We saw previously that when linear models are fitted to time series
data, the residuals can display autocorrelation. The consequences of
autocorrelation are that
standard errors given by standard least squares theory (and hence
by standard R output) will usually be smaller than the true standard
deviations of the parameter estimates.
the result is that t-test statistics will be inflated,
p-values too small, and confidence intervals will be too
narrow.
Accounting for Autocorrelation in the Errors
The consequence of standard errors and p-values being out means that
we need to account for autocorrelation in the errors when it is
present.
This will require two steps:
- Definition of an appropriate model for autocorrelated errors;
- Fitting the linear model with autocorrelated errors.
We now consider modeling the errors using autoregressive models.
Autoregressive Models
In a time series, the errors \(\varepsilon_1, \varepsilon_2, \ldots,
\varepsilon_n\) can be thought of as a realization of a random
process (in time).
We can model serial correlation between these errors by making each
one explicitly dependent on the previous one: \[\varepsilon_t = \phi \varepsilon_{t-1} +
\eta_t\] where \(\eta_t~(t=1,2,\ldots,n)\) is white
noise, that is, a sequence of independent and identically
distributed (normal) random variables with zero mean.
- This equation is a first order autoregressive (or
AR1) model for \(\varepsilon_t\).
- Under this model, \(\mbox{Corr}(\varepsilon_t, \varepsilon_{t-1}) =
\phi\).
- Consequently, more generally, \(\mbox{Corr}(\varepsilon_t, \varepsilon_{t-k}) =
\phi^k\)
ACF Plots for AR1 Processes
To illustrate an ACF plot for a function demonstrating
autocorrelation, we create two variables from white noise
Z1 = rnorm(1000)
X1 = Z1[-1] + 0.85 * Z1[-1000]
X2 = Z1[-1] - 0.85 * Z1[-1000]
par(mfrow = c(1, 2), mai = rep(0.5, 4))
plot(X1, type = "l")
plot(X2, type = "l")
par(mfrow = c(1, 2))
acf(X1)
acf(X2)
The X1
series has correlation of 0.502 at lag 1, while
the X2
series has autocorrelation of -0.478 at lag1
Autoregressive Models for Errors in Linear Modelling
If residuals in a linear model for time series data display
autocorrelation then we change the model to allow for an AR1 correlation
structure for the residuals in our model to account for this.
N.B. More complex models are also possible. For example:
- AR models of order q>1, where \(\varepsilon_t\) is modelled as explicitly
dependent on the previous q errors;
- moving average (MA) models and autoregressive moving average (ARMA)
models.
- For the purposes of this course we will focus on AR1 models for the
error process.
Application to the Tourism Data
Download motel.csv
## tourism <- read_csv(file = "motel.csv")
tourism <- tourism |>
mutate(Time = round(time_length(Date - min(Date), unit = "month")), Month = factor(month(Date,
label = TRUE), ordered = FALSE), Year = year(Date))
tourism
# A tibble: 180 × 6
Date RoomNights AvePrice Time Month Year
<date> <dbl> <dbl> <dbl> <fct> <dbl>
1 1980-01-01 276986 27.7 0 Jan 1980
2 1980-02-01 260633 28.7 1 Feb 1980
3 1980-03-01 291551 28.6 2 Mar 1980
