Some data (50 iid
standard normal draws)
x = c(-0.027,-0.530,-1.582,-0.431,-0.248,0.478,0.697,1.484,-0.514,1.312,-0.584,0.854,0.473,
-0.691,-0.651,-0.596,0.557,-0.950,-0.006,1.162,0.444,-1.156,-0.880,-1.073,-0.332,
0.824,0.512,0.311,-1.027,-1.069,2.307,-0.126,1.903,-0.197,-0.581,0.170,0.236,0.481,
1.246,0.341,0.664,-0.769,1.017,-0.353,-0.074,-0.515,-0.997,1.073,-0.110,2.526)
Estimation of a few
population quantities
Assuming that the above data is a random sample of size \(n=50\) from a population with mean \(\mu\) and variance \(\sigma^2\). Assuming the data is Gaussian
(normally distributed), we can show that the maximum likelihood
estimators (MLEs) of \(\mu\) and \(\sigma^2\) are, respectively \[
{\widehat \mu}_{MLE} = \bar{x}_n = \frac{1}{n} \sum_{i=1}^n x_i \ \ \
\mbox{and} \ \ \
{\widehat \sigma}_{MLE}^2 = \frac{1}{n} \sum_{i=1}^n (x_i-\bar{x}_n)^2,
\] such that \({\widehat
\sigma}_{MLE}=\sqrt{{\widehat \sigma}_{MLE}^2}\). Finally , the
mean absolute deviation is computed as \[
MAD = \frac{1}{n} \sum_{i=1}^n |x_i-\bar{x}_n|.
\]
n = length(x)
mu.mle = mean(x)
sigma2.mle = mean((x-mu.mle)^2)
sigma.mle = sqrt(sigma2.mle)
mad = mean(abs(x-mu.mle))
MLE for the population mean: 0.10006
MLE for the population variance: 0.8334424
MLE for the population standard deviation: 0.9129307
Mean absolute deviation (MAD): 0.7508248
Sampling
distributions
A few results are well known and easy to show:
\({\widehat \mu}_{MLE}|\mu,\sigma^2
\sim N(\mu,\sigma^2/n)\), so the 95% confidence interval for
\(\mu\) is given by \({\widehat \mu}_{MLE} \pm 1.95996
\sigma/\sqrt{n}\).
\({\widehat \mu}_{MLE}|\mu,{\widehat
\sigma}^2 \sim t_{n-1}(\mu,{\widehat \sigma}^2/n)\), so the 95%
confidence interval for \(\mu\) is
given by \({\widehat \mu}_{MLE} \pm
2.00958{\widehat \sigma}/\sqrt{n}\).
\({\widehat \sigma}_{MLE}^2|\sigma^2
\sim \frac{\sigma^2}{n} \chi_{n-1}^2\). Similarly, a 95%
confidence interval for \(\sigma^2\) is
given by \[
[n{\widehat \sigma}_{MLE}^2/\chi^2_{0.975,n-1};
n{\widehat \sigma}_{MLE}^2/\chi^2_{0.025,n-1}]
\]
\({\widehat \sigma}_{MLE}|\sigma \sim
\sigma \sqrt{\chi_{n-1}^2/n}\) Â Â Â (sampling distribution of
unknown format). A very rough approximation based on the Central Limit
Theorem (CLT) is such that \[
{\widehat \sigma}_{MLE}|\sigma \sim
N(\sigma((n-1)/n)^{1/2},\sigma^2/(2n)).
\]
The CLT also helps showing that \[
MAD | \sigma \overset{a}\sim
N\left[(2\sigma^2/\pi)^{1/2};\frac{\sigma^2(1-2/\pi)}{n}\right] \equiv
N\left[0.7979\sigma;0.3634\sigma^2/n\right].
\] Then, an approximate 95% confidence interval for \(\sigma\) based on the MAD is given by \[
[MAD/(0.7979-0.7122509/\sqrt{n});MAD/(0.7979+0.7122509/\sqrt{n})]
\]
Confidence
intervals
IC.mu = c(mu.mle+qt(c(0.025,0.975),n-1)*sigma.mle/sqrt(n))
IC.sigma2 = c(n*sigma2.mle/qchisq(0.025,n-1),n*sigma2.mle/qchisq(0.975,n-1))
IC.sigma = c(sigma.mle/(sqrt((n-1)/n)+1.96/sqrt(2*n)),sigma.mle/(sqrt((n-1)/n)-1.96/sqrt(2*n)))
IC.sigma1 = c(mad/(0.7979+0.7122509/sqrt(n)),mad/(0.7979-0.7122509/sqrt(n)))
tab = rbind(IC.mu,IC.sigma2,IC.sigma,IC.sigma1)
tab
## [,1] [,2]
## IC.mu -0.1593920 0.3595120
## IC.sigma2 1.3206221 0.5934305
## IC.sigma 0.7697888 1.1498599
## IC.sigma1 0.8355240 1.0769570
Monte Carlo simulation
exercises
set.seed(20102025)
alpha = 0.05 # Level of the confidence interval
mu = 0 # Normal(mu,sigma^2)
sigma = 1
R = 1000 # Replications
par(mfrow=c(3,4))
for (n in c(20,50,100)){
estimators = matrix(0,R,4)
for (r in 1:R){
x = rnorm(n,mu,sigma)
mu.mle = mean(x)
sigma2.mle = mean((x-mu.mle)^2)
sigma.mle = sqrt(sigma2.mle)
mad = mean(abs(x-mu.mle))
estimators[r,] = c(mu.mle,sigma2.mle,sigma.mle,mad)
}
hist(estimators[,1],xlab="mu",main="mu (MLE)",prob=TRUE)
abline(v=mu,col=2,lwd=2)
legend("topright",legend=paste("n = ",n,sep=""),bty="n")
hist(estimators[,2],xlab="sigma2",main="sigma2 (MLE)",prob=TRUE)
abline(v=sigma^2,col=2,lwd=2)
hist(estimators[,3],xlab="sigma",main="sigma (MLE)",prob=TRUE)
abline(v=sigma,col=2,lwd=2)
hist(estimators[,4],xlab="sigma",main="sigma (MAD)",prob=TRUE)
abline(v=sqrt(2/pi)*sigma,col=2,lwd=2)
}

