1 Gaussian homoscedastic linear model

We observe \(n\) pairs of observations, \((y_i,x_i)\), such that \[ \mbox{data} = \{(y_1,x_1),\ldots,(y_n,x_n)\}. \] The model that relates \(y\)s and the \(x\)s is a Gaussian homoscedastic linear model: \[ y_i = \beta x_i + \varepsilon_i \qquad \varepsilon_i \sim N(0,\sigma^2), \] with \(E(\varepsilon_i\varepsilon_j)=0\) for all \(i \neq j\). The likelihood function can be written as \[\begin{eqnarray*} L(\beta,\sigma^2|\mbox{data}) &=& \prod_{i=1}^n \frac{1}{\sqrt{2\pi\sigma^2}}\exp\left\{-\frac12\frac{(y_i-\beta x_i)^2}{\sigma^2}\right\}\\ &\propto& (\sigma^2)^{-n/2}\exp\left\{-\frac12\frac{\sum_{i=1}^n (y_i-\beta x_i)^2}{\sigma^2}\right\} \end{eqnarray*}\]

2 Prior

In this model, the two unknown quantities are the slope parameter \(\beta\) and the residual variance, \(\sigma^2\). We will assume conditionally conjugate priors as follows: \[ \beta \sim N(b_0,V_0) \ \ \ \mbox{and} \ \ \ \sigma^2 \sim IG(c_0,d_0), \] such that \[ p(\beta,\sigma^2) = p(\beta)p(\sigma^2) = \left[\frac{1}{\sqrt{2\pi V_0}}\exp\left\{-0.5\frac{(\beta-b_0)^2}{V_0}\right\}\right] \left[ \frac{d_0^{c_0}}{\Gamma(c_0)}(\sigma^2)^{-(c_0+1)}\exp\left\{-\frac{d_0}{\sigma^2}\right\}\right]. \]

3 Posterior distribution

The posterior distribution of \((\beta,\sigma^2)\) \[ p(\beta,\sigma^2|\mbox{data}) \propto p(\beta)p(\sigma^2)L(\beta,\sigma^2|\mbox{data}), \] does not belong to any known family of bivariate distributions and, consequently, there are not closed form answers to questions such as the following:

4 Gibbs-assisted posterior inference

The Gibbs sampler is a Markov Chain Monte Carlo (MCMC) scheme that samples from the distribution of interest (aka target distribution), in our case the posterior \(p(\beta,\sigma^2|\mbox{data})\), by iteratively sampling from the full conditional distributions: \[ p(\beta|\sigma^2,\mbox{data}) \ \ \ \mbox{and} \ \ \ p(\sigma^2|\beta,\mbox{data}). \] The beauty of the Gibbs sampler, and therefore of all MCMC schemes, is that it essentially breaks down the complexicity of a given model into the complexities of smaller models where blocks of parameters are kept fixed.

4.1 \(p(\sigma^2|\beta,\mbox{data})\)

In this full conditional distribution, the parameter \(\beta\) is treated as known. Therefore, we could define \(z_i = y_i-\beta x_i\) and the model becomes \[ z_1,\ldots,z_n \ \ iid \ \ N(0,\sigma^2). \] In this case, \[ p(\sigma^2|z_1,\ldots,z_n) \propto (\sigma^2)^{-(c_0+1)}\exp\left\{-\frac{d_0}{\sigma^2}\right\} (\sigma^2)^{-n/2}\exp\left\{-\frac{\sum_{i=1}^n z_i^2/2}{\sigma^2}\right\}, \] which resembles an inverse gamma distribution with hyperparameters \[ c_1 = c_0+\frac{n}{2} \ \ \ \mbox{and} \ \ \ d_1 = d_0 + \frac{\sum_{i=1}^n z_i^2}{2} = d_0 + \frac{\sum_{i=1}^n (y_i-\beta x_i)^2}{2}, \] or \(\sigma^2|\beta,\mbox{data} \sim IG(c_1,d_1)\).

sample.sigma2 = function(beta,c0,d0,y,x){
  c1 = c0+n/2
  d1 = d0+sum((y-x*beta)^2)/2
  return(1/rgamma(1,c1,d1))
}

4.2 \(p(\beta|\sigma^2,\mbox{data})\)

