NAG Library Routine Document
g02fcf (linregm_stat_durbwat)
1
Purpose
g02fcf calculates the Durbin–Watson statistic, for a set of residuals, and the upper and lower bounds for its significance.
2
Specification
Fortran Interface
Integer, Intent (In)  ::  n, ip  Integer, Intent (Inout)  ::  ifail  Real (Kind=nag_wp), Intent (In)  ::  res(n)  Real (Kind=nag_wp), Intent (Out)  ::  d, pdl, pdu, work(n) 

C Header Interface
#include nagmk26.h
void 
g02fcf_ (const Integer *n, const Integer *ip, const double res[], double *d, double *pdl, double *pdu, double work[], Integer *ifail) 

3
Description
For the general linear regression model
where 
$y$ is a vector of length $n$ of the dependent variable,
$X$ is a $n$ by $p$ matrix of the independent variables,
$\beta $ is a vector of length $p$ of unknown arguments, 
and 
$\epsilon $ is a vector of length $n$ of unknown random errors. 
The residuals are given by
and the fitted values,
$\hat{y}=X\hat{\beta}$, can be written as
$Hy$ for a
$n$ by
$n$ matrix
$H$. Note that when a mean term is included in the model the sum of the residuals is zero. If the observations have been taken serially, that is
${y}_{1},{y}_{2},\dots ,{y}_{n}$ can be considered as a time series, the Durbin–Watson test can be used to test for serial correlation in the
${\epsilon}_{i}$, see
Durbin and Watson (1950),
Durbin and Watson (1951) and
Durbin and Watson (1971).
The Durbin–Watson statistic is
Positive serial correlation in the
${\epsilon}_{i}$ will lead to a small value of
$d$ while for independent errors
$d$ will be close to
$2$. Durbin and Watson show that the exact distribution of
$d$ depends on the eigenvalues of the matrix
$HA$ where the matrix
$A$ is such that
$d$ can be written as
and the eigenvalues of the matrix
$A$ are
${\lambda}_{j}=\left(1\mathrm{cos}\left(\pi j/n\right)\right)$, for
$j=1,2,\dots ,n1$.
However bounds on the distribution can be obtained, the lower bound being
and the upper bound being
where the
${u}_{i}$ are independent standard Normal variables. The lower tail probabilities associated with these bounds,
${p}_{\mathrm{l}}$ and
${p}_{\mathrm{u}}$, are computed by
g01epf. The interpretation of the bounds is that, for a test of size (significance)
$\alpha $, if
${p}_{l}\le \alpha $ the test is significant, if
${p}_{u}>\alpha $ the test is not significant, while if
${p}_{\mathrm{l}}>\alpha $ and
${p}_{\mathrm{u}}\le \alpha $ no conclusion can be reached.
The above probabilities are for the usual test of positive autocorrelation. If the alternative of negative autocorrelation is required, then a call to
g01epf should be made with the argument
d taking the value of
$4d$; see
Newbold (1988).
4
References
Durbin J and Watson G S (1950) Testing for serial correlation in least squares regression. I Biometrika 37 409–428
Durbin J and Watson G S (1951) Testing for serial correlation in least squares regression. II Biometrika 38 159–178
Durbin J and Watson G S (1971) Testing for serial correlation in least squares regression. III Biometrika 58 1–19
Granger C W J and Newbold P (1986) Forecasting Economic Time Series (2nd Edition) Academic Press
Newbold P (1988) Statistics for Business and Economics Prentice–Hall
5
Arguments
 1: $\mathbf{n}$ – IntegerInput

On entry: $n$, the number of residuals.
Constraint:
${\mathbf{n}}>{\mathbf{ip}}$.
 2: $\mathbf{ip}$ – IntegerInput

On entry: $p$, the number of independent variables in the regression model, including the mean.
Constraint:
${\mathbf{ip}}\ge 1$.
 3: $\mathbf{res}\left({\mathbf{n}}\right)$ – Real (Kind=nag_wp) arrayInput

