David F. Hendry 49
In (1.40),
(
R∗
) 2
is the squared multiple correlation when a constant is added,
FM(13, 45)is the associated test of the null, and̂σis the residual standard devia-
tion, with coefficient standard errors shown in parentheses. The diagnostic tests
are of the formFj(k,T−l), which denotes an approximateF-test against the
alternative hypothesisjfor:kth-order serial correlation (Far: see Godfrey, 1978),
kth-order autoregressive conditional heteroskedasticity (Farch: see Engle, 1982),
heteroskedasticity (Fhet: see White, 1980a); theRESETtest (Freset: see Ramsey, 1969);
parameter constancy (FChow(see Chow, 1960) overkperiods; and a chi-square test
for normality (χnd^2 ( 2 )(see Doornik and Hansen, 2008). No misspecification test
rejects.
The result in (1.40) is to be contrasted with the equation reported earlier, which
had a similar equilibrium correction term based on Johansen (1988):
c 2 =ef+7.88−0.4e+0.4
(
pf−p
)
, (1.41)
leading to (D3133 and D4446 are dummies with the value unity over the periods
1931–33 and 1944–46 respectively):
ef,t= 0.27
(0.04)
st− 1 − 0.34
(0.02)
c2,t− 1 − 0.019
(0.004)
+ 0.24
(0.05)
st
+ 0.53
(0.05)
et− 0.46
(0.04)
(pf−p)t− 0.12
(0.01)
D3133+ 0.038
(0.010)
D4446
R^2 =0.936FM(7, 51)=107.2∗∗̂σ=0.0098Far(2, 49)=0.18
χ^2 ( 2 )=0.21Farch(1, 49)=0.59Freset(1, 50)=0.26Fhet(13, 37)=0.47. (1.42)
Thus, six additional outliers have been detected in (1.40), whereas none of the
components of D4446 was found, nor was I 33 : neither dummy is remotely sig-
nificant if added to (1.40). Consistent with that result, when (1.42) and (1.40)
are denoted models 1 and 2 on encompassing tests,FEnc1,2(10, 41) = 4.83∗∗
andFEnc2,1(5, 41)=2.18, so (1.42) is encompassed by (1.40) but not vice versa.
Nevertheless, both models are rejected against the other on Cox (1961) and Ericsson
(1983) non-nested tests witĥσJ=0.0074.
Another recent development that can be implemented based on impulse satura-
tion is to test for the super exogeneity of the parameters of the conditional model in
response to changes in the LDGPs of the two main conditioning variables,etand
(pf−p)t(see section 1.4.5 and Hendry and Santos, 2009). The latter’s equation
revealed no significant breaks, but commencing from one lag ofe,(pf−p),s
anda, the former produced:
et= 0.016
(0.003)
+ 0.256
(0.081)
et− 1 − 0.302
(0.083)
(pf−p)t− 1 − 0.11
(0.02)
I 31
− 0.19
(0.02)
I 32 + 0.10
(0.02)
I 34