Similarly, assuming that \(\sigma^2\) is known, we have a simpler model,i.e. a Gaussian regression model with an unknown slope, \(\beta\), but known residual variance, \(\sigma^2\). In this case, \[\begin{eqnarray*} p(\beta|\sigma^2,\mbox{data}) &\propto& \exp\{-0.5(\beta-b_0)^2/V_0\}\exp\left\{-0.5\sum_{i=1}^n (y_i-\beta x_i)^2/\sigma^2\right\}\\ &\propto& \exp\left\{-0.5\left[\beta^2/V_0-2\beta b_0/V_0+\beta^2s_x^2/\sigma^2 -2\beta s_{xy}/\sigma^2\right]\right\}\\ &\propto& \exp\left\{-0.5\left[\beta^2(1/V_0+s_x^2/\sigma^2)-2\beta(b_0/V_0+s_{xy}/\sigma^2) \right]\right\}, \end{eqnarray*}\] where \(s_x^2 = \sum_{i=1}^n x_i^2\) and \(s_{xy} = \sum_{i=1}^n y_i x_i\). It is now easy to see that \[ \beta|\sigma^2,\mbox{data} \sim N(b_1,V_1), \] where \(V_1=1/(1/V_0+s_x^2/\sigma^2)\) and \[ b_1 = V_1(b_0/V_0+s_{xy}/\sigma^2) \]

sample.beta = function(sigma2,b0,V0,sx2,sxy){
  V1 = 1/(1/V0+sx2/sigma2)
  b1 = V1*(b0/V0+sxy/sigma2)
  return(rnorm(1,b1,sqrt(V1)))
}

5 Turning the Bayesian crank

5.1 Simulating some data

n = 50
x = runif(n,0,3)
y = 0.75*x+rnorm(n)
plot(x,y)

sx2 = sum(x^2)
sxy = sum(x*y)

5.2 Setting up the hyperparameters

b0 = 0
V0 = 9
c0 = 1/2
d0 = 1/2

par(mfrow=c(1,2))
sig2 = seq(0.0001,10,length=1000)
plot(sig2,dgamma(1/sig2,c0,d0)/(sig2^2),xlab=expression(sigma^2),ylab="Prior density",type="l")
beta = seq(-10,10,length=1000)
plot(beta,dnorm(beta,b0,sqrt(V0)),xlab=expression(beta),ylab="Prior density",type="l")

5.3 Setting up the MCMC scheme

beta.initial = 0

n.burn  = 1000
n.draws = 1000
step    = 1
niter   = n.burn+n.draws*step

5.4 Running the Gibbs sampler

beta = beta.initial
draws = matrix(0,niter,2)
for (iter in 1:niter){
  sigma2 = sample.sigma2(beta,c0,d0,y,x)
  beta   = sample.beta(sigma2,b0,V0,sx2,sxy)
  draws[iter,] = c(beta,sqrt(sigma2))
}

5.5 MCMC output

par(mfrow=c(2,3))
ts.plot(draws[,1],ylab="",main=expression(beta),xlab="Iterations")
acf(draws[,1],main="")
hist(draws[,1],prob=TRUE,main="",xlab=expression(beta))

ts.plot(draws[,2],ylab="",main=expression(sigma),xlab="Iterations")
acf(draws[,2],main="")
hist(draws[,2],prob=TRUE,main="",xlab=expression(sigma))

5.6 Comparing priors and posteriors

beta = seq(-10,10,length=1000)
sig2 = seq(0.0001,10,length=1000)
par(mfrow=c(1,2))
plot(density(draws[,1]),xlab=expression(beta),main="",ylab="Density",lwd=2)
lines(beta,dnorm(beta,b0,sqrt(V0)),col=2,lwd=2)
abline(v=0.75,col=4,lwd=2)
plot(density(draws[,2]^2),xlab=expression(sigma^2),main="",ylab="Density",xlim=c(0,4),lwd=2)
lines(sig2,dgamma(1/sig2,c0,d0)/(sig2^2),col=2,lwd=2)
abline(v=1,col=4,lwd=2)
legend("topright",legend=c("Prior","Posterior","True value"),col=c(2,1,4),bty="n",lty=1,lwd=2)

5.7 What is \(E(\beta|\mbox{data})\)?

mean(draws[,1])
## [1] 0.6707462

5.8 What is \(Pr(\sigma>1|\mbox{data})\)?

mean(draws[,2]>1)
## [1] 0.707
---
title: "Bayesian linear regression"
subtitle: "Gibbs sampler in action"
author: "Hedibert Freitas Lopes"
date: "5/27/2023"
output:
  html_document:
    toc: true
    toc_depth: 2
    code_download: yes
    number_sections: true
---

```{r setup, include=FALSE}
knitr::opts_chunk$set(echo = TRUE)
```

