State space time series modelling of the Dutch Labour Force Survey: Model selection and mean squared errors estimation
Section 6. Concluding remarks

There is a gradually increasing interest among NSIs in the use of STS models for the production of monthly figures on the labour force. In the Netherlands, such a model has been applied in the production of official LFS figures since 2010. STS models constitute a type of small area estimation (SAE), where sample information from preceding periods is used to obtain more precise estimates, as well as to account for the rotating panel design, often used in Labour Force Surveys.

Ignoring the hyperparameter uncertainty in the MSEs of STS model-based estimates results in underestimation of the MSEs of domain estimates. Particularly when series are short, which is often the case at NSIs, the bias due to ignoring hyperparameter uncertainty can be substantial. Most applications of SAE procedures in the literature are based on multilevel models, where it is common practice to account for hyperparameter uncertainty. The literature on STS models applied in the context of SAE is rather limited, with most applications ignoring hyperparameter uncertainty in the MSE estimates. Whether the bias in the obtained MSEs becomes substantial, depends on the structure of the model and on the length of the series. The present work describes a Monte-Carlo simulation applied to the STS model used by Statistics Netherlands for estimating monthly unemployment. The simulation serves two purposes. Firstly, it establishes the amount of bias in the DLFS MSEs when hyperparameter uncertainty is ignored. In addition to that, several MSE estimation methods available in the literature for the STS framework are compared in this simulation, and the best approach for the Dutch LFS is established. Secondly, simulating the distributions of the hyperparameter estimators is useful for obtaining better insights into the dynamics of the unobserved components in the STS model, and thus, ascertain the necessity to model the components as time-variant. In the case of the DLFS, the simulation shows that it might be worth considering a more restricted version of the model, where the rotation group bias is time-invariant and the population white noise is ignored. For both reasons, it is advisable to conduct a simulation as described in this paper as part of the model implementation process into official statistical production.

The comparison of the MSE estimation procedures also sheds new light on their properties. The asymptotic approximation is not applicable to cases where hyperparameters are close to zero because the information matrix of the hyperparameter estimates becomes (almost) singular. The non-parametric bootstraps, being less dependent on normality assumptions, perform better than their parametric counterparts under both Pfeffermann and Tiller (2005) and Rodriguez and Ruiz (2012) approaches, except in very short series. The most important finding is that the PT bootstraps have positive biases and consistently outperform the RR bootstraps, where the biases are generally negative and larger (in absolute terms) than those produced by the Kalman filter. This is contrary to the claim of Rodriguez and Ruiz (2012) about the superiority of their method in short time series. Apparently, their findings are purely heuristic and are based on a simple model (random walk plus noise), while Pfeffermann and Tiller (2005) prove that their bootstrap approach produces MSE estimates with a bias of correct order.

The variances of the PT MSE estimators are larger than the variances of the RR MSE estimators. Differences between MSEs of the PT and RR MSE estimators are modest to moderate (MSEs of the RR MSE estimators are 28 to 8 percent lower than those of the PT estimators, depending on the model and the time series length). More importantly, the tendency of the RR MSE estimators to have negative biases, sometimes exceeding those of the Kalman filter, renders these bootstrap methods inapplicable. Hence, the PT MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFfFv0dd9Wqpe0dar pepeuf0xe9q8qiYRWFGCk9vi=dbvc9s8vr0db9Ff0dbbG8Fq0Jfr=x fr=xcbpdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaeiuaiaabs facaaMc8UaeyOeI0caaa@3924@ methods should be generally considered for other survey data too, despite the fact that these methods may occasionally be outperformed by the RR MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFfFv0dd9Wqpe0dar pepeuf0xe9q8qiYRWFGCk9vi=dbvc9s8vr0db9Ff0dbbG8Fq0Jfr=x fr=xcbpdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaeOuaiaabk facaaMc8UaeyOeI0caaa@3924@ methods.

For very short time series, the non-parametric bootstraps do not seem to be an option for a model of the presented complexity. The PT parametric bootstrap, however, corrects the negatively biased MSE up to a small positive bias (1.4 to 4.4 percent, depending on the model). For the present series length of 114 months, the negative MSE bias can be reduced from about -2.4 to 1.9 percent with the non-parametric method of Pfeffermann and Tiller (2005) in the model with a time-invariant RGB. The true Kalman filter root MSEs are about 20 smaller than the standard errors of the GREG estimates in all the four models applied to the DLFS data. In general, the biases in the Kalman filter MSE estimates are relatively small in the DLFS application. Therefore, it may be deemed sufficient to rely on these naive MSE estimates for publication purposes.

