For the beta distribution with parameters , the Euler beta function gives . Its probability density function is therefore on . Direct integration gives the raw momentsIn particular, its mean is . Equating this to the sample mean and rearranging givesThe observations lie strictly between zero and one with probability one, so and this method of moments estimator is well defined and positive. This is an instance of estimation of a beta shape parameter.
Using the raw moments from part (i), the variance of one observation isThe central limit theorem for the independent statistical sample givesFor , its derivative at the mean is . The delta method therefore givesEquivalently, the large-sample normal approximation isHere denotes the leading asymptotic variance, rather than an assertion about an exact finite-sample variance.
Write , with the natural logarithm. The likelihood function and log-likelihood function areThe score function is and the second derivative is . Thus the log-likelihood function is strictly concave, its stationary point is the unique global maximum, and the maximum-likelihood estimator isThe one-observation Fisher information is . The support of a probability distribution here is independent of , so the regular asymptotic normality of a maximum likelihood estimator givesThere is also a direct check: has an exponential distribution with rate , since for . Its mean and variance are and . Apply the central limit theorem to and the delta method to to obtain the same result.
The specified asymptotic relative efficiency isFor every fixed this lies strictly between zero and one. Prefer on grounds of asymptotic precision: it has the smaller leading asymptotic variance and attains the inverse Fisher information. Both are consistent estimators, by the law of large numbers and the continuous mapping theorem applied respectively to and . The efficiency approaches zero as and one as .
This preference is an asymptotic comparison. In particular, it does not assert that is an unbiased estimator: since has a gamma distribution of shape and rate , for .
The standard error suggested by part (iii) is . Substituting the consistent estimator gives ; Slutsky's theorem givesUsing the central standard normal quantiles , an approximate 95% Wald confidence interval isIts coverage probability approaches 0.95 for each fixed as . The intersection enforces positivity and does not change whether the true positive statistical parameter is covered. The value 1.64 would give the wrong central two-sided coverage probability.
Put , , and . The two independent statistical samples give the joint likelihood functionThe unrestricted maximum-likelihood estimators are and . Under the null hypothesis, the common statistical parameter has log-likelihood function , maximized at . With the likelihood ratio defined as the null maximum divided by the unrestricted maximum,The statistic in the paper is , since both original sums of natural logarithms are negative. HenceIt has maximum one at , corresponding to equal fitted rates. This is the likelihood-ratio test for equality of beta shape parameters.
A likelihood-ratio test rejects for small . The derivative of the natural logarithm of its variable factor isThus increases up to and decreases thereafter, tending to zero at both endpoints. Every nontrivial lower level set of therefore consists of two tails. For a prescribed test size , the exact critical region isWriting for the cumulative distribution function of the beta distribution with parameters , the required two equations areThe first makes both cutoffs have the same likelihood ratio; the second calibrates the null hypothesis rejection probability. Equivalently, the second left-hand side isAs the common likelihood ratio threshold increases from zero to one, this probability increases continuously and strictly from zero to one; hence the equations determine unique cutoffs. The two tail probabilities need not each equal when . Exact calibration holds for every common rate because the given null distribution of is independent of that rate. Boundary equalities have zero probability.
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