Let $L(\vartheta ;x)$ be the likelihood function, with full parameter space $\Theta$ and null hypothesis $\vartheta \in {\Theta }_0\subseteq \Theta$. The generalized likelihood-ratio test compares the best null fit to the best unrestricted fit:The likelihood ratio $R$ lies between zero and one, and small values count against the null hypothesis; equivalently, large values of the likelihood-ratio test statistic $\Lambda$ count against it.

Compute restricted and unrestricted maximum-likelihood estimates, evaluate their log-likelihoods, and form $\Lambda =2(\ell (\hat{\vartheta })-\ell ({\hat{\vartheta }}_0))$. Under the regular conditions of Wilks theorem, the null limit isThese statistical degrees of freedom count independent parameter restrictions. The regularity includes a locally identifiable smooth model, nonsingular Fisher information, and an interior null value; parameter-dependent support can invalidate the result.

For a chosen significance level $\alpha$, obtain the $(1-\alpha )$ quantile $q_{d,1-\alpha }$ of the chi-squared distribution and useEquivalently, compare the asymptotic p-value $\mathrm{Pr}({\chi }_d^2\ge {\Lambda }_{\mathrm{obs}})$ to $\alpha$. This is a large-sample calibration; part (c) requires direct treatment because its support depends on a parameter.

For the normal distribution, the density at its centre is $f(\theta )=1/(\sigma \sqrt{2\pi })$. The sample mean has exact variance ${\sigma }^2/n$, whereas part (b) gives the sample median the leading variance $\pi {\sigma }^2/(2n)$. Thus the requested asymptotic relative efficiency isAt a fixed confidence level, a confidence interval based on the sample mean has a leading half-width smaller by the factor $\sqrt{2/\pi }$. With known $\sigma$, $\overline{X}\pm z_{1-\alpha /2}\sigma /\sqrt{n}$ also has exact normal coverage. Prefer the sample mean under the normal model.

For the Laplace distribution, symmetry puts both the mean and median at $\theta$. Its density there is $1/(2\sigma )$, andConsequently the sample mean has variance $2{\sigma }^2/n$, while the sample median has leading variance ${\sigma }^2/n$. HenceA large-sample confidence interval based on the sample median has leading half-width smaller by $1/\sqrt{2}$; with known scale it is $M_X\pm z_{1-\alpha /2}\sigma /\sqrt{n}$. Prefer the sample median under the Laplace model. Consistent estimation of an unknown scale preserves these leading comparisons. The reason for the reversal is quantitative: the median's precision depends on the central density $f(\theta )$, while the sample mean's precision depends on the whole population variance.

Use $A=a+{\sum }_i{x}_i$ and $B=b+n$ as above. The future observation is independent of the old observations conditional on $\theta$, so the posterior predictive probability is obtained by integrating its Poisson distribution against the posterior distribution of $\theta$:The last integral is the normalizing gamma function integral, equal to $\Gamma (A+k)/(B+1{)}^{A+k}$. This is a negative binomial distribution in the count-of-failures convention with shape $A$ and success probability $B/(B+1)$; the gamma-function expression remains valid for noninteger $A>0$. As checks, its mean is $A/B$, and the law of total variance gives variance $A/B+A/B^2$. The additional term is the contribution of posterior uncertainty in $\theta$.