Cantor distribution
| Probability mass function | |
| Cumulative distribution function File:CantorFunction.png Cumulative distribution function of the Cantor distribution | |
| Parameters | none |
|---|---|
| Support | Cantor set |
| Probability mass function (pmf) | none |
| Cumulative distribution function (cdf) | Cantor function |
| Mean | 1/2 |
| Median | anywhere in [1/3, 2/3] |
| Mode | n/a |
| Variance | 1/8 |
| Skewness | 0 |
| Excess kurtosis | -8/5 |
| Entropy | |
| Moment-generating function (mgf) | <math>e^{t/2}
\prod_{i=1}^{\infty} \cosh{\left(\frac{t}{3^{i
|
| Characteristic function | {{{char}}} |
\right)}</math>|
char =<math>e^{\mathrm{i}\,t/2}
\prod_{i=1}^{\infty} \cos{\left(\frac{t}{3^{i}}
\right)}</math>|
}}
The Cantor distribution is the probability distribution whose cumulative distribution function is the Cantor function.
This distribution has neither a probability density function nor a probability mass function, as it is not absolutely continuous with respect to Lebesgue measure, nor has it any point-masses. It is thus neither a discrete nor a continuous probability distribution, nor is it a mixture of these. Rather it is an example of a singular distribution.
Its cumulative distribution function is sometimes referred to as the Devil's staircase, although that term has a more general meaning.
Characterization
The support of the Cantor distribution is the Cantor set, itself the (countably infinite) intersection of the sets
- <math>
\begin{align}
C_{0} = & [0,1] \\
C_{1} = & [0,1/3]\cup[2/3,1] \\
C_{2} = & [0,1/9]\cup[2/9,1/3]\cup[2/3,7/9]\cup[8/9,1] \\
C_{3} = & [0,1/27]\cup[2/27,1/9]\cup[2/9,7/27]\cup[8/27,1/3]\cup \\
& [2/3,19/27]\cup[20/27,7/9]\cup[8/9,25/27]\cup[26/27,1] \\
C_{4} = & \cdots .
\end{align} </math>
The Cantor distribution is the unique probability distribution for which for any Ct (t ∈ { 0, 1, 2, 3, ... }), the probability of a particular interval in Ct containing the Cantor-distributed random variable is identically 2-t on each one of the 2t intervals.
Moments
It is easy to see by symmetry that for a random variable X having this distribution, its expected value E(X) = 1/2, and that all odd central moments of X are 0.
The law of total variance can be used to find the variance var(X), as follows. For the above set C1, let Y = 0 if X ∈ [0,1/3], and 1 if X ∈ [2/3,1]. Then:
- <math>
\begin{align} \operatorname{var}(X) & = \operatorname{E}(\operatorname{var}(X\mid Y)) +
\operatorname{var}(\operatorname{E}(X\mid Y)) \\
& = \frac{1}{9}\operatorname{var}(X) +
\operatorname{var}
\left\{
\begin{matrix} 1/6 & \mbox{with probability}\ 1/2 \\
5/6 & \mbox{with probability}\ 1/2
\end{matrix}
\right\} \\
& = \frac{1}{9}\operatorname{var}(X) + \frac{1}{9}
\end{align} </math>
From this we get:
- <math>\operatorname{var}(X)=\frac{1}{8}.</math>
A closed form expression for any even central moment can be found by first obtaining the even cumulants[1]
- <math>
\kappa_{2n} = \frac{2^{2n-1} (2^{2n}-1) B_{2n}}
{n (3^{2n}-1)},
</math>
where B2n is the 2nth Bernoulli number, and then expressing the moments as functions of the cumulants.
External links
- Morrison, Kent. "Random Walks with Decreasing Steps", Department of Mathematics, California Polytechnic State University, 1998-07-23. Retrieved on 2007-02-16.
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