Chernoff's distribution

In probability theory, Chernoff's distribution, named after Herman Chernoff, is the probability distribution of the random variable

 Z =\underset{s \in \mathbf{R}}{\operatorname{argmax}}\ (W(s) - s^2),

where W is a "two-sided" Wiener process (or two-sided "Brownian motion") satisfying W(0) = 0. If

 V(a,c) = \underset{s \in \mathbf{R}}{\operatorname{argmax}} \ (W(s) - c(s-a)^2),

then V(0, c) has density

 f_c(t) = \frac{1}{2} g_c(t) g_c(-t)

where gc has Fourier transform given by

 \hat{g}_c (s) = \frac{(2/c)^{1/3}}{\operatorname{Ai} (i (2c^2)^{-1/3} s)}, \ \ \ s \in \mathbf{R}

and where Ai is the Airy function. Thus fc is symmetric about 0 and the density ƒZ = ƒ1. Groeneboom (1989) shows that

 f_Z (z) \sim \frac{1}{2} \frac{4^{4/3} |z|}{\operatorname{Ai}' (\tilde{a}_1)} \exp \left( - \frac{2}{3} |z|^3 + 2^{1/3} \tilde{a}_1 |z| \right)
\text{ as }z \rightarrow \infty

where \tilde{a}_1 \approx -2.3381 is the largest zero of the Airy function Ai and where \operatorname{Ai}' (\tilde{a}_1 ) \approx 0.7022.

References


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