Approximating sampling
distributions via bootstrap
x = c(-0.027,-0.530,-1.582,-0.431,-0.248,0.478,0.697,1.484,-0.514,
1.312,-0.584,0.854,0.473,-0.691,-0.651,-0.596,0.557,-0.950,
-0.006,1.162,0.444,-1.156,-0.880,-1.073,-0.332,0.824,0.512,
0.311,-1.027,-1.069,2.307,-0.126,1.903,-0.197,-0.581,0.170,
0.236,0.481,1.246,0.341,0.664,-0.769,1.017,-0.353,-0.074,
-0.515,-0.997,1.073,-0.110,2.526)
n = length(x)
mu0.mle = mean(x)
sigma20.mle = mean((x-mu0.mle)^2)
sigma0.mle = sqrt(sigma20.mle)
mad0 = mean(abs(x-mu0.mle))
set.seed(3141593)
R = 10000 # Bootstrap replications
estimators = matrix(0,R,2)
for (r in 1:R){
x1 = sample(x,size=n,replace=TRUE)
mu.mle = mean(x1)
sigma2.mle = mean((x1-mu.mle)^2)
estimators[r,] = c(mu.mle,sigma2.mle)
}
quantiles = apply(estimators,2,quantile,c(0.025,0.975))
par(mfrow=c(1,2))
hist(estimators[,1],xlab="mu",main="mu (MLE)",prob=TRUE)
abline(v=mu0.mle,col=2,lwd=4)
abline(v=mean(estimators[,1]),lwd=4)
segments(IC.mu[1],0,IC.mu[2],0,col=2,lwd=4)
segments(quantiles[1,1],0.1,quantiles[2,1],0.1,lwd=4)
legend("topright",legend=c("Exact","Bootstrap"),col=2:1,lwd=4,bty="n")
hist(estimators[,2],xlab="sigma2",main="sigma2 (MLE)",prob=TRUE)
abline(v=sigma20.mle,col=2,lwd=4)
abline(v=mean(estimators[,2]),lwd=4)
segments(IC.sigma2[1],0,IC.sigma2[2],0,col=2,lwd=4)
segments(quantiles[1,2],0.1,quantiles[2,2],0.1,lwd=4)

Notice that the exact confidence intervals are relatively close to
the bootstrap ones, but they do not match. The intervals are almost
identical for the estimator of \(\mu\).
For \(\sigma^2\), the exact sampling
distribution is a \(\chi^2\), which
skewed, while the bootstrap approximation resembles a Gaussian
distribution. The differences decrease when the sample size \(n\) increases and the bootstrap will
eventually converse to the sampling distribution of the estimator.
---
title: "Monte Carlo Methods"
author: "Hedibert Freitas Lopes"
date: "20/10/2025"
output:
  html_document:
    toc: true
    toc_depth: 3
    toc_collapsed: true
    code_download: true
    number_sections: true
  pdf_document:
    toc: true
    toc_depth: '3'
subtitle: MC simulation and the boostrap
---