Acknowledgements

We thank the National Statistical Office of the Netherlands, Statistics Netherlands, for funding this research, as well as the Associate Editor and the two anonymous reviewers for careful reading of this manuscript and valuable comments. The views expressed in this paper are those of the authors and do not necessarily reflect the policy of Statistics Netherlands.

Appendices

A. Simulated densities of the hyperparameters under the four versions of the DLFS model

This appendix presents the hyperparameter density functions obtained from simulations where the four versions of the DLFS model (see Table 5.1) act as the data generating process. The x-axes depict variance hyperparameters on a log-scale, while the y-axes stand for frequencies. The x-axis may be extended due to outliers.

Figure A.1 

Description for Figure A.1

Figure showing the hyperparameter distributions under the complete DLFS model (Model 1) for eight variance hyperparameters: σ ^ R 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamOuaaqaaiaaikdaaaGccaGGSaaaaa@384B@   σ ^ γ 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaeq4SdCgabaGaaGOmaaaakiaacYcaaaa@391B@   σ ^ λ 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaeq4UdWgabaGaaGOmaaaakiaacYcaaaa@3928@   σ ^ v t t 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaaaaaSqa aiaaikdaaaGccaGGSaaaaa@3A9A@   σ ^ v t t3 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiodaaaaaleaacaaIYaaaaOGaaiilaaaa@3C44@   σ ^ v t t6 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiAdaaaaaleaacaaIYaaaaOGaaiilaaaa@3C47@   σ ^ v t t9 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiMdaaaaaleaacaaIYaaaaaaa@3B90@  and σ ^ v t t12 2 . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaigdacaaIYaaaaaWcbaGaaGOmaaaakiaac6caaaa@3D00@  The normal density function with the same mean and variance is superimposed on each graph. The x-axes show the variance hyperparameters on a log-scale and the y-axes stand for frequencies. The x-axis may be extended due to outliers.

For σ ^ R 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamOuaaqaaiaaikdaaaGccaGGSaaaaa@384B@  the x-axis goes from -80 to -10 and the y-axis goes from 0 to 0.75. The values are highly concentrated around the mean creating a peak and are above the normal curve.

For σ ^ γ 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaeq4SdCgabaGaaGOmaaaakiaacYcaaaa@391B@  the x-axis goes from -100 to -10 and the y-axis goes from 0 to 0.075. There are extreme values at the left. The distribution is bimodal.

For σ ^ λ 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaeq4UdWgabaGaaGOmaaaakiaacYcaaaa@3928@  the x-axis goes from -100 to 0 and the y-axis goes from 0 to 0.2. There are extreme values at the left. The distribution is bimodal and very flat.

For σ ^ v t t 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaaaaaSqa aiaaikdaaaGccaGGSaaaaa@3A9A@  the x-axis goes from -0.5 to 0.75 and the y-axis goes from 0 to 3. The distribution seems close to the normal one.

For σ ^ v t t3 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiodaaaaaleaacaaIYaaaaOGaaiilaaaa@3C44@  the x-axis goes from -1.0 to 0.5 and the y-axis goes from 0 to 3. The distribution seems close to the normal one.

For σ ^ v t t6 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiAdaaaaaleaacaaIYaaaaOGaaiilaaaa@3C47@  the x-axis goes from -12.5 to 1.0 and the y-axis goes from 0 to 3. The values are highly concentrated around the mean creating a small peak.

For σ ^ v t t9 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiMdaaaaaleaacaaIYaaaaaaa@3B90@  and σ ^ v t t12 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaigdacaaIYaaaaaWcbaGaaGOmaaaakiaacYcaaaa@3CFE@  the x-axes go from -30 to 2 and the y-axes go from 0 to 3. The values are concentrated around the mean creating a peak and are above the normal curve.

