Compute some expectations involving beta and gamma distributions

152 Views Asked by At

a) Let $X \sim {\text {Beta}}(a,b)$, with density $f(x) = \frac{x^{a-1}(1-x)^{b-1}} {B (a,b)}$. Find the expectation of $X \ln X$ and $\frac{1}{X+1}.$

b) Let $Y \sim {\text {Gamma}}(\alpha,\beta)$, with density $g(y) = {\frac {\beta ^{\alpha }}{\Gamma (\alpha )}}y^{\alpha \,-\,1}e^{-\beta y}$. Find the expectation of $Y \ln Y$ and $\frac{1}{Y+1}.$

c) Assume $X,Y$ are independent. Find $\Bbb E [\frac{1}{XY+1}]$ and $\Bbb E [\frac{1}{Y-XY+1}]$.

I reduced my previous question to the above much simpler questions. Any help with this question will help the previous question as well. Any help with any of above expectation calculations will be very much appreciated.

2

There are 2 best solutions below

0
On BEST ANSWER

Have you tried a computer algebra system?

Part (a): For $X \sim \text{Beta}(a,b)$ with pdf $f(x)$:

enter image description here

Then here is the output generated by mathStatica / Mathematica to the first problem:

enter image description here

... where HarmonicNumber[n] denotes the $n^\text{th}$ harmonic number $H_n=\sum _{i=1}^n \frac{1}{i}$, and

enter image description here where Hypergeometric2F1Regularized[a,b,c,z] denotes ${_2}F{_1}(a,b;c;z) / \Gamma(c)$, and Expect is a mathStatica function (of which I am one of the authors).


Part (b): For $Y \sim \text{Gamma}(\alpha,\beta)$ with pdf $g(y)$:

enter image description here

... you seek:

enter image description here

... where EulerGamma is Euler's constant (approx 0.577), and:

enter image description here

where ExpInteralE[$\alpha$, $\beta$ ] is the exponential integral function $\int _1^{\infty} \frac{1}{t^\alpha} e^{-\beta t} dt$


Part (c): Find $\Bbb E [\frac{1}{XY+1}]$ and $\Bbb E [\frac{1}{Y-XY+1}]$.

These two questions are essentially the same. To see this, note that if $X \sim \text{Beta}(a,b)$, then $(1-X) \sim \text{Beta}(b,a)$, and that $\Bbb E [\frac{1}{Y-XY+1}] = \Bbb E [\frac{1}{(1-X)Y+1}]$ which is thus also of form $\Bbb E [\frac{1}{XY+1}]$ (just with the $X$ parameters swapped). So we only need to solve the first part.

Given independence, the joint pdf of $(X,Y)$, say $h(x,y) = f(x) g(y)$:

enter image description here

Then $\Bbb E [\frac{1}{XY+1}]$ is:

enter image description here

While this expression looks rather cumbersome, it appears to be correct, and works fine for non-integer parameter values. For instance, when ${a = 2.2, b = 3.3, \alpha = 4.1, \beta = 5.2}$, the above expression returns a value of 0.780101 for the expectation (which is consistent with Monte Carlo simulation).

