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6.3 Unit Roots in Time Series Models 197<br />

We confine our discussion of unit root tests to first-order moving-average models,<br />

the general case being considerably more complicated and not fully resolved. Let<br />

X1,...,Xn be observations from the MA(1) model<br />

Xt Zt + θZt−1, {Zt} ∼IID 0,σ 2 .<br />

Davis and Dunsmuir (1996) showed that under the assumption θ −1,n(ˆθ +1) (ˆθ is<br />

the maximum likelihood estimator) converges in distribution. A test of H0 : θ −1<br />

vs. H1 : θ>−1 can be fashioned on this limiting result by rejecting H0 when<br />

ˆθ >−1 + cα/n,<br />

where cα is the (1 − α) quantile of the limit distribution of n ˆθ + 1 . (From Table<br />

3.2 of Davis, Chen, and Dunsmuir (1995), c.01 11.93, c.05 6.80, and c.10 <br />

4.90.) In particular, if n 50, then the null hypothesis is rejected at level .05 if<br />

ˆθ >−1 + 6.80/50 −.864.<br />

The likelihood ratio test can also be used for testing the unit root hypothesis. The<br />

likelihood ratio for this problem is L(−1,S(−1)/n)/L ˆθ, ˆσ 2<br />

<br />

, where L θ,σ2 is<br />

the Gaussian likelihood of the data based on an MA(1) model, S(−1) is the sum of<br />

squares given by (5.2.11) when θ −1, and ˆθ and ˆσ 2 are the maximum likelihood<br />

estimators of θ and σ 2 . The null hypothesis is rejected at level α if<br />

⎛<br />

λn : −2ln⎝<br />

L(−1,S(−1)/n)<br />

<br />

L ˆθ, ˆσ 2<br />

⎞<br />

⎠ >cLR,α<br />

where the cutoff value is chosen such that Pθ−1[λn >cLR,α] α. The limit distribution<br />

of λn was derived by Davis et al. (1995), who also gave selected quantiles<br />

of the limit. It was found that these quantiles provide a good approximation to their<br />

finite-sample counterparts for time series of length n ≥ 50. The limiting quantiles<br />

for λn under H0 are cLR,.01 4.41, cLR,.05 1.94, and cLR,.10 1.00.<br />

Example 6.3.2 For the overshort data {Xt} of Example 3.2.8, the maximum likelihood MA(1) model<br />

for the mean corrected data {Yt Xt + 4.035} was (see Example 5.4.1)<br />

Yt Zt − 0.818Zt−1, {Zt} ∼WN(0, 2040.75).<br />

In the structural formulation of this model given in Example 3.2.8, the moving-average<br />

parameter θ was related to the measurement error variances σ 2 U and σ 2 V through the<br />

equation<br />

θ<br />

1 + θ 2 −σ 2 U<br />

2σ 2 U + σ 2 .<br />

V<br />

(These error variances correspond to the daily measured amounts of fuel in the tank<br />

and the daily measured adjustments due to sales and deliveries.) A value of θ −1

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