Figure A.2 

Description for Figure A.2

Figure showing the hyperparameter distributions under the complete DLFS model (Model 2) for seven variance hyperparameters: σ ^ R 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamOuaaqaaiaaikdaaaGccaGGSaaaaa@384B@   σ ^ λ 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaeq4UdWgabaGaaGOmaaaakiaacYcaaaa@3928@   σ ^ v t t 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaaaaaSqa aiaaikdaaaGccaGGSaaaaa@3A9A@   σ ^ v t t3 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiodaaaaaleaacaaIYaaaaOGaaiilaaaa@3C44@   σ ^ v t t6 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiAdaaaaaleaacaaIYaaaaOGaaiilaaaa@3C47@   σ ^ v t t9 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiMdaaaaaleaacaaIYaaaaaaa@3B90@  and σ ^ v t t12 2 . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaigdacaaIYaaaaaWcbaGaaGOmaaaakiaac6caaaa@3D00@  The normal density function with the same mean and variance is superimposed on each graph. The x-axes show the variance hyperparameters on a log-scale and the y-axes stand for frequencies. The x-axis may be extended due to outliers.

For σ ^ R 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamOuaaqaaiaaikdaaaGccaGGSaaaaa@384B@  the x-axis goes from -80 to -10 and the y-axis goes from 0 to 0.75. The values are highly concentrated around the mean creating a peak and are above the normal curve.

For σ ^ λ 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaeq4UdWgabaGaaGOmaaaakiaacYcaaaa@3928@  the x-axis goes from -100 to 0 and the y-axis goes from 0 to 0.3. The distribution is bimodal and the normal curve is very flat.

For σ ^ v t t 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaaaaaSqa aiaaikdaaaGccaGGSaaaaa@3A9A@  the x-axis goes from -50 to 2 and the y-axis goes from 0 to 3. The values are highly concentrated around the mean creating a high peak and are above the normal curve.

For σ ^ v t t3 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiodaaaaaleaacaaIYaaaaOGaaiilaaaa@3C44@  the x-axis goes from -20 to 1 and the y-axis goes from 0 to 3. The values are concentrated around the mean creating a peak.

For σ ^ v t t6 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiAdaaaaaleaacaaIYaaaaOGaaiilaaaa@3C47@  the x-axis goes from -80 to 0 and the y-axis goes from 0 to 2. The values are highly concentrated around the mean creating a high peak and are above the normal curve.

For σ ^ v t t9 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiMdaaaaaleaacaaIYaaaaaaa@3B90@  and σ ^ v t t12 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaigdacaaIYaaaaaWcbaGaaGOmaaaakiaacYcaaaa@3CFE@  the x-axes go from -100 to 0 and the y-axes go from 0 to 2. The values are concentrated around the mean creating a high peak and are above the normal curve.

Figure A.3 

Description for Figure A.3

Figure showing the hyperparameter distributions under the complete DLFS model (Model 3) for seven variance hyperparameters: σ ^ R 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamOuaaqaaiaaikdaaaGccaGGSaaaaa@384B@   σ ^ γ 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaeq4SdCgabaGaaGOmaaaakiaacYcaaaa@391B@   σ ^ v t t 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaaaaaSqa aiaaikdaaaGccaGGSaaaaa@3A9A@   σ ^ v t t3 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiodaaaaaleaacaaIYaaaaOGaaiilaaaa@3C44@   σ ^ v t t6 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiAdaaaaaleaacaaIYaaaaOGaaiilaaaa@3C47@   σ ^ v t t9 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiMdaaaaaleaacaaIYaaaaaaa@3B90@  and σ ^ v t t12 2 . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaigdacaaIYaaaaaWcbaGaaGOmaaaakiaac6caaaa@3D00@  The normal density function with the same mean and variance is superimposed on each graph. The x-axes show the variance hyperparameters on a log-scale and the y-axes stand for frequencies.

For σ ^ R 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamOuaaqaaiaaikdaaaGccaGGSaaaaa@384B@  the x-axis goes from -18 to -10 and the y-axis goes from 0 to 0.75. The values are concentrated around the mean and asymmetric but close the normal curve.

For σ ^ γ 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaeq4SdCgabaGaaGOmaaaakiaacYcaaaa@391B@  the x-axis goes from -37.5 to -25 and the y-axis goes from 0 to 0.3. The values are concentrated around the mean and asymmetric but close the normal curve.

