Intro
Let Z>0 be a random variable with the mean and variance defined as E{Z} and Var{Z}, respectively. The variance stabilization transform (VST) f(z) turns heteroskedastic data z to homoskedastic data f(z) with constant variance, e.g., variance equals 1.
Poisson distribution
For Poisson distributed data with E{Z}=Var{Z}=λ this VST, so-called Anscombe transformation, is given by [1,2]:
f(z)=2√z+3/8
Based on the first order Taylor expansion we can write (this is called Delta method in the literature) [3]:
Var{f(z)}≈(dfdz|z=E{Z})2Var{Z}=Var{Z}E{Z}+3/8
Problem
I performed a Monte Carlo simulations to compare sample variance of the stabilized data f(z) and the variance obtained by the above equation, i.e., Var{f(z)} both numerically as a sample variance and theoretically as follows:
Var{f(z)}≈λλ+3/8
Moreover, I went further and derived second order approximation for Var{f(z)}.
There is a mismatch between variance of stabilized data f(z) (green curve) and those obtained theoretically and numerically by means of the Var{f(z)}. Can anyone explain me this inconsistency?
- Anscombe, F. J. (1948), "The transformation of Poisson, binomial and negative-binomial data", Biometrika 35 (3–4): 246–254, doi:10.1093/biomet/35.3-4.246, JSTOR 2332343
- http://en.wikipedia.org/wiki/Anscombe_transform
- Kendall's Advanced Theory of Statistics: Volume 1: Distribution Theory by Alan Stuart and Keith Ord (Apr 20, 2009), page. 351, eq. 10.14
No comments:
Post a Comment