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

# Some data (50 iid standard normal draws)
```{r comment=NA}
x = c(-0.027,-0.530,-1.582,-0.431,-0.248,0.478,0.697,1.484,-0.514,1.312,-0.584,0.854,0.473,
      -0.691,-0.651,-0.596,0.557,-0.950,-0.006,1.162,0.444,-1.156,-0.880,-1.073,-0.332,
      0.824,0.512,0.311,-1.027,-1.069,2.307,-0.126,1.903,-0.197,-0.581,0.170,0.236,0.481,
      1.246,0.341,0.664,-0.769,1.017,-0.353,-0.074,-0.515,-0.997,1.073,-0.110,2.526)
```

## Estimation of a few population quantities
Assuming that the above data is a random sample of size $n=50$ from a population with mean $\mu$ and variance $\sigma^2$.  Assuming the data is Gaussian (normally distributed), we can show that the maximum likelihood estimators (MLEs) of $\mu$ and $\sigma^2$ are, respectively
$$
{\widehat \mu}_{MLE} = \bar{x}_n = \frac{1}{n} \sum_{i=1}^n x_i \ \ \ \mbox{and} \ \ \ 
{\widehat \sigma}_{MLE}^2 = \frac{1}{n} \sum_{i=1}^n (x_i-\bar{x}_n)^2,
$$
such that ${\widehat \sigma}_{MLE}=\sqrt{{\widehat \sigma}_{MLE}^2}$.  Finally , the mean absolute deviation is computed as 
$$
MAD = \frac{1}{n} \sum_{i=1}^n |x_i-\bar{x}_n|.
$$
```{r}
n = length(x)
mu.mle = mean(x)
sigma2.mle = mean((x-mu.mle)^2)
sigma.mle = sqrt(sigma2.mle)
mad = mean(abs(x-mu.mle))
```

```{r comment=NA, echo=FALSE, fig.align='center', fig.width=12, fig.height=4}
cat(
" MLE for the population mean:", mu.mle, "\n",
"MLE for the population variance:", sigma2.mle, "\n",
"MLE for the population standard deviation:", sigma.mle, "\n",
"Mean absolute deviation (MAD):",mad, "\n"
)
```


# Sampling distributions 
A few results are well known and easy to show:

* ${\widehat \mu}_{MLE}|\mu,\sigma^2 \sim N(\mu,\sigma^2/n)$, so the 95\% confidence interval for $\mu$ is given by ${\widehat \mu}_{MLE} \pm 1.95996 \sigma/\sqrt{n}$.

* ${\widehat \mu}_{MLE}|\mu,{\widehat \sigma}^2 \sim t_{n-1}(\mu,{\widehat \sigma}^2/n)$, so the 95\% confidence interval for $\mu$ is given by ${\widehat \mu}_{MLE} \pm 2.00958{\widehat \sigma}/\sqrt{n}$.

* ${\widehat \sigma}_{MLE}^2|\sigma^2 \sim \frac{\sigma^2}{n} \chi_{n-1}^2$.  Similarly, a 95\% confidence interval for $\sigma^2$ is given by 
$$
[n{\widehat \sigma}_{MLE}^2/\chi^2_{0.975,n-1};
n{\widehat \sigma}_{MLE}^2/\chi^2_{0.025,n-1}]
$$

* ${\widehat \sigma}_{MLE}|\sigma \sim \sigma \sqrt{\chi_{n-1}^2/n}$ \ \ \ (sampling distribution of unknown format).  A very rough approximation based on the Central Limit Theorem (CLT) is such that 
$$
{\widehat \sigma}_{MLE}|\sigma \sim N(\sigma((n-1)/n)^{1/2},\sigma^2/(2n)).
$$

* The CLT also helps showing that 
$$
MAD | \sigma \overset{a}\sim N\left[(2\sigma^2/\pi)^{1/2};\frac{\sigma^2(1-2/\pi)}{n}\right] \equiv N\left[0.7979\sigma;0.3634\sigma^2/n\right].
$$
Then, an approximate 95\% confidence interval for $\sigma$ based on the MAD is given by
$$
[MAD/(0.7979-0.7122509/\sqrt{n});MAD/(0.7979+0.7122509/\sqrt{n})]
$$