For σ ^ v t t 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaaaaaSqa aiaaikdaaaGccaGGSaaaaa@3A9A@   σ ^ v t t3 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiodaaaaaleaacaaIYaaaaOGaaiilaaaa@3C44@   σ ^ v t t6 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiAdaaaaaleaacaaIYaaaaaaa@3B8D@  and σ ^ v t t12 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaigdacaaIYaaaaaWcbaGaaGOmaaaakiaacYcaaaa@3CFE@  the x-axes go from -0.50 to 0.50 and the y-axes go from 0 to 3. The values are very close to the normal curve.

For σ ^ v t t9 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiMdaaaaaleaacaaIYaaaaOGaaiilaaaa@3C4A@  the x-axes go from -0.25 to 0.75 and the y-axes go from 0 to 3. The values are very close to the normal curve.

Figure A.4 

Description for Figure A.4

Figure showing the hyperparameter distributions under the complete DLFS model (Model 4) for six variance hyperparameters: σ ^ R 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamOuaaqaaiaaikdaaaGccaGGSaaaaa@384B@   σ ^ v t t 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaaaaaSqa aiaaikdaaaGccaGGSaaaaa@3A9A@   σ ^ v t t3 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiodaaaaaleaacaaIYaaaaOGaaiilaaaa@3C44@   σ ^ v t t6 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiAdaaaaaleaacaaIYaaaaOGaaiilaaaa@3C47@   σ ^ v t t9 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiMdaaaaaleaacaaIYaaaaaaa@3B90@  and σ ^ v t t12 2 . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaigdacaaIYaaaaaWcbaGaaGOmaaaakiaac6caaaa@3D00@  The normal density function with the same mean and variance is superimposed on each graph. The x-axes show the variance hyperparameters on a log-scale and the y-axes stand for frequencies.

For σ ^ R 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamOuaaqaaiaaikdaaaGccaGGSaaaaa@384B@  the x-axis goes from -17 to -11 and the y-axis goes from 0 to 0.75. The values are concentrated around the mean and asymmetric but close the normal curve.

For σ ^ v t t 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaaaaaSqa aiaaikdaaaaaaa@39E0@  and σ ^ v t t9 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiMdaaaaaleaacaaIYaaaaOGaaiilaaaa@3C4A@  the x-axes go from -0.25 to 0.75 and the y-axes go from 0 to 3. The values are very close to the normal curve.

For σ ^ v t t3 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiodaaaaaleaacaaIYaaaaOGaaiilaaaa@3C44@   σ ^ v t t6 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaiAdaaaaaleaacaaIYaaaaaaa@3B8D@  and σ ^ v t t12 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrFgFv0dd9Wqpe0dd9 qqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9Ff0dfrpe0dXdHqps0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafq4WdmNbaK aadaqhaaWcbaGaamODamaaDaaameaacaWG0baabaGaamiDaiabgkHi TiaaigdacaaIYaaaaaWcbaGaaGOmaaaakiaacYcaaaa@3CFE@  the x-axes go from -0.50 to 0.50 and the y-axes go from 0 to 3. The values are very close to the normal curve.