4 1980-04-01 275383 28.3 3 Apr 1980
5 1980-05-01 275302 28.7 4 May 1980
6 1980-06-01 231693 28.6 5 Jun 1980
7 1980-07-01 238829 29.2 6 Jul 1980
8 1980-08-01 274215 29.8 7 Aug 1980
9 1980-09-01 277808 29.6 8 Sep 1980
10 1980-10-01 299060 30.3 9 Oct 1980
# ℹ 170 more rows
tourism.lm <- lm(RoomNights ~ Time + Month, data = tourism)
acf(resid(tourism.lm))
There is a suggestion of exponential decay in autocorrelations. - AR1
model (with positive \(\phi\)) for
errors seems reasonable.
The model incorporating the AR1 error process, and written in
regression format, is as follows:
\[\begin{aligned}
Y_{t} &= \beta_0 + \beta_1 \mbox{Time} + \beta_2 z_{t,2} + \beta_3
z_{t,3}
+ \ldots + \beta_{12} z_{t,12} + \varepsilon_t \\
\varepsilon_t &= \phi \varepsilon_{t-1} +
\eta_{t}\end{aligned}\]
where:
- \(Y_t\) is the \(t\)th observation of
RoomNights
;
- \(z_{t,j} = 1\) if observation
\(t\) is taken in month \(j\);
- \(z_{t,j} = 0\) otherwise.
- \(\eta_1, \ldots, \eta_n\) are
independent and identically distributed normal random variables with
mean zero.
Model Fitting with Autoregressive Errors
To fit a model with AR1 errors, we must:
- Estimate the size of the autocorrelation parameter, \(\phi\).
- Account for the autocorrelation in errors when estimating the
regression coefficients.
The AR1 parameter, \(\phi\), can be
estimated by the method of (restricted) maximum likelihood.
The details are beyond the scope of this paper, but you will meet
maximum likelihood estimation if you take 161.304 or 161.331.
Once \(\phi\) is estimated, we can
account for the AR1 nature of the errors by fitting the linear model
using generalized least squares.
Generalized Least Squares
Once we have \(\phi\) estimated, we
can then estimate the regression coefficients \(\beta\) by rearranging the regression
equation to eliminate the autocorrelation:
Suppose \[
\begin{aligned}
y_t &= \beta_0 + \beta_1 x_t + \varepsilon_t\\
\varepsilon_t &= \phi \varepsilon_{t-1} + \eta_t
\end{aligned}
\] where \(\eta_t
\underset{\mathsf{iid}}\sim N(0, 1)\). Then \[
\begin{aligned}
y_t - \phi y_{t-1} &= \beta_0 + \beta_1 x_t + \varepsilon_t - \phi
(\beta_0 + \beta_1 x_{t-1} + \varepsilon_{t-1})\\
&= \beta_0(1 - \phi) + \beta_1 (x_t - \phi x_{t-1}) + \varepsilon_t
- \phi \varepsilon_{t-1}\\
&= \beta_0(1 - \phi) + \beta_1 (x_t - \phi x_{t-1}) + \eta_t
\end{aligned}
\] which is a standard linear regression in the new variables
\(Y_t = y_t - \phi y_{t-1}\), \(X_t = x_t - \phi x_{t-1}\).
Thus we can fit this with least squares. The “generalised” bit is the
trick we use to transform something that is not regular least squares to
a least squares situation - it turns out we can do this no matter what
the covariance structure is among the predictors as long as the
structure is estimable from the data.
Generalized Least Squares in R
In R, linear models can be fitted using this technique using the
gls()
command found in the nlme
add-on
package.
Call this package using library(nlme)
before using the
gls()
command.
- The
gls()
command uses the same model formula as
lm()
, but also accepts an additional argument to describe
the correlation structure for the errors.