# Gaussian homoscedastic linear model
We observe $n$ pairs of observations, $(y_i,x_i)$, such that
$$
\mbox{data} = \{(y_1,x_1),\ldots,(y_n,x_n)\}.
$$
The model that relates $y$s and the $x$s is a Gaussian homoscedastic linear model:
$$
y_i = \beta x_i + \varepsilon_i \qquad \varepsilon_i \sim N(0,\sigma^2),
$$
with $E(\varepsilon_i\varepsilon_j)=0$ for all $i \neq j$.  The likelihood function can be written as
\begin{eqnarray*}
L(\beta,\sigma^2|\mbox{data}) &=& \prod_{i=1}^n
\frac{1}{\sqrt{2\pi\sigma^2}}\exp\left\{-\frac12\frac{(y_i-\beta x_i)^2}{\sigma^2}\right\}\\
&\propto& (\sigma^2)^{-n/2}\exp\left\{-\frac12\frac{\sum_{i=1}^n (y_i-\beta x_i)^2}{\sigma^2}\right\}
\end{eqnarray*}

# Prior
In this model, the two unknown quantities are the slope parameter $\beta$ and the residual variance, $\sigma^2$.  We will assume conditionally conjugate priors as follows:
$$
\beta \sim N(b_0,V_0) \ \ \ \mbox{and} \ \ \ \sigma^2 \sim IG(c_0,d_0),
$$
such that 
$$
p(\beta,\sigma^2) = p(\beta)p(\sigma^2) = \left[\frac{1}{\sqrt{2\pi V_0}}\exp\left\{-0.5\frac{(\beta-b_0)^2}{V_0}\right\}\right] \left[
\frac{d_0^{c_0}}{\Gamma(c_0)}(\sigma^2)^{-(c_0+1)}\exp\left\{-\frac{d_0}{\sigma^2}\right\}\right].
$$

# Posterior distribution
The posterior distribution of $(\beta,\sigma^2)$ 
$$
p(\beta,\sigma^2|\mbox{data}) \propto p(\beta)p(\sigma^2)L(\beta,\sigma^2|\mbox{data}),
$$
does not belong to any known family of bivariate distributions and, consequently, there are not closed form answers to questions such as the following:

* What is $E(\beta|\mbox{data})$?

* What is $Pr(\sigma>1|\mbox{data})$?

# Gibbs-assisted posterior inference
The Gibbs sampler is a Markov Chain Monte Carlo (MCMC) scheme that samples from the distribution of interest (aka target distribution), in our case the posterior $p(\beta,\sigma^2|\mbox{data})$, by iteratively sampling from the full conditional distributions:
$$
p(\beta|\sigma^2,\mbox{data}) \ \ \ \mbox{and} \ \ \ 
p(\sigma^2|\beta,\mbox{data}).
$$
The beauty of the Gibbs sampler, and therefore of all MCMC schemes, is that it essentially breaks down the complexicity of a given model into the complexities of smaller models where blocks of parameters are kept fixed.

## $p(\sigma^2|\beta,\mbox{data})$
In this full conditional distribution, the parameter $\beta$ is treated as known.  Therefore, we could define $z_i = y_i-\beta x_i$ and the model becomes
$$
z_1,\ldots,z_n \ \ iid \ \ N(0,\sigma^2).
$$
In this case,
$$
p(\sigma^2|z_1,\ldots,z_n) \propto (\sigma^2)^{-(c_0+1)}\exp\left\{-\frac{d_0}{\sigma^2}\right\}
(\sigma^2)^{-n/2}\exp\left\{-\frac{\sum_{i=1}^n z_i^2/2}{\sigma^2}\right\},
$$
which resembles an inverse gamma distribution with hyperparameters
$$
c_1 = c_0+\frac{n}{2} \ \ \ \mbox{and} \ \ \ d_1 = d_0 + \frac{\sum_{i=1}^n z_i^2}{2}
= d_0 + \frac{\sum_{i=1}^n (y_i-\beta x_i)^2}{2},
$$
or $\sigma^2|\beta,\mbox{data} \sim IG(c_1,d_1)$.

```{r}
sample.sigma2 = function(beta,c0,d0,y,x){
  c1 = c0+n/2
  d1 = d0+sum((y-x*beta)^2)/2
  return(1/rgamma(1,c1,d1))
}
```