On entry: the residuals, ${r}_{1},{r}_{2},\dots ,{r}_{n}$.
Constraint:
the mean of the residuals $\text{}\le \sqrt{\epsilon}$, where $\epsilon =\mathit{machineprecision}$.
 4: $\mathbf{d}$ – Real (Kind=nag_wp)Output

On exit: the Durbin–Watson statistic, $d$.
 5: $\mathbf{pdl}$ – Real (Kind=nag_wp)Output

On exit: lower bound for the significance of the Durbin–Watson statistic, ${p}_{\mathrm{l}}$.
 6: $\mathbf{pdu}$ – Real (Kind=nag_wp)Output

On exit: upper bound for the significance of the Durbin–Watson statistic, ${p}_{\mathrm{u}}$.
 7: $\mathbf{work}\left({\mathbf{n}}\right)$ – Real (Kind=nag_wp) arrayWorkspace

 8: $\mathbf{ifail}$ – IntegerInput/Output

On entry:
ifail must be set to
$0$,
$1\text{ or}1$. If you are unfamiliar with this argument you should refer to
Section 3.4 in How to Use the NAG Library and its Documentation for details.
For environments where it might be inappropriate to halt program execution when an error is detected, the value
$1\text{ or}1$ is recommended. If the output of error messages is undesirable, then the value
$1$ is recommended. Otherwise, if you are not familiar with this argument, the recommended value is
$0$.
When the value $\mathbf{1}\text{ or}\mathbf{1}$ is used it is essential to test the value of ifail on exit.
On exit:
${\mathbf{ifail}}={\mathbf{0}}$ unless the routine detects an error or a warning has been flagged (see
Section 6).
6
Error Indicators and Warnings
If on entry
${\mathbf{ifail}}=0$ or
$1$, explanatory error messages are output on the current error message unit (as defined by
x04aaf).
Errors or warnings detected by the routine:
 ${\mathbf{ifail}}=1$

On entry, ${\mathbf{ip}}=\u2329\mathit{\text{value}}\u232a$.
Constraint: ${\mathbf{ip}}\ge 1$.
On entry, ${\mathbf{n}}=\u2329\mathit{\text{value}}\u232a$ and ${\mathbf{ip}}=\u2329\mathit{\text{value}}\u232a$.
Constraint: ${\mathbf{n}}>{\mathbf{ip}}$.
 ${\mathbf{ifail}}=2$

On entry, mean of ${\mathbf{res}}=\u2329\mathit{\text{value}}\u232a$.
Constraint: the mean of the residuals $\text{}\le \sqrt{\epsilon}$, where $\epsilon =\mathit{machineprecision}$
 ${\mathbf{ifail}}=3$

On entry, all residuals are identical.
 ${\mathbf{ifail}}=99$
An unexpected error has been triggered by this routine. Please
contact
NAG.
See
Section 3.9 in How to Use the NAG Library and its Documentation for further information.
 ${\mathbf{ifail}}=399$
Your licence key may have expired or may not have been installed correctly.
See
Section 3.8 in How to Use the NAG Library and its Documentation for further information.
 ${\mathbf{ifail}}=999$
Dynamic memory allocation failed.
See
Section 3.7 in How to Use the NAG Library and its Documentation for further information.
7
Accuracy
The probabilities are computed to an accuracy of at least $4$ decimal places.
8
Parallelism and Performance
g02fcf makes calls to BLAS and/or LAPACK routines, which may be threaded within the vendor library used by this implementation. Consult the documentation for the vendor library for further information.
Please consult the
X06 Chapter Introduction for information on how to control and interrogate the OpenMP environment used within this routine. Please also consult the
Users' Note for your implementation for any additional implementationspecific information.
If the exact probabilities are required, then the first
$np$ eigenvalues of
$HA$ can be computed and
g01jdf used to compute the required probabilities with the argument
c set to
$0.0$ and the argument
d set to the Durbin–Watson statistic
$d$.
10
Example
A set of $10$ residuals are read in and the Durbin–Watson statistic along with the probability bounds are computed and printed.
10.1
Program Text
Program Text (g02fcfe.f90)
10.2
Program Data
Program Data (g02fcfe.d)
10.3
Program Results
Program Results (g02fcfe.r)