Generalized Least Squares and the Tourism Data
tourism.gls <- gls(RoomNights ~ Time + Month, correlation = corAR1(), data = tourism)
anova(tourism.gls)
Denom. DF: 167
numDF F-value p-value
(Intercept) 1 45239.15 <.0001
Time 1 1092.85 <.0001
Month 11 81.94 <.0001
The use of an AR1 error process is obtained by setting
correlation=corAR1()
in the gls()
command.
Both Time
and Month
are associated with
RoomNights (P-value less than \(0.0001\) in both cases).
Generalized least squares fit by REML
Model: RoomNights ~ Time + Month
Data: tourism
AIC BIC logLik
3727.911 3774.681 -1848.955
Correlation Structure: AR(1)
Formula: ~1
Parameter estimate(s):
Phi
0.392721
Coefficients:
Value Std.Error t-value p-value
(Intercept) 275492.20 4692.407 58.71021 0.0000
Time 1062.25 31.870 33.33115 0.0000
MonthFeb -31194.09 4205.044 -7.41825 0.0000
MonthMar 23482.73 4959.531 4.73487 0.0000
MonthApr -2170.47 5225.494 -0.41536 0.6784
MonthMay -19419.12 5325.710 -3.64630 0.0004
MonthJun -65827.11 5362.987 -12.27434 0.0000
MonthJul -44522.34 5373.207 -8.28599 0.0000
MonthAug -29768.74 5365.559 -5.54812 0.0000
MonthSep -12039.27 5331.948 -2.25795 0.0252
MonthOct 26393.95 5238.620 5.03834 0.0000
MonthNov 16471.67 4988.022 3.30224 0.0012
MonthDec -58631.94 4272.401 -13.72342 0.0000
Correlation:
(Intr) Time MnthFb MnthMr MnthAp MnthMy MnthJn MnthJl MnthAg MnthSp
Time -0.586
MonthFeb -0.447 0.003
MonthMar -0.525 -0.001 0.589
MonthApr -0.551 -0.005 0.462 0.659
MonthMay -0.558 -0.011 0.416 0.535 0.682
MonthJun -0.559 -0.016 0.398 0.487 0.560 0.690
MonthJul -0.557 -0.022 0.391 0.468 0.512 0.568 0.692
MonthAug -0.552 -0.028 0.387 0.460 0.492 0.520 0.571 0.692
MonthSep -0.545 -0.034 0.383 0.454 0.481 0.498 0.520 0.569 0.690
MonthOct -0.532 -0.039 0.376 0.445 0.470 0.482 0.493 0.513 0.561 0.683
MonthNov -0.502 -0.044 0.358 0.423 0.446 0.456 0.463 0.471 0.491 0.538
MonthDec -0.426 -0.048 0.308 0.364 0.384 0.392 0.396 0.400 0.407 0.425
MnthOc MnthNv
Time
MonthFeb
MonthMar
MonthApr
MonthMay
MonthJun
MonthJul
MonthAug
MonthSep
MonthOct
MonthNov 0.662
MonthDec 0.471 0.597
Standardized residuals:
Min Q1 Med Q3 Max
-2.5656600 -0.6285951 -0.1307054 0.5424996 3.2823396
Residual standard error: 14799.38
Degrees of freedom: 180 total; 167 residual
acf(residuals(tourism.gls, type = "normalized"))
Next steps?
What might be the next step? It looks like there is a significant
12-month correlation, which would also make sense.
But we will leave the task of adjusting for more complicated
correlation structures for another course.
---
title: "Lecture 35: Models with Autoregressive Errors"
subtitle: 161.251 Regression Modelling
author: "Presented by Jonathan Marshall <J.C.marshall@massey.ac.nz>"  
date: "Week 12 of Semester 2, `r lubridate::year(lubridate::now())`"
output:
  html_document:
    code_download: true
    theme: yeti
    highlight: tango
  html_notebook:
    code_download: true
    theme: yeti
    highlight: tango
  ioslides_presentation:
    widescreen: true
    smaller: true
  word_document: default
  slidy_presentation: 
    theme: yeti
    highlight: tango
  pdf_document: default
---




