Appendix J

Random Intercept Model

(Sources: Cameron and Trivedi [1], Hsiao [2])

The random effects model can be written as

(J.1) equation

or

(J.2) equation

where img. The variance–covariance matrix of img is

(J.3) equation

Its inverse is

(J.4) equation

The individual-specific effects img are assumed to be realizations of i.i.d. random variables with distribution img and the error img is i.i.d. img. The model can be re-expressed as img, where the error term img has two components img. For this reason the random effects model is also called the error components model or random intercept model. The random intercept model can be estimated by the maximum likelihood method.

When img and img are random and normally distributed, the logarithm of the likelihood function is

(J.5) equation

where

(J.6) equation

The maximum likelihood estimator (MLE) of img is obtained by solving the following first-order conditions simultaneously:

(J.7) equation

(J.8) equation

(J.9) equation

(J.10) equation

Simultaneous solution of Equations J.7J.10 is complicated. The Newton–Raphson iterative procedure can be used to solve for the MLE. The procedure uses an initial trial value img of img to start the iteration by substituting it into the formula

(J.11) equation

to obtain a revised estimate of img. The process is repeated until the jth iterative solution img is close to the imgth iterative solution img.

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