The previous note stated Wilks' theorem and previewed, in one paragraph, why a Taylor expansion of the log-likelihood is the engine behind it. This note carries that argument out in full, in two stages. First, the scalar case — testing a single fully-specified against an unrestricted one-dimensional — reduces to a short, self-contained calculation: expand around the unrestricted MLE , use the fact that the score vanishes at to kill the first-order term, and recognise the surviving quadratic term as (a constant times) the square of the already-known asymptotically Normal quantity . Second, the general multiparameter case extends this by the same spectral-decomposition machinery Cochran's theorem already supplied for splitting a sum of squares into independent chi-squared pieces — here applied not to and , but to the restricted and unrestricted maximum-likelihood fits.
Learning objectives. By the end of this note you should be able to:
- Taylor-expand the log-likelihood around the unrestricted MLE and identify why the first-order term vanishes;
- derive the scalar-case result in full, identifying every asymptotic ingredient used;
- state the multiparameter generalisation as a quadratic form in an asymptotically Normal vector, standardised by the Fisher information matrix;
- apply Cochran's theorem to decompose that quadratic form into independent and pieces, recovering Wilks' degrees-of-freedom rule from first principles;
- identify precisely which regularity conditions the argument leans on, and where each one is used.
In this lesson
- Setup and notation
- The scalar case
- The general multiparameter case
Before you start
- Wilks' Theorem: the Asymptotic χ² Distribution
- Asymptotic Properties of the MLE
- Derivation — The Sampling Distribution of S² and Cochran's Theorem
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