0
On

$\newcommand{\bbx}[1]{\,\bbox[15px,border:1px groove navy]{\displaystyle{#1}}\,} \newcommand{\braces}[1]{\left\lbrace\,{#1}\,\right\rbrace} \newcommand{\bracks}[1]{\left\lbrack\,{#1}\,\right\rbrack} \newcommand{\dd}{\mathrm{d}} \newcommand{\ds}[1]{\displaystyle{#1}} \newcommand{\expo}[1]{\,\mathrm{e}^{#1}\,} \newcommand{\ic}{\mathrm{i}} \newcommand{\mc}[1]{\mathcal{#1}} \newcommand{\mrm}[1]{\mathrm{#1}} \newcommand{\pars}[1]{\left(\,{#1}\,\right)} \newcommand{\partiald}[3][]{\frac{\partial^{#1} #2}{\partial #3^{#1}}} \newcommand{\root}[2][]{\,\sqrt[#1]{\,{#2}\,}\,} \newcommand{\totald}[3][]{\frac{\mathrm{d}^{#1} #2}{\mathrm{d} #3^{#1}}} \newcommand{\verts}[1]{\left\vert\,{#1}\,\right\vert}$ $\ds{\Large\left.a\right)}$ \begin{align} &\bbox[13px,#ffd]{\int_{0}^{1}{x^{a - 1}\pars{1 - x}^{b - 1} \over \mrm{B}\pars{a,b}}\,x\ln\pars{x}\,\dd x} = \left.{1 \over \mrm{B}\pars{a,b}}\,\partiald{}{\nu} \int_{0}^{1}x^{a + \nu}\pars{1 - x}^{b - 1}\,\dd x\,\right\vert_{\ \nu\ =\ 0} \\[5mm] = &\ \left.{1 \over \mrm{B}\pars{a,b}}\,\partiald{\mrm{B}\pars{a + \nu + 1,b}}{\nu} \,\right\vert_{\ \nu\ =\ 0} = \left.{1 \over \mrm{B}\pars{a,b}}\,\partiald{}{\nu} {\Gamma\pars{a + \nu + 1}\Gamma\pars{b} \over \Gamma\pars{a + \nu + 1 + b}} \,\right\vert_{\ \nu\ =\ 0} \\[5mm] = &\ {\Gamma\pars{b} \over \Gamma\pars{a}\Gamma\pars{b}/\Gamma\pars{a + b}} \bracks{\Gamma\pars{1 + a}\,{H_{a} - H_{a + b} \over \Gamma\pars{1 + a + b}}} \\[5mm] = &\ {\Gamma\pars{a + b} \over \Gamma\pars{a}}\bracks{% a\,\Gamma\pars{a}\,{H_{a} - H_{a + b} \over \pars{a + b}\Gamma\pars{a + b}}} = \bbx{{a \over a + b}\pars{H_{a} - H_{a + b}}} \end{align}


\begin{align} &\bbox[13px,#ffd]{\int_{0}^{1}{x^{a - 1}\pars{1 - x}^{b - 1} \over \mrm{B}\pars{a,b}} \,{1 \over x + 1}\,\dd x} = {1 \over \mrm{B}\pars{a,b}}\int_{0}^{1}x^{a - 1}\pars{1 - x}^{b - 1} \bracks{1 - \pars{-1}x}^{\,-1}\,\dd x \\[5mm] = &\ {1 \over \mrm{B}\pars{a,b}}\bracks{% \mrm{B}\pars{a,b}\,\mbox{}_{2}\mrm{F}_{1}\pars{1,a;a + b;-1}} = \bbx{\mbox{}_{2}\mrm{F}_{1}\pars{1,a;a + b;-1}}\label{1}\tag{1} \end{align}

\eqref{1} is evaluated as an 'Euler Type' expression for the Hypergeometric Function: It's given in this link.


$\ds{\Large\left.b\right)}$ \begin{align} &\bbox[13px,#ffd]{\int_{0}^{\infty}{\beta^{\alpha} \over \Gamma\pars{\alpha}} \,y^{\alpha - 1}\expo{-\beta y}y\ln\pars{y}\,\dd y} = {\beta^{\alpha} \over \Gamma\pars{\alpha}} \left.\partiald{}{\nu}\int_{0}^{\infty}y^{\alpha + \nu}\expo{-\beta y}\,\dd y \,\right\vert_{\ \nu\ =\ 0} \\[5mm] = &\ {\beta^{\alpha} \over \Gamma\pars{\alpha}} \partiald{}{\nu}\bracks{{1 \over \beta^{\alpha + \nu + 1}} \int_{0}^{\infty}y^{\alpha + \nu}\expo{-y}\,\dd y}_{\ \nu\ =\ 0} = {\beta^{\alpha} \over \Gamma\pars{\alpha}} \partiald{}{\nu}\bracks{{\Gamma\pars{\alpha + \nu + 1} \over \beta^{\alpha + \nu + 1}}}_{\ \nu\ =\ 0} \\[5mm] = &\ {\beta^{\alpha} \over \Gamma\pars{\alpha}}\braces{% -\beta^\pars{-1 - \alpha}\,\Gamma\pars{1 + \alpha}\bracks{\ln\pars{\beta} - H_{\alpha} + \gamma}} = \bbx{{\alpha \over \beta}\bracks{H_{\alpha} - \gamma - \ln\pars{\beta}}} \end{align}