## Confidence intervals
```{r}
IC.mu = c(mu.mle+qt(c(0.025,0.975),n-1)*sigma.mle/sqrt(n))
IC.sigma2 = c(n*sigma2.mle/qchisq(0.025,n-1),n*sigma2.mle/qchisq(0.975,n-1))
IC.sigma = c(sigma.mle/(sqrt((n-1)/n)+1.96/sqrt(2*n)),sigma.mle/(sqrt((n-1)/n)-1.96/sqrt(2*n)))
IC.sigma1 = c(mad/(0.7979+0.7122509/sqrt(n)),mad/(0.7979-0.7122509/sqrt(n)))

tab = rbind(IC.mu,IC.sigma2,IC.sigma,IC.sigma1)
tab
```



# Monte Carlo simulation exercises
```{r fig.align='center', fig.width=16, fig.height=12}
set.seed(20102025)
alpha = 0.05      # Level of the confidence interval
mu     = 0           # Normal(mu,sigma^2)
sigma = 1
R        = 1000     # Replications

par(mfrow=c(3,4))
for (n in c(20,50,100)){
  estimators = matrix(0,R,4)
  for (r in 1:R){
    x = rnorm(n,mu,sigma)
    mu.mle = mean(x)
    sigma2.mle = mean((x-mu.mle)^2)
    sigma.mle = sqrt(sigma2.mle)
    mad = mean(abs(x-mu.mle))
    estimators[r,] = c(mu.mle,sigma2.mle,sigma.mle,mad)
  }
  hist(estimators[,1],xlab="mu",main="mu (MLE)",prob=TRUE)
  abline(v=mu,col=2,lwd=2)
  legend("topright",legend=paste("n = ",n,sep=""),bty="n")
  hist(estimators[,2],xlab="sigma2",main="sigma2 (MLE)",prob=TRUE)
  abline(v=sigma^2,col=2,lwd=2)
  hist(estimators[,3],xlab="sigma",main="sigma (MLE)",prob=TRUE)
  abline(v=sigma,col=2,lwd=2)
  hist(estimators[,4],xlab="sigma",main="sigma (MAD)",prob=TRUE)
  abline(v=sqrt(2/pi)*sigma,col=2,lwd=2)
}
```



# Approximating sampling distributions via bootstrap
```{r fig.align='center', fig.width=10, fig.height=5}
x = c(-0.027,-0.530,-1.582,-0.431,-0.248,0.478,0.697,1.484,-0.514,
          1.312,-0.584,0.854,0.473,-0.691,-0.651,-0.596,0.557,-0.950,
          -0.006,1.162,0.444,-1.156,-0.880,-1.073,-0.332,0.824,0.512,
          0.311,-1.027,-1.069,2.307,-0.126,1.903,-0.197,-0.581,0.170,
          0.236,0.481,1.246,0.341,0.664,-0.769,1.017,-0.353,-0.074,
          -0.515,-0.997,1.073,-0.110,2.526)
n = length(x)
mu0.mle = mean(x)
sigma20.mle = mean((x-mu0.mle)^2)
sigma0.mle = sqrt(sigma20.mle)
mad0 = mean(abs(x-mu0.mle))

set.seed(3141593)
R = 10000  # Bootstrap replications
estimators = matrix(0,R,2)
for (r in 1:R){
  x1 = sample(x,size=n,replace=TRUE)
  mu.mle = mean(x1)
  sigma2.mle = mean((x1-mu.mle)^2)
  estimators[r,] = c(mu.mle,sigma2.mle)
}

quantiles = apply(estimators,2,quantile,c(0.025,0.975))

par(mfrow=c(1,2))
hist(estimators[,1],xlab="mu",main="mu (MLE)",prob=TRUE)
abline(v=mu0.mle,col=2,lwd=4)
abline(v=mean(estimators[,1]),lwd=4)
segments(IC.mu[1],0,IC.mu[2],0,col=2,lwd=4)
segments(quantiles[1,1],0.1,quantiles[2,1],0.1,lwd=4)
legend("topright",legend=c("Exact","Bootstrap"),col=2:1,lwd=4,bty="n")

hist(estimators[,2],xlab="sigma2",main="sigma2 (MLE)",prob=TRUE)
abline(v=sigma20.mle,col=2,lwd=4)
abline(v=mean(estimators[,2]),lwd=4)
segments(IC.sigma2[1],0,IC.sigma2[2],0,col=2,lwd=4)
segments(quantiles[1,2],0.1,quantiles[2,2],0.1,lwd=4)
```

Notice that the exact confidence intervals are relatively close to the bootstrap ones, but they do not match.  The intervals are almost identical for the estimator of $\mu$.  For $\sigma^2$, the exact sampling distribution is a $\chi^2$, which skewed, while the bootstrap approximation resembles a Gaussian distribution.  The differences decrease when the sample size $n$ increases and the bootstrap will eventually converse to the sampling distribution of the estimator.
