St · Statistics & Probability

Expected Value of 1/(X + 1) for a Poisson Distribution

Published By the 9to5Science editorial team

At a glance

  1. 1. Identify the distribution

    Let X be Poisson with parameter λ, so its probability at k is e^(−λ)λ^k/k!.

  2. 2. Substitute the probabilities

    Weight each value 1/(k+1) by the probability that X equals k, then sum over nonnegative integers.

  3. 3. Shift the index

    Rewrite the summand using λ^(k+1)/(k+1)! so the series becomes the exponential series.

  4. 4. Check the boundary

    For λ = 0, X is zero with certainty, so the expectation is 1.

Assume the expression is E[1/(X+1)]\mathbb{E}[1/(X+1)], where XX has a Poisson distribution with parameter λ\lambda. This expectation averages the reciprocal 1/(k+1)1/(k+1) over all possible count values kk.

For λ>0\lambda>0, the result is

E[1X+1]=1−e−λλ.\mathbb{E}\left[\frac{1}{X+1}\right]=\frac{1-e^{-\lambda}}{\lambda}.

The case λ=0\lambda=0 is handled separately: then X=0X=0 with probability 1, and the expectation is 1.

Derivation from the Poisson probability mass function

For a Poisson random variable,

Pr⁡(X=k)=e−λλkk!,k=0,1,2,…\Pr(X=k)=e^{-\lambda}\frac{\lambda^k}{k!},\qquad k=0,1,2,\ldots

By the definition of expectation for a discrete random variable, multiply each possible value 1/(k+1)1/(k+1) by its probability and sum:

E[1X+1]=∑k=0∞1k+1e−λλkk!=e−λλ∑k=0∞λk+1(k+1)!=e−λλ∑j=1∞λjj!=e−λλ(eλ−1)=1−e−λλ.\begin{aligned} \mathbb{E}\left[\frac{1}{X+1}\right] &=\sum_{k=0}^{\infty}\frac{1}{k+1}e^{-\lambda}\frac{\lambda^k}{k!}\\ &=\frac{e^{-\lambda}}{\lambda}\sum_{k=0}^{\infty}\frac{\lambda^{k+1}}{(k+1)!}\\ &=\frac{e^{-\lambda}}{\lambda}\sum_{j=1}^{\infty}\frac{\lambda^j}{j!}\\ &=\frac{e^{-\lambda}}{\lambda}(e^{\lambda}-1)\\ &=\frac{1-e^{-\lambda}}{\lambda}. \end{aligned}

In the second line, λk/((k+1)k!)\lambda^k/((k+1)k!) is rewritten as λk/(k+1)!\lambda^k/(k+1)!, then a factor of 1/λ1/\lambda is taken out. The index shift j=k+1j=k+1 makes the remaining sum the exponential series with its j=0j=0 term removed.

Worked example: λ=2\lambda=2

If X∼Poisson⁡(2)X\sim\operatorname{Poisson}(2), then

E[1X+1]=1−e−22≈0.4323.\mathbb{E}\left[\frac{1}{X+1}\right] =\frac{1-e^{-2}}{2} \approx 0.4323.

This is an average over the possible counts, not the reciprocal evaluated at the average count. For instance, E[X]=2\mathbb{E}[X]=2, but substituting that mean into the expression gives 1/(2+1)=1/3≈0.33331/(2+1)=1/3\approx0.3333, not the desired expectation. The terms in the expectation are weighted by the individual Poisson probabilities; values of XX near 2 are more likely than many other counts, but every nonnegative count contributes.

Why it is not the reciprocal of the mean

In general, a nonlinear function cannot be moved outside an expectation. Thus

E[1X+1]≠1E[X]+1.\mathbb{E}\left[\frac{1}{X+1}\right]\ne\frac{1}{\mathbb{E}[X]+1}.

For λ>0\lambda>0, the two expressions are strictly different. The function f(x)=1/(x+1)f(x)=1/(x+1) is convex for x≥0x\ge0, so Jensen’s inequality gives

E[1X+1]≥1λ+1.\mathbb{E}\left[\frac{1}{X+1}\right]\ge\frac{1}{\lambda+1}.

The numerical example confirms this: 0.4323>1/30.4323>1/3. Equality holds in the degenerate case λ=0\lambda=0, when XX is constant.

Common mistakes

  • Dropping the +1: The formula above is for 1/(X+1)1/(X+1), not 1/X1/X. The added 1 also ensures the expression is defined when X=0X=0.
  • Using only the mean: Replacing XX by E[X]=λ\mathbb{E}[X]=\lambda computes 1/(λ+1)1/(\lambda+1), which is generally not the expectation.
  • Forgetting the zero-count probability: The Poisson sum starts at k=0k=0. Since Pr⁡(X=0)=e−λ\Pr(X=0)=e^{-\lambda}, this term contributes e−λe^{-\lambda} to the expectation.
  • Applying the formula at zero without a limit: The displayed fraction has denominator zero when λ=0\lambda=0. Use the distribution directly, or take the limit, which is 1.

If the intended expression was E[1/X]\mathbb{E}[1/X], that is a different quantity and needs special care: an ordinary Poisson variable has positive probability of being zero, where 1/X1/X is undefined. The shift by 1 avoids that problem.

References

  1. A First Course in Probability — Sheldon Ross

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