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Normal-exponential-gamma distribution

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Normal-Exponential-Gamma
Parameters μR — mean (location)
k > 0 {\displaystyle k>0} shape
θ > 0 {\displaystyle \theta >0} scale
Support x ( , ) {\displaystyle x\in (-\infty ,\infty )}
PDF exp ( ( x μ ) 2 4 θ 2 ) D 2 k 1 ( | x μ | θ ) {\displaystyle \propto \exp {\left({\frac {(x-\mu )^{2}}{4\theta ^{2}}}\right)}D_{-2k-1}\left({\frac {|x-\mu |}{\theta }}\right)}
Mean μ {\displaystyle \mu }
Median μ {\displaystyle \mu }
Mode μ {\displaystyle \mu }
Variance θ 2 k 1 {\displaystyle {\frac {\theta ^{2}}{k-1}}} for k > 1 {\displaystyle k>1}
Skewness 0

In probability theory and statistics, the normal-exponential-gamma distribution (sometimes called the NEG distribution) is a three-parameter family of continuous probability distributions. It has a location parameter μ {\displaystyle \mu } , scale parameter θ {\displaystyle \theta } and a shape parameter k {\displaystyle k} .

Probability density function

The probability density function (pdf) of the normal-exponential-gamma distribution is proportional to

f ( x ; μ , k , θ ) exp ( ( x μ ) 2 4 θ 2 ) D 2 k 1 ( | x μ | θ ) {\displaystyle f(x;\mu ,k,\theta )\propto \exp {\left({\frac {(x-\mu )^{2}}{4\theta ^{2}}}\right)}D_{-2k-1}\left({\frac {|x-\mu |}{\theta }}\right)} ,

where D is a parabolic cylinder function.

As for the Laplace distribution, the pdf of the NEG distribution can be expressed as a mixture of normal distributions,

f ( x ; μ , k , θ ) = 0 0   N ( x | μ , σ 2 ) E x p ( σ 2 | ψ ) G a m m a ( ψ | k , 1 / θ 2 ) d σ 2 d ψ , {\displaystyle f(x;\mu ,k,\theta )=\int _{0}^{\infty }\int _{0}^{\infty }\ \mathrm {N} (x|\mu ,\sigma ^{2})\mathrm {Exp} (\sigma ^{2}|\psi )\mathrm {Gamma} (\psi |k,1/\theta ^{2})\,d\sigma ^{2}\,d\psi ,}

where, in this notation, the distribution-names should be interpreted as meaning the density functions of those distributions.

Within this scale mixture, the scale's mixing distribution (an exponential with a gamma-distributed rate) actually is a Lomax distribution.

Applications

The distribution has heavy tails and a sharp peak at μ {\displaystyle \mu } and, because of this, it has applications in variable selection.

See also


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References

  1. ^ http://www.newton.ac.uk/programmes/SCB/seminars/121416154.html
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