<!--- Data is on
https://r-resources.massey.ac.nz/data/161251/
--->

```{r setup, purl=FALSE, include=FALSE}
library(knitr)
opts_chunk$set(dev=c("png", "pdf"))
opts_chunk$set(fig.height=6, fig.width=7, fig.path="Figures/", fig.alt="unlabelled")
opts_chunk$set(comment="", fig.align="center", tidy=TRUE)
options(knitr.kable.NA = '')
library(tidyverse)
library(broom)
```


<!--- Do not edit anything above this line. --->


```{r extraLib, include=FALSE} 
library(nlme)        
```


##

We saw previously that when linear models are fitted to time series data, the residuals can display autocorrelation. The consequences of autocorrelation are that

- standard errors given by standard least squares theory (and
    hence by standard R output) will usually be smaller than the true
    standard deviations of the parameter estimates.
    
- the result is that *t*-test statistics will be inflated, p-values too small, and 
    confidence intervals will be too narrow.
    

## Accounting for Autocorrelation in the Errors

The consequence of standard errors and p-values being out means that we need to account for autocorrelation in the errors when it is present.

This will require two steps:
    
- Definition of an appropriate model for autocorrelated errors;
- Fitting the linear model with autocorrelated errors.

We now consider modeling the  errors using autoregressive models.

## Autoregressive Models

In a time series, the errors $\varepsilon_1, \varepsilon_2, \ldots, \varepsilon_n$
    can be thought of as a realization of a random process (in time).

We can model serial correlation between these errors by making each
    one explicitly dependent on the previous one:
    $$\varepsilon_t = \phi \varepsilon_{t-1} + \eta_t$$ where $\eta_t~(t=1,2,\ldots,n)$ is **white  noise**, that is, a sequence of independent and identically distributed  (normal) random variables with zero mean.

- This equation  is a first order autoregressive (or     **AR1**) model for $\varepsilon_t$.
- Under this model, $\mbox{Corr}(\varepsilon_t, \varepsilon_{t-1}) = \phi$.
- Consequently, more generally, $\mbox{Corr}(\varepsilon_t, \varepsilon_{t-k}) = \phi^k$

## ACF Plots for AR1 Processes

To illustrate an ACF plot for a function demonstrating autocorrelation, we create two variables from white noise 

```{r whiteNoise, fig.width=8, fig.height=3}
Z1 = rnorm(1000)
X1 = Z1[-1] + 0.85*Z1[-1000]
X2 = Z1[-1] - 0.85*Z1[-1000]
par(mfrow=c(1,2), mai=rep(0.5, 4))
plot(X1, type="l")
plot(X2, type="l")
```

##

```{r whiteNoise2, fig.width=8, fig.height=4}
par(mfrow=c(1,2))
acf(X1)
acf(X2)
```

The `X1` series has correlation of `r round(cor(X1[-1],X1[-999]),3)` at lag 1, while the `X2` series has autocorrelation of `r round(cor(X2[-1],X2[-999]),3)` at lag1 


## Autoregressive Models for Errors in Linear Modelling

If residuals in a linear model for time series data display autocorrelation then we change the model to allow for an AR1 correlation structure for the residuals in our model to account for this.

N.B. More complex models are also possible. For example:
    
- AR models of order *q>1*, where $\varepsilon_t$ is modelled as explicitly dependent on the previous *q* errors;
- moving average (MA) models and autoregressive moving average (ARMA) models.
- For the purposes of this course we will focus on AR1 models for the
    error process.

## Application to the Tourism Data

`r xfun::embed_file("../../data/motel.csv")`


```{r getTourismData, echo=-1, eval=-2, message=FALSE}
tourism <- read_csv(file="../../data/motel.csv")
tourism <- read_csv(file="motel.csv")
tourism <- tourism |>
  mutate(Time = round(time_length(Date - min(Date), unit="month")),
         Month = factor(month(Date, label=TRUE), ordered=FALSE),
         Year = year(Date))
tourism
```

##

```{r Tourism.lmResidACF,fig.height=4.5}
tourism.lm <- lm(RoomNights ~ Time + Month, data=tourism)
acf(resid(tourism.lm))
```

There is a suggestion of exponential decay in autocorrelations.
- AR1 model (with positive $\phi$) for errors seems reasonable.

##

The model incorporating the AR1 error process, and written in regression format,
is as follows: 

$$\begin{aligned}
Y_{t} &= \beta_0 + \beta_1 \mbox{Time} + \beta_2 z_{t,2} + \beta_3 z_{t,3} 
+ \ldots + \beta_{12} z_{t,12} + \varepsilon_t \\
\varepsilon_t &= \phi \varepsilon_{t-1} + \eta_{t}\end{aligned}$$ 

where:

- $Y_t$ is the $t$^th^ observation of `RoomNights`;
- $z_{t,j} = 1$ if observation $t$ is taken in month $j$;
- $z_{t,j} = 0$ otherwise.
- $\eta_1, \ldots, \eta_n$ are independent and identically
    distributed normal random variables with mean zero.

## Model Fitting with Autoregressive Errors

To fit a model with AR1 errors, we must:

- Estimate the size of the autocorrelation parameter, $\phi$.
- Account for the autocorrelation in errors when estimating the
        regression coefficients.

