When do the bounds on a Poisson’s median almost equal the mean?

Mathematics
Mathematical-Statistics
Author

Galen Seilis

Published

January 28, 2024

Question 1

When do the bounds on the median \(\nu\) of a Poisson distribution equal (or nearly equal) the mean of the distribution, \(\frac{1}{\lambda}\)?

The bounds of the median are given as (Choi 1994)

\[\lambda - \ln 2 \leq \nu < \lambda + \frac{1}{3}\]

Lower Bound

Let \[\lambda - \ln 2 = \frac{1}{\lambda}\] then we can obtain the polynomial

\[\lambda^2 - \lambda \ln 2 - 1 = 0\] for which we can then use the quadratic equation to obtain

\[\lambda = \frac{\ln2 \pm \sqrt{\left( \ln 2 \right)^2 +4}}{2}.\]

We obtain two approximate solutions for lambda:

\[\lambda_- \approx -0.7117804400329233\]

\[\lambda_+ \approx 1.4049276205928687\]

However, since we already know that \(\lambda > 0\) we can exclude \(\lambda_-\) and take \(\lambda_+\) as the unique solution.

Upper Bound

Let

\[\frac{1}{\lambda} = \lambda + \frac{1}{3}\]

then we can arrange to see this is a quadratic polynomial

\[\lambda^2 + \frac{\lambda}{3} - 1 = 0\] and apply the quadratic formula:

\[\lambda = \frac{-\frac{1}{3} \pm \sqrt{\left( \frac{1}{3} \right)^2 + 4}}{2}\]

This gives two candidate solutions:

\[\lambda_- \approx -1.18046042171637\]

\[\lambda_+ \approx 0.8471270883830365\]

Like with the lower bound, we can only take the upper bound to be \(\lambda_+\). But unlike the lower bound, we can only say that the median is strictly less than \(\lambda_+\) even if it is really really close.

Question 2

Assuming \(\lambda\) is known, how wide a range of values can the median take?

\[\lambda + \frac{1}{3} - \lambda + \ln 2 = \frac{1}{3} + \ln 2\]

Interestingly, no matter what value \(\lambda\) takes there is a constant-width interval for the values of the median.

References

Choi, Kwok Pui. 1994. “On the Medians of Gamma Distributions and an Equation of Ramanujan.” Proceedings of the American Mathematical Society 121 (1): 245–51. https://doi.org/10.1090/S0002-9939-1994-1195477-8.