Statistics/Distributions/Gamma

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The Gamma distribution is very important for technical reasons, since it is the parent of the exponential distribution and can explain many other distributions.

The probability distribution function is:


f_x (x) =
\begin{cases}
\frac{1}{a^p \Gamma (p)} x^{p-1} e^{-x/a}, & \mbox{if } x \ge 0 \\
0, & \mbox{if } x < 0
\end{cases}\quad a,p >0

Where  \Gamma(p) = \int_0^\infty  t^{p-1} e^{-t}\,dt\, is the Gamma function. The cumulative distribution function cannot be found unless p=1, in which case the Gamma distribution becomes the exponential distribution. The Gamma distribution of the stochastic variable X is denoted as  X \in \Gamma (p,a) .

Alternatively, the gamma distribution can be parameterized in terms of a shape parameter α = k and an inverse scale parameter β = 1 / θ, called a rate parameter:

 g(x;\alpha,\beta) = K x^{\alpha-1}  e^{-\beta\,x}   \ \mathrm{for}\ x > 0 \,\!.

where the K constant can be calculated setting the integral of the density function as 1:


\int_{-\infty}^{+\infty}g(x;\alpha,\beta) \mathrm{d}t \, = \int_{0}^{+\infty} K x^{\alpha-1}  e^{-\beta\,x}  \mathrm{d}x \, = 1

following:


K \int_{0}^{+\infty} x^{\alpha-1}  e^{-\beta\,x}  \mathrm{d}x \, = 1

K = \frac{1}{\int_{0}^{+\infty} x^{\alpha-1}  e^{-\beta\,x}  \mathrm{d}x}

and, with change of variable y = βx :


\begin{align}
K &= \frac{1}{\int_{0}^{+\infty} \frac{y^{\alpha-1}}{\beta^{\alpha - 1}}  e^{-y}  \frac{\mathrm{d}y}{\beta}} \\

&= \frac{1}{\frac{1}{\beta^{\alpha}}\int_{0}^{+\infty} y^{\alpha-1}  e^{-y} \mathrm{d}y} \\

&= \frac{\beta^{\alpha}}{\int_{0}^{+\infty} y^{\alpha-1}  e^{-y}  \mathrm{d}y} \\

&= \frac{\beta^{\alpha}}{\Gamma(\alpha)}
\end{align}

following:

 g(x;\alpha,\beta) = x^{\alpha-1}  \frac{\beta^{\alpha} \, e^{-\beta\,x} }{\Gamma(\alpha)}  \ \mathrm{for}\ x > 0 \,\!.

Contents

[edit] Probability Density Function

We first check that the total integral of the probability density function is 1.

\int^\infin_{-\infin}\frac{1}{a^p \Gamma (p)} x^{p-1} e^{-x/a}dx

Now we let y=x/a which means that dy=dx/a

\frac{1}{ \Gamma (p)} \int^\infin_{0} y^{p-1} e^{-y}dy
\frac{1}{ \Gamma (p)} \Gamma (p)=1

[edit] Mean

\operatorname{E}[X]=\int^\infin_{-\infin}x \cdot \frac{1}{a^p \Gamma (p)} x^{p-1} e^{-x/a}dx

Now we let y=x/a which means that dy=dx/a.

\operatorname{E}[X]=\int^\infin_{0}ay \cdot \frac{1}{\Gamma (p)} y^{p-1} e^{-y}dy
\operatorname{E}[X]=\frac{a}{\Gamma (p)}\int^\infin_{0}y^{p} e^{-y}dy
\operatorname{E}[X]=\frac{a}{\Gamma (p)}\Gamma (p+1)

We now use the fact that Γ(z + 1) = zΓ(z)

\operatorname{E}[X]=\frac{a}{\Gamma (p)}p\Gamma (p)=ap

[edit] Variance

We first calculate E[X^2]

\operatorname{E}[X^2]=\int^\infin_{-\infin}x^2 \cdot \frac{1}{a^p \Gamma (p)} x^{p-1} e^{-x/a}dx

Now we let y=x/a which means that dy=dx/a.

\operatorname{E}[X^2]=\int^\infin_0 a^2 y^2 \cdot \frac{1}{a \Gamma (p)} y^{p-1} e^{-y}ady
\operatorname{E}[X^2]=\frac{a^2}{ \Gamma (p)}\int^\infin_0  y^{p+1} e^{-y}dy
\operatorname{E}[X^2]=\frac{a^2}{ \Gamma (p)}\Gamma (p+2) =pa^2(p+1)

Now we use calculate the variance

\operatorname{Var}(X)=\operatorname{E}[X^2]-(\operatorname{E}[X])^2
\operatorname{Var}(X)=pa^2(p+1)-(ap)^2=pa^2

[edit] External links

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