The AR1 parameter, $\phi$, can be estimated by the method of
    (restricted) maximum likelihood.

The details are beyond the scope of this paper, but you will meet maximum likelihood estimation if you take 161.304 or 161.331.

Once $\phi$ is estimated, we can account for the AR1 nature of the
    errors by fitting the linear model using **generalized least
    squares**.
    
## Generalized Least Squares

Once we have $\phi$ estimated, we can then estimate the regression coefficients $\beta$ by rearranging the regression equation to eliminate the autocorrelation:

Suppose
$$
\begin{aligned}
y_t &= \beta_0 + \beta_1 x_t + \varepsilon_t\\
\varepsilon_t &= \phi \varepsilon_{t-1} + \eta_t
\end{aligned}
$$
where $\eta_t \underset{\mathsf{iid}}\sim N(0, 1)$. Then
$$
\begin{aligned}
y_t - \phi y_{t-1} &= \beta_0 + \beta_1 x_t + \varepsilon_t - \phi (\beta_0 + \beta_1 x_{t-1} + \varepsilon_{t-1})\\
&= \beta_0(1 - \phi) + \beta_1 (x_t - \phi x_{t-1}) + \varepsilon_t - \phi \varepsilon_{t-1}\\
&= \beta_0(1 - \phi) + \beta_1 (x_t - \phi x_{t-1}) + \eta_t
\end{aligned}
$$
which is a standard linear regression in the new variables $Y_t = y_t - \phi y_{t-1}$, $X_t = x_t - \phi x_{t-1}$.

Thus we can fit this with least squares. The "generalised" bit is the trick we use to transform something that is not regular least squares to a least squares situation - it turns out we can do this no matter what the covariance structure is among the predictors as long as the structure is estimable from the data.

## Generalized Least Squares in R

In R, linear models can be fitted using this technique using the `gls()` command found in the `nlme` add-on package.

Call this package using `library(nlme)` before using the `gls()` command.

```{r getLib, message=FALSE}
library(nlme)
```

- The `gls()` command uses the same model formula as `lm()`, but also accepts an additional argument to describe    the correlation structure for the errors.

## Generalized Least Squares and the Tourism Data

```{r Tourism.gls}
tourism.gls <- gls(RoomNights ~ Time + Month, correlation=corAR1(), data=tourism) 
anova(tourism.gls)
```
The use of an AR1 error process is obtained by setting `correlation=corAR1()` in the `gls()` command.

Both `Time` and `Month` are associated with
    RoomNights (*P*-value less than $0.0001$ in both
    cases).

##

```{r summaryTourism.gls}
summary(tourism.gls)
```



## Comments on the Analysis

The estimated value of AR1 correlation parameter is $\hat \phi = 0.393$.

Comparison of the output from `summary(tourism.gls)` with
    the corresponding output from the earlier analysis (assuming
    independent errors) shows that the standard errors are usually
    larger here, particularly for the intercept and the coefficient of `Time`:

```{r, echo=FALSE}
library(broom.mixed)
list(gls=tourism.gls |> tidy(),
     lm=tourism.lm |> tidy()) |>
  bind_rows(, .id="model") |>
  filter(term == "Time") |>
  select(model, term, estimate, std.error)
```

The only remaining question is, was the use of `gls()` successful?

We can get the normalized residuals (i.e. 'decorrelated' residuals) with

```{r, eval=FALSE}
residuals(tourism.gls, type = "normalized")
```

##

```{r getResids}
acf(residuals(tourism.gls, type="normalized"))
```

## Next steps?

What might be the next step?  It looks like there is a significant 12-month correlation, which would also make sense.

But we will leave the task of adjusting for more complicated correlation structures for another course.

Comments on the Analysis
The estimated value of AR1 correlation parameter is \(\hat \phi = 0.393\).
Comparison of the output from
summary(tourism.gls)
with the corresponding output from the earlier analysis (assuming independent errors) shows that the standard errors are usually larger here, particularly for the intercept and the coefficient ofTime
:The only remaining question is, was the use of
gls()
successful?We can get the normalized residuals (i.e. ‘decorrelated’ residuals) with