## $p(\beta|\sigma^2,\mbox{data})$
Similarly, assuming that $\sigma^2$ is known, we have a simpler model,i.e. a Gaussian regression model with an unknown slope, $\beta$, but known residual variance, $\sigma^2$.  In this case,
\begin{eqnarray*}
p(\beta|\sigma^2,\mbox{data}) &\propto& \exp\{-0.5(\beta-b_0)^2/V_0\}\exp\left\{-0.5\sum_{i=1}^n (y_i-\beta x_i)^2/\sigma^2\right\}\\
&\propto&
\exp\left\{-0.5\left[\beta^2/V_0-2\beta b_0/V_0+\beta^2s_x^2/\sigma^2 -2\beta s_{xy}/\sigma^2\right]\right\}\\
&\propto& 
\exp\left\{-0.5\left[\beta^2(1/V_0+s_x^2/\sigma^2)-2\beta(b_0/V_0+s_{xy}/\sigma^2) \right]\right\},
\end{eqnarray*}
where $s_x^2 = \sum_{i=1}^n x_i^2$ and $s_{xy} = \sum_{i=1}^n y_i x_i$.  It is now easy to see that
$$
\beta|\sigma^2,\mbox{data} \sim N(b_1,V_1),
$$
where $V_1=1/(1/V_0+s_x^2/\sigma^2)$ and 
$$
b_1 = V_1(b_0/V_0+s_{xy}/\sigma^2)
$$
```{r}
sample.beta = function(sigma2,b0,V0,sx2,sxy){
  V1 = 1/(1/V0+sx2/sigma2)
  b1 = V1*(b0/V0+sxy/sigma2)
  return(rnorm(1,b1,sqrt(V1)))
}
```

# Turning the Bayesian crank

## Simulating some data
```{r fig.width=6, fig.height=6, fig.align='center'}
n = 50
x = runif(n,0,3)
y = 0.75*x+rnorm(n)
plot(x,y)

sx2 = sum(x^2)
sxy = sum(x*y)
```


## Setting up the hyperparameters
```{r fig.width=8, fig.height=4, fig.align='center'}
b0 = 0
V0 = 9
c0 = 1/2
d0 = 1/2

par(mfrow=c(1,2))
sig2 = seq(0.0001,10,length=1000)
plot(sig2,dgamma(1/sig2,c0,d0)/(sig2^2),xlab=expression(sigma^2),ylab="Prior density",type="l")
beta = seq(-10,10,length=1000)
plot(beta,dnorm(beta,b0,sqrt(V0)),xlab=expression(beta),ylab="Prior density",type="l")
```

## Setting up the MCMC scheme
```{r}
beta.initial = 0

n.burn  = 1000
n.draws = 1000
step    = 1
niter   = n.burn+n.draws*step
```

## Running the Gibbs sampler
```{r}
beta = beta.initial
draws = matrix(0,niter,2)
for (iter in 1:niter){
  sigma2 = sample.sigma2(beta,c0,d0,y,x)
  beta   = sample.beta(sigma2,b0,V0,sx2,sxy)
  draws[iter,] = c(beta,sqrt(sigma2))
}
```

## MCMC output
```{r fig.width=8, fig.height=6, fig.align='center'}
par(mfrow=c(2,3))
ts.plot(draws[,1],ylab="",main=expression(beta),xlab="Iterations")
acf(draws[,1],main="")
hist(draws[,1],prob=TRUE,main="",xlab=expression(beta))

ts.plot(draws[,2],ylab="",main=expression(sigma),xlab="Iterations")
acf(draws[,2],main="")
hist(draws[,2],prob=TRUE,main="",xlab=expression(sigma))
```

## Comparing priors and posteriors
```{r fig.width=8, fig.height=4, fig.align='center'}
beta = seq(-10,10,length=1000)
sig2 = seq(0.0001,10,length=1000)
par(mfrow=c(1,2))
plot(density(draws[,1]),xlab=expression(beta),main="",ylab="Density",lwd=2)
lines(beta,dnorm(beta,b0,sqrt(V0)),col=2,lwd=2)
abline(v=0.75,col=4,lwd=2)
plot(density(draws[,2]^2),xlab=expression(sigma^2),main="",ylab="Density",xlim=c(0,4),lwd=2)
lines(sig2,dgamma(1/sig2,c0,d0)/(sig2^2),col=2,lwd=2)
abline(v=1,col=4,lwd=2)
legend("topright",legend=c("Prior","Posterior","True value"),col=c(2,1,4),bty="n",lty=1,lwd=2)
```

## What is $E(\beta|\mbox{data})$?
```{r}
mean(draws[,1])
```

## What is $Pr(\sigma>1|\mbox{data})$?
```{r}
mean(draws[,2]>1)
```
