The above manipulation might be called on to produce −1 outside of the context of a sufficiently powerful summation procedure. For the most well-known and straightforward sum concepts, including the fundamental convergent one, it is absurd that a series of positive terms could have a negative value. A similar phenomenon occurs with the divergent geometric series 1 − 1 + 1 − 1 + · · ·, where a series of integers appears to have the non-integer sum 1⁄2. These examples illustrate the potential danger in applying similar arguments to the series implied by such recurring decimals as 0.111… and most notably 0.999…. The arguments are ultimately justified for these convergent series, implying that 0.111… = 1⁄9 and 0.999… = 1, but the underlying proofs demand careful thinking about the interpretation of endless sums.[4]

It is also possible to view this series as convergent in a number system different from the real numbers, namely, the 2-adic numbers. As a series of 2-adic numbers this series converges to the same sum, −1, as was derived above by analytic continuation.[5]

Notes

  1. ^ Hardy p.10
  2. ^ Hardy pp.8, 10
  3. ^ The two roots of s = 1 + 2s are briefly touched on by Hardy p.19.
  4. ^ Gardiner pp. 93–99; the argument on p.95 for 1 + 2 + 4 + 8 + … is slightly different but has the same spirit.
  5. ^ Koblitz, Neal (1984). p-adic Numbers, p-adic Analysis, and Zeta-Functions. Graduate Texts in Mathematics, vol. 58. Springer-Verlag. pp. chapter I, exercise 16, p. 20. ISBN 0-387-96017-1. 

See also

References

  • Gardiner, A. (2002) [1982]. Understanding infinity: the mathematics of infinite processes (Dover ed.). Dover. ISBN 0-486-42538-X. 
  • Hardy, G.H. (1949). Divergent Series. Clarendon Press. LCC QA295 .H29 1967. 

Further reading