Gauss–Kuzmin distribution

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Gauss–Kuzmin
Parameters (none)
Support k \in \{1,2,\ldots\}
pmf -\log_2\left[ 1-\frac{1}{(k+1)^2}\right]
CDF 1 - \log_2\left(\frac{k+2}{k+1}\right)
Mean +\infty
Median 2\,
Mode 1\,
Variance +\infty
Skewness (not defined)
Ex. kurtosis (not defined)
Entropy 3.432527514776...[1][2][3]

In mathematics, the Gauss–Kuzmin distribution is a discrete probability distribution that arises as the limit probability distribution of the coefficients in the continued fraction expansion of a random variable uniformly distributed in (0, 1).[4] The distribution is named after Carl Friedrich Gauss, who derived it around 1800,[5] and Rodion Kuzmin, who gave a bound on the rate of convergence in 1929.[6][7] It is given by the probability mass function

 p(k) = - \log_2 \left( 1 - \frac{1}{(1+k)^2}\right)~.

Gauss–Kuzmin theorem

Let

 x = \frac{1}{k_1 + \frac{1}{k_2 + \cdots}}

be the continued fraction expansion of a random number x uniformly distributed in (0, 1). Then

 \lim_{n \to \infty} \mathbb{P} \left\{ k_n = k \right\} = - \log_2\left(1 - \frac{1}{(k+1)^2}\right)~.

Equivalently, let

 x_n = \frac{1}{k_{n+1} + \frac{1}{k_{n+2} + \cdots}}~;

then

 \Delta_n(s) = \mathbb{P} \left\{ x_n \leq s \right\} - \log_2(1+s)

tends to zero as n tends to infinity.

Rate of convergence

In 1928, Kuzmin gave the bound

 |\Delta_n(s)| \leq C \exp(-\alpha \sqrt{n})~.

In 1929, Paul Lévy[8] improved it to

 |\Delta_n(s)| \leq C \, 0.7^n~.

Later, Eduard Wirsing showed[9] that, for λ=0.30366... (the Gauss-Kuzmin-Wirsing constant), the limit

 \Psi(s) = \lim_{n \to \infty} \frac{\Delta_n(s)}{(-\lambda)^n}

exists for every s in [0, 1], and the function Ψ(s) is analytic and satisfies Ψ(0)=Ψ(1)=0. Further bounds were proved by K.I.Babenko.[10]

See also

References

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  4. Weisstein, Eric W., "Gauss–Kuzmin Distribution", MathWorld.
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