B. Predictive performance of the four DLFS models

Table B.1
Root mean square deviations of GREG estimates of the numbers of unemployed from their one-step-ahead predictions, per wave
Table summary
This table displays the results of Root mean square deviations of GREG estimates of the numbers of unemployed from their one-step-ahead predictions. The information is grouped by W (appearing as row headers), Model 1, Model 2, Model 3 and Model 4 (appearing as column headers).
W Model 1 Model 2 Model 3 Model 4
d = 20 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7HqGqFjpu0de9LqFHe9Lq pepeea0xd9q8qiYRWxGi6xij=hbba9q8aq0=yq=He9q8qiLsFr0=vr 0=vr0db8meqabeqadiWaceGabeqabeWabeqaeeaakeaacaWGKbGaaG ypaiaaikdacaaIWaaaaa@3BD2@ d = 30 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7HqGqFjpu0de9LqFHe9Lq pepeea0xd9q8qiYRWxGi6xij=hbba9q8aq0=yq=He9q8qiLsFr0=vr 0=vr0db8meqabeqadiWaceGabeqabeWabeqaeeaakeaacaWGKbGaaG ypaiaaikdacaaIWaaaaa@3BD2@ d = 60 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7HqGqFjpu0de9LqFHe9Lq pepeea0xd9q8qiYRWxGi6xij=hbba9q8aq0=yq=He9q8qiLsFr0=vr 0=vr0db8meqabeqadiWaceGabeqabeWabeqaeeaakeaacaWGKbGaaG ypaiaaikdacaaIWaaaaa@3BD2@ d = 20 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7HqGqFjpu0de9LqFHe9Lq pepeea0xd9q8qiYRWxGi6xij=hbba9q8aq0=yq=He9q8qiLsFr0=vr 0=vr0db8meqabeqadiWaceGabeqabeWabeqaeeaakeaacaWGKbGaaG ypaiaaikdacaaIWaaaaa@3BD2@ d = 30 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7HqGqFjpu0de9LqFHe9Lq pepeea0xd9q8qiYRWxGi6xij=hbba9q8aq0=yq=He9q8qiLsFr0=vr 0=vr0db8meqabeqadiWaceGabeqabeWabeqaeeaakeaacaWGKbGaaG ypaiaaikdacaaIWaaaaa@3BD2@ d = 60 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7HqGqFjpu0de9LqFHe9Lq pepeea0xd9q8qiYRWxGi6xij=hbba9q8aq0=yq=He9q8qiLsFr0=vr 0=vr0db8meqabeqadiWaceGabeqabeWabeqaeeaakeaacaWGKbGaaG ypaiaaikdacaaIWaaaaa@3BD2@ d = 20 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7HqGqFjpu0de9LqFHe9Lq pepeea0xd9q8qiYRWxGi6xij=hbba9q8aq0=yq=He9q8qiLsFr0=vr 0=vr0db8meqabeqadiWaceGabeqabeWabeqaeeaakeaacaWGKbGaaG ypaiaaikdacaaIWaaaaa@3BD2@ d = 30 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7HqGqFjpu0de9LqFHe9Lq pepeea0xd9q8qiYRWxGi6xij=hbba9q8aq0=yq=He9q8qiLsFr0=vr 0=vr0db8meqabeqadiWaceGabeqabeWabeqaeeaakeaacaWGKbGaaG ypaiaaikdacaaIWaaaaa@3BD2@ d = 60 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7HqGqFjpu0de9LqFHe9Lq pepeea0xd9q8qiYRWxGi6xij=hbba9q8aq0=yq=He9q8qiLsFr0=vr 0=vr0db8meqabeqadiWaceGabeqabeWabeqaeeaakeaacaWGKbGaaG ypaiaaikdacaaIWaaaaa@3BD2@ d = 20 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7HqGqFjpu0de9LqFHe9Lq pepeea0xd9q8qiYRWxGi6xij=hbba9q8aq0=yq=He9q8qiLsFr0=vr 0=vr0db8meqabeqadiWaceGabeqabeWabeqaeeaakeaacaWGKbGaaG ypaiaaikdacaaIWaaaaa@3BD2@ d = 30 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7HqGqFjpu0de9LqFHe9Lq pepeea0xd9q8qiYRWxGi6xij=hbba9q8aq0=yq=He9q8qiLsFr0=vr 0=vr0db8meqabeqadiWaceGabeqabeWabeqaeeaakeaacaWGKbGaaG ypaiaaikdacaaIWaaaaa@3BD2@ d = 60 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqk0Jf9crFfpeea0xh9v8qiW7HqGqFjpu0de9LqFHe9Lq pepeea0xd9q8qiYRWxGi6xij=hbba9q8aq0=yq=He9q8qiLsFr0=vr 0=vr0db8meqabeqadiWaceGabeqabeWabeqaeeaakeaacaWGKbGaaG ypaiaaikdacaaIWaaaaa@3BD2@
1 34,370 33,582 34,641 34,370 33,582 34,641 34,518 33,754 34,881 34,525 33,757 34,885
2 30,130 29,770 29,410 30,130 29,770 29,410 30,138 29,780 29,418 30,144 29,779 29,409
3 35,792 32,631 34,654 35,792 32,631 34,654 35,714 32,535 34,499 35,716 32,532 34,499
4 39,647 38,556 36,797 39,647 38,556 36,797 39,753 38,640 36,891 39,743 38,633 36,889
5 38,271 37,622 36,341 38,271 37,622 36,341 38,183 37,528 36,225 38,